PRODUCTS AND CAPABILITIES 2017
Gooch & Housego generates, controls, amplifies, connects, and measures lasers and light sources. Our expertise enables customers to push the boundaries of commercial applications of photonics technology.
CONTENTS ABOUT US Global Leaders in Photonics Technology
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Sectors and Applications
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Continuous Improvement
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Quality Management
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CAPABILITIES AND PRODUCTS Acousto-Optics13 Crystal Optics
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Electro-Optics35 Fiber Optics
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Precision Optics
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Light Measurement Instrumentation
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CONTACT US Gooch & Housego Locations
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Sales Contacts
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Distributors86 INDEX Products, Capabilities and Services
GOOCH & HOUSEGO
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ABOUT US
GLOBAL LEADERS IN PHOTONICS TECHNOLOGY Gooch & Housego generates, controls, amplifies, connects, and measures lasers and light sources. Our expertise enables customers to push the boundaries of commercial applications of photonics technology. Custom and Commercial Off-the-Shelf Our products are at the heart of systems, whether custom or commercial off-the-shelf (COTS). We also provide complete optical system design, engineering, and volume manufacturing services. Many of our customers start with a COTS product for proofof-concept or prototyping stages of development and migrate into a semi-custom or completely customized solution as they move into production.
Design, Prototyping through to Volume Manufacturing From the research and development of our own products, to helping our customers design, prototype, and scale-up, our engineers and technologists support customers at every step.
• Acousto-optics (AO) • Crystal optics (CO) • Electro-optics (EO) • Electro-optic systems (EOS) • Fiber optics (FO) • Light measurement instrumentation (LMI) • Precision optics (PO)
Applied Research and Development
Quality and Compliance With five facilities in the USA and four in the UK, we can often serve both ITAR or non-ITAR requests. All of our facilities are ISO9001 certified, with ISO18001 and ISO14001 certifications in process.
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Gooch & Housego demonstrates unparalleled capabilities in the following photonic technologies:
In 2013 we established the Systems Technology Group (STG) with the specific purpose of designing, developing, and prototyping systems-level products. Our multi-disciplinary team, with expertise in mechanical, electronic, and software design and modeling, integrates these technologies with G&H’s expertise in photonics.
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1995
1999
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2007
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ACOUSTO AND PRECISION OPTICS
LIGHT MEASUREMENT INSTRUMENTATION
CRYSTAL AND ELECTRO-OPTICS
ACOUSTO-OPTICS
FIBER OPTICS
PRECISION OPTICS
Founded in Ilminster, our core capabilities at the time centered on manufacturing scientific optical components and crystalline materials; skills that are still very much at the cornerstone of the current operation. In 1982 we diversified into fabrication of water cooled acousto-optic devices.
The acquisition of Optronic Laboratories allowed us to add the manufacture of optical radiation instrumentation products to our portfolio. Today we work with customers from all sectors in the provision of light measurement solutions.
Cleveland Crystals Inc. became part of G&H, adding a world class crystal growth facility. At the Cleveland site, in addition to growing crystals, we develop crystal optics and electrooptic devices for industrial, medical and scientific laser systems.
NEOS Technologies was one of the first to design and make acousto-optic devices for commercial use. New expertise in conduction-cooled and driver technology, broadened the range of applications for which we could supply acoustooptically controlled devices. In 2014 manufacturing was relocated to Palo Alto and Ilminster.
SIFAM Fiber Optics had worldwide renown in the design and manufacture of high reliability modular and passive components to the undersea telecoms, aerospace & defense and life science sectors. This acquisition allowed our diversification into a new area of photonics.
General Optics brought a unique capability in superpolished mirrors for scientific research and avionic and space applications.
ILMINSTER, UK
ORLANDO, FL
CLEVELAND, OH
MELBOURNE, FL
TORQUAY, UK
MOORPARK, CA
GOOCH & HOUSEGO
ABOUT US
Glenrothes PO
EOS Fremont AO
CO
CO
EO
PO Cleveland PO
Norderstedt
St. Asaph FO
FO
Bedford
Torquay
LMI
STG
Paris
HQ
AO
PO Nagoya
Ilminster
Orlando
Moorpark
Manufacturing locations Sales offices
Gooch & Housego now comprises nine state-of-the-art manufacturing sites in the US and UK.
Facts and Figures • Listed on London’s AIM Stock Exchange (GHH)
With sales offices in France, Germany, Japan, and a field-based sales team throughout the world, we are well prepared to help our customers to push technical, environmental, and economic boundaries with photonics technology.
• 2016 revenues of £86.1M • 755 employees
2011
2011
2013
2013
2016
2017
FIBER OPTICS
ACOUSTO-OPTICS
PRECISION OPTICS
RESEARCH AND DEVELOPMENT
ELECTRO-OPTICS SYSTEMS
PHOTONIC SOLUTIONS
EM4’s expertise as a manufacturer of active fiber optic components and subsystems and provider of photonic packaging services, added to our fiber optic capabilities. G&H now had a North American base for the supply of fiber optic solutions for performance in the harshest of environments.
Crystal Technology was a pioneer in the development of acousto-optic technology. Their considerable experience enabled us to expand the range of acoustooptic devices we could provide to customers in a variety of markets, notably in the area of crystal-based devices.
The acquisition of Spanoptic added the manufacture of aspheric optics and infrared coating to our range of precision optic capabilities.
Constelex Technology Enablers was an Athensbased designer and manufacturer of advanced photonic systems for satellite and space. This addition allowed us to couple our experience in fiber optic systems with specific expertise in space photonics to enable the next generation of satellite systems.
The acquisition of Wisconsin-based Alfalight, renowned for high reliability, rugged laser-based, electro-optic systems, and Kent Periscopes, North Wales, with its global reputation for armored fighting vehicle imaging systems, significantly reinforces G&H's capabilities in photonics based defense systems.
Through the acquisition of the best-in-breed companies Gooch & Housego has grown to become a global photonics technology leader with vertically integrated engineering,design, manufacturing and supply capabilities.
BEDFORD, MA
PALO ALTO, CA
GLENROTHES, UK
ATHENS, GREECE
MADISON, WI ST. ASAPH, UK
WORLDWIDE
GOOCH & HOUSEGO
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ABOUT US
SECTORS AND APPLICATIONS Gooch & Housego’s wide range of photonic devices are deployed across a uniquely broad range of applications, often in testing environments where extremes of atmospheric pressure, humidity, temperature or vibration are common.
AEROSPACE & DEFENSE Defense and avionics markets have been important drivers for our investment in operational quality and program management. As a trusted supplier for aerospace & defense prime contractors, G&H has invested in robust systems and processes to ensure compliance with import and export regulations, export licensing, ITAR-controls, documentation and revision control, extreme environmental performance, and accounting documentation such as FAR and CAS. We continue to invest in our continuous improvement and lean manufacturing programs, as well as production equipment and metrology to better serve our most demanding aerospace and defense customers.
Communications Tactical communications require rugged, hi-reliability components and sub-systems; in some instances light weight for maximum mobility. We support a number of C4ISR (command, control, communications, computers, intelligence, surveillance, and reconnaissance) applications including: • • •
RF over fiber Secure fiber optic networks Surveillance and target acquisition
Our military-grade components are designed for survivability under extreme conditions, manufactured in AS9100C facilities, and qualified to the necessary Telcordia, BSI, DIN, or MIL specifications as required. Active components are hermetically sealed. Many are ROHS compliant. We manufacture in both the UK and the US, enabling maximum flexibility for customers who require ITAR compliance.
Head-up Displays Heads-up displays (HUDs) comprise three main sub-systems: a projector, a combiner, and a video generating computer. A sub-set of the HUD is the head (or helmet) mounted display (HMD), where the HUD components are miniaturized. Originally developed for military applications, they are now used in an ever-growing number of commercial applications: automotive HUDS, gaming, and wearables. G&H’s expertise in designing and developing components for imaging, as well as its capability to miniaturize sub-systems, is well-leveraged in this arena: • • •
Beam combiners for HUD and HMDs Lens systems for projection Waveguides for space constrained projection
Imaging under Extreme Conditions Sights, telescopes, periscopes, and other imaging systems have long played a role in defense. In recent years photonics has since broadened imaging systems to a wide variety of conditions (night, fog and haze, smoke, sand storm, aerial, and space) and adapted to a range of situations: • • • • •
Building and asset surveillance Firefighting, policing, and hunting Low-light/night vision surveillance LIDAR mapping Hyper-spectral imaging and target identification
G&H provides a wide variety of photonic components, sub-assemblies, and systems into these applications: • • • • •
Beam steering lenses, mirrors, and prisms Prism and lens assemblies Electro-optic zoom lenses Periscopes and vision blocks Electro-optic sighting systems for armored vehicles
Passive and active components include: • • • • •
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HI REL fused fiber couplers DFB lasers and modules High power pump combiners HI REL amplifiers PM fiber couplers
GOOCH & HOUSEGO
ABOUT US
Target Designation and Rangefinding used on Land-Based and Airborne Systems
Countermeasures for Ground-Based Systems and Airborne Platforms
From missiles to guided bombs, photonic targeting and rangefinding systems ensure correct deployment of the munition. Extreme conditions require athermalized, instant “on” systems.
Infrared countermeasures protect military assets from missile attacks by confusing the seeker guidance system. These systems require accurate modulation of the infrared energy under extreme environmental conditions.
G&H designs and delivers a wide variety of sub-systems and components to prime contractors:
We provide fiber optic, acousto-optic, and nonlinear crystal products which are used in customer-specific countermeasure applications, both ground based and airborne.
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Micro-optical packaging for missile systems Prism assemblies for lightweight target designators EO modulators and Q-switches for rangefinding laser systems Fiber optic gyroscopes (FOG) for navigation Polarization components, hybrid lenses and lens assemblies for rangefinding and target designation
Gyroscopes for Navigation Gyroscopes are used in inertial navigation systems in aircraft, guided missiles, submarines, ships, and spacecraft for rotation sensing to measure or maintain orientation. We design and produce ring laser gyroscopes (RLGs) and fiber optic gyroscopes (FOG) which are deployed in commercial aircraft as well as missiles, satellites, and other military vehicles. ITAR and ITAR-free programs are managed in both the US and the UK.
The U.S. Army via VisualHunt.com /CC BY
Courtesy of ESA
Crown Copyright 2012
GOOCH & HOUSEGO
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ABOUT US
SPACE G&H has a proven track record in the design and development of space hardware for international space agencies including European Space Agency (ESA), National Aeronautics and Space Administration (NASA) amongst others. Commercial projects include systems and components, modules integrated within operational satellites and on board the probes and rovers. We maintain a leading role in research and development programs in Europe, the USA and Asia, through multiple projects and contracts centered on optical inter- and intrasatellite communication links. Our work on space projects fuels the company roadmap on a new generation of product lines.
Fiber Optics G&H develops space-grade fused and photonic components, including lasers, detectors, and couplers. We have also developed and deployed fiber-optic laser communication sub-systems.
Precision Optics We develop and manufacture world-class precision optical components and assemblies with space flight heritage, including reflective and superpolished optics on remote sensing satellites and rovers.
G&H works with major prime contractors and government agencies on ground-breaking scientific and technology development programs for: • • •
Communication Earth observation and deep space Navigation
Our enabling technologies cross many disciplines.
Acousto-Optics Exploiting our 40-year experience in manufacturing acoustooptic modules, we develop space-qualified versions of AO tunable filters and switches. Our products have a rich space heritage and are flying on-board ExoMars, Hayabusa-II, and Lisa PathFinder amongst others.
Courtesy of SSTL
Courtesy of ESA
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Courtesy of ESA
GOOCH & HOUSEGO
ABOUT US
INDUSTRIAL Photonics plays an ever-increasing role in industrial manufacturing, replacing formerly mechanical, chemical, or electrical production processes, or increasing production quality and conformance by replacing manual inspections or batch testing. G&H serves these applications and markets with an expanding product portfolio, from components to sub-assemblies and final test and measurement equipment.
PRODUCTION TECHNOLOGIES Laser Material Processing Laser material processing is a broad term which encompasses production processes such as ablating, bending, cutting, curing, forming, fusing, marking, micro-machining, sintering, thermal annealing, via drilling, or welding. For these applications, we design and manufacture products which are used in laser cavities, to steer and control or to modulate the beam. Our products serve wavelength ranges from the UV to the FIR, usually with very high laser damage thresholds. Examples include: • • • • •
Beamsplitters, polarization control components, lenses, mirrors, windows, and beam dumps Bulk optic and fiber optic based modulators and Q–switches Fiber components for fiber lasers or fiber-fed amplifiers and laser systems Laser cavity mirrors, pulse pickers, output couplers, attenuators, frequency shifting non-linear crystals Metrology tools and instrumentation
Printing In lithography and micro-lithography, the production process is inherently photonic in nature. Computer-to-plate technologies, flexographic, and offset printing production components utilize laser processing to create the printing tools. We provide a variety of optical components into these applications where accurate transmitted wavefronts and high energy tolerance provide superior printed image quality and longevity in production. Fiber Q-switches are used in the cavities of fiber lasers which are the primary tool for the engraving of anilox rolls used in flexographic printing.
GOOCH & HOUSEGO
TEST AND MEASUREMENT Photonics is used across a wide variety of applications to ascertain quality, damage, motion, chemical composition, temperature, location, distance, or automation of these types of tests.
Non-Destructive Testing Photonics is applied to non-destructively determine aircraft worthiness, find bruises in fruits and vegetables, or assess the chemical purity of a pharmaceutical pre-agent or final product. For LED and display testing applications, we provide test and measurement instrumentation and calibration standards used to manufacture products used in lighting, automotive, and consumer electronics. For a wide variety of laser-based, high-precision, noncontact metrology systems, including agricultural moisture measurements, food production, forestry analysis, metal and glass production, photovoltaic manufacturing, and waste recycling, we supply: • • • •
Precision optics and lens systems SWIR low-f# lens assemblies Zoom lens assemblies Polarization control optics from custom prism and cube assemblies to high precision waveplates 7
ABOUT US
Stand-off Measurements Commercial LIDAR and hyperspectral imaging can be used to determine water content of crops, fire danger of a forest, map cities for urban planning, and select drilling locations. G&H serves these applications across the product platform: rugged fiber optics, Q-switches for laser cavities, and precision optics. Components for airborne systems are engineered for long-lifetimes in the field. ITAR and non-ITAR options are available in the US and the UK. Telemetry can be utilized to track the location of livestock, herds of endangered animals, whales, fish and game. It can track spacecraft, oil rigs and wind farms, or monitor agricultural conditions.
Semiconductor Lithography Manufacture, Test and Measurement A unique sub-sector of metrology is found in semiconductor and microelectronic production lines to test, qualify, and quantify performance. Manufacturers generally separate semiconductor metrology from other branches due to the unique requirements and needs of semiconductor manufacturing: •
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Our components are well-suited for these applications: • • •
Proven longevity in the field High durability coatings and designs Athermalized assembly designs
Examples include: • • •
High reliability (HI REL) fiber optics, DFB lasers, and amplifiers Precision optics Athermalized SWIR lens assemblies
Extreme precision in imaging and wavefront control is needed when features are nm in dimensions and small errors can result in millions of dollars lost Production tools must be precise and long-lasting in an aggressive UV environment Post-production tools require accurate positioning and beam exposures
G&H supplies components, sub-systems, and assemblies optimized for each environment. • • •
Q-switches and laser cavity optics for production tooling Imaging optics for metrology Post-production optical components for applications as wide ranging as laser trimming and laser voltage probing in the infrared
Sensing Fiber optics are deployed in a wide variety of sensing applications. These applications may use fiber simply as the communication medium for speed, lack of ignition sources, or weight. They may also integrate fiber gratings as the sensor to leverage the superior resolution. We supply fiber optic and acousto-optic sub-assemblies and components to equipment manufacturers and installers of these systems: • • •
High reliability (HI REL) fiber optic couplers, lasers, and amplifiers Fiber-coupled and free space Q-switches Acousto-optic tunable filters
TELECOMMUNICATIONS We serve the more demanding applications within telecommunications. Our customers deploy our fiber-based products in undersea networks and in space for satellite-tosatellite communications. We provide ITAR and non-ITAR designs out of our UK or US manufacturing facilities.
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GOOCH & HOUSEGO
ABOUT US
LIFE SCIENCES
SCIENTIFIC RESEARCH
G&H serves the life sciences markets with photonics engineering solutions from across the company’s technology portfolio.
G&H works with some of most prestigious Big Science projects in the world.
Optical Coherence Tomography (OCT) Widely used for ophthalmic imaging, OCT has proven invaluable in improving the diagnosis of glaucoma and macular degeneracy. We serve most of the world’s leading manufacturers of OCT retinal imaging systems. We partner with key customers to develop OCT systems for cancer detection, cardiological imaging, and emerging new medical diagnostic applications.
We are a primary supplier of many critical optical components such as very large frequency conversion crystals used in the world’s most powerful laser system at the National Ignition Facility (NIF) at Lawrence Livermore National Laboratory. We supply similar products to the Commissariat à l'énergie atomique et aux énergies alternatives (CEA) and other inertial confinement fusion (ICF) programs around the world. G&H also manufactures superpolished optics for leading edge synchrotron experiments around the world.
G&H provides a complete family of fiber optic products: • • • •
Discrete components Interferometers Spectrometers and other modules Full OCT optical systems
Medical and Cosmetic Laser Systems G&H is helping develop new fiber-delivered laser products which enable less invasive surgical techniques. Applications include cataract replacement, vision correction, prostate surgery, varicose vein treatment, and mole treatment in addition to tattoo removal, teeth whitening, freckle removal, and wrinkle reduction.
Courtesy of Michelson Diagnostics Ltd
G&H supplies critical optical components such as: • • •
Acousto-optic modulators and fiber optic assemblies to system manufacturers Q-switches and precision optics for laser cavities Beam control and steering optics to system manufacturers
Biomedical Microscopy Laser-based techniques such as multi-photon and super-resolution microscopy enable real time in vivo imaging of subcellular processes and revolutionizing our understanding of cellular biology. G&H is developing systems for new wavelengths to enhance deep brain imaging and early cancer detection.
Courtesy of LLNL
We supply optical components and sub-assemblies for these and other applications to both laser system and microscope manufacturers: • • • •
Acousto-optic tunable filters for confocal microscopy Lens assemblies Polarization control optics Q-switches and cavity optics for lasers
GOOCH & HOUSEGO
Courtesy of Michelson Diagnostics Ltd
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ABOUT US
CONTINUOUS IMPROVEMENT Our goal is to deliver expertise and excellence by every one of our staff, every day. Our lean manufacturing initiatives enable us to maximize product quality, optimize manufacturing efficiency and deliver the highest quality products to our customers in the most cost-effective way. DRIVING CUSTOMER SATISFACTION
OUR TOOLS AND SYSTEMS
We strive to push the boundaries of our capabilities and manufacturing efficiency; passing on the benefits to our customers by providing high quality, durable and costeffective assemblies and components.
Establishing a Strong Foundation
This requires innovation in our products and our processes and continuous improvement is central to this evolution.
True North: "World class begins with everyone every day" means that all employees are engaged at all times in the improvement process, and in the design and deployment of tools and training.
The G&H Operating System is built upon a foundation of core principles and processes that we rely on to guide every deployment of lean manufacturing.
Customers come to G&H because we have innovative products, the ability to offer technologically leading customized solutions, and expertise in photonics engineering and manufacturing; enabling them to innovate.
This results in improvement in flow, reduction in waste, and an increase in output. In this way we better meet, if not exceed, customer needs and expectations.
G&H customers need short lead times, on-time delivery, and quick reaction to demand or design changes, as their customers’ requirements change. This is the impetus behind our investment in continuous improvement across every facet of our business.
Three pillars support our lean manufacturing initiative: Flow: The first tool optimizes continuous flow within order management, manufacturing, and product delivery. Our empowered workforce: At the center of our company, and our success, is our workforce. We look to our workforce to initiate and sustain these improvements.
In response, we have embarked upon a worldwide deployment of the G&H Operating System which was built to advance lean manufacturing principles in all of our sites.
Designing in quality: A quality system which relies upon an inspection filter inherently creates waste. Parts which are made right the first time flow through the system directly to the customer.
Our lean manufacturing culture systematically drives customer satisfaction and operational excellence.
G&H OPERATING SYSTEM
QUALITY
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COST
WORKFORCE
QUALITY
Production Levelling
Health and Safety
Voice of Customer
Value Streams
Personal Development
Quality Assurance
Cellular Manufacturing
Motivation
Quality Compliance
Pull Systems
Maintaining Standards
Fact Based Decisions
Kanban
Lean 6σ Culture
DMAIC/Six Sigma
Demand Capacity
Question Without Judgement
Error Proofing
TPM
Respect for Others
Quality Methods
SMED
Continual Learning
Mistake Proofing
6S
Visual Management
Employee Empowerment
Standards
Waste Elimination
Problem Solving
Kaizen
SYSTEMS
FLOW
FOCUS
DELIVERY
TRUE NORTH: WORLD CLASS BEGINS WITH EVERYONE, EVERY DAY
CULTURE
SYSTEMS
Employee Engagement
CULTURE
SAFETY
Shareholder Satisfaction
Lean principles and processes underpin the three pillars that deliver operational excellence. GOOCH & HOUSEGO
FOCUS
Customer Satisfaction
RESULTS
RESULTS
OPERATIONAL EXCELLENCE
ABOUT US
World class begins with everyone, every day
INVESTING IN A LEAN FUTURE STANDARDIZE
Repeat every 3-6 months
IDEAL FUTURE STATE “Ultimate Goal”
CURRENT STATE
Employee empowerment – Enables our workforce to improve, innovate, and communicate. KAIZEN FLOW
Standards – Standardized work forms the baseline for continuous improvement.
Improving Value for the Customer The five principles of lean thinking begin and end with the customer.
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6S – Formerly known as 5S + safety, this fundamental methodology is quite simple: sort, straighten, shine, standardize, and sustain. Visual management – Enables the teams to see what and how they are doing through visual control charts and other monitoring methods.
FUTURE STATE
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Our lean principles and processes:
Know what the customer considers is willing Standardize Idealvalue, and to pay for Future State “Ultimate Map the Value Stream, analyzing theGoal” wastes that exist Future within the processes State Create flow through elimination of errors and waste Current Create pull system responding to customer demands State Continuously improve in pursuit of perfection
Waste elimination – G&H focuses on eight deadly wastes: defects, overproduction, waiting, non-value added processing, transportation, inventory excess, motion, and employee-related. Problem solving – G&H utilizes four approaches: plan, do, check, act (PDCA); 5-why analysis, fishbone diagrams, and simplified failure mode and effects analysis (FMEA). Kaizen – Japanese for “improvement”. Typically Kaizen events are scheduled activities to re-organize, re-arrange, or re-tool production to improve flow.
IDENTIFY VALUE
PLAN
PURSUE PERFECTION
MAP VALUE
VALUE MAPPING
PULL SYSTEMS
GOOCH & HOUSEGO
ACT
CREATE FLOW
CONTINUAL IMPROVEMENT
DO
CHECK
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ABOUT US
QUALITY MANAGEMENT DELIVERING EXCELLENCE Combined with our vision of continuous improvement, the core principles and processes, systems and tools facilitate the operational excellence that delivers successful outcomes: customer satisfaction, shareholder satisfaction, employee engagement and a more robust supply chain. Quality Management System for Product and Sites G&H’s continued focus on quality management systems (QMS) across all of our UK and US manufacturing sites, as part of the accreditation standardization process benefits our customers in many ways: • • • • • •
Improved consistency Improved reliability Improved traceability Reduced risk Reduction of waste and downstream costs Improved sustainability
Our quality management strategy is constantly evolving, with the following four standards: ISO9001, AS9100C, OHSAS 45001 and ISO 14001, forming the basis of our current and wider deployment plans for the future.
ISO 9001
Aerospace Industry quality management system. G&H is gaining certification in facilities that serve the aerospace and space industries in addition to transitioning to Rev D.
AS 9100C
OHSAS 45001
Longer term plans exist for a wider site coverage for the International standard for the environmental management of our business.
Currently certified to ISO9001:2008, G&H in the process of transitioning to ISO9001:2015.
International standard for Occupational Health & Safety. 45001 will replace 18001 by the end of 2017, so in the meantime G&H have adopted 18001 as an aspirational target in preparation for the 45001 standard.
ISO 14001
Compliance G&H recognizes that compliance with export regulations, material sources, and material regulations around the world is an important activity. Legislative changes, worldwide, have driven the recent expansion of this function. Our compliance managers are focused on ensuring we provide the necessary documentation to support our customers. This information includes an ever-expanding range of regulations, of which these are the most common: • • • • • •
International Traffic in Arms Regulation (ITAR) UK Export Control Organization (UK ECO) US Export Administration Regulations (US EAR) EU Restriction of Hazardous Substances (RoHS) EU Registration, Evaluation, Authorization, and Restriction of Chemicals (REACH) Conflict Minerals Compliance (Section 1502 of the US Dodd-Frank Act of 2010)
Our sales staff, together with country-specific compliance managers, are able to readily provide customers with compliance information or documentation on request.
WORK IN PROCESS, NOT AN END STATE Continuous improvement is just that: continuously improving our products and our processes to improve flow, to remove waste, and to improve our products and services. As part of this activity a more proactive quality deployment within the product lifecycle is being realized. Inputs from the recent customer satisfaction survey are also being incorporated as part of this exercise. We look forward to updating our customers on our progress and to learn about how we can improve our systems to support our customers’ own lean initiatives. The latest news about our lean manufacturing and QMS initiatives can be found at: goochandhousego.com/news
WOR
Precision is at the heart of everything we do
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ISO90 Curren AS910
GOOCH & HOUSEGO
Aeros certifi
OHSA Intern
AO ACOUSTO-OPTICS Gooch & Housego has been a leader in acousto-optic device design and manufacturing since 1979, bringing together some of the best minds and technologies in the field to create a comprehensive line of high-quality products backed by premier service and reliability.
Capabilities
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Products Beam Deflectors
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Frequency Shifters
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Mode Lockers
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Modulators 18 Fiber-Q® Fiber-Coupled Modulators
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Multi-Channel Modulators
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Pulse Pickers/Cavity Dumpers
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Q-Switches 24 Tunable Filters
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RF Drivers
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ACOUSTO-OPTICS
TECHNICAL EXPERTISE AND MANUFACTURING CAPABILITIES G&H acousto-optic components are characterized by unmatched optical power handling, optical performance delivered consistently over time and in volume, and designs optimized for a wide variety of applications.
Acousto-optic products covering wavelengths from the ultraviolet to the infrared are available in a wide range of optical materials, including TeO2 grown in-house, to minimize distortion, scatter, and transmission loss. Depending on the product type, we optimize transducer geometry to drive the acousto-optic crystal: longitudinal (compressional) acoustic mode or shear acoustic mode. Special attention is given to the transducer orientation to maximize electrical to acoustic conversion efficiency. Cold weld metal bonding and thermal expansion coefficient matching are used to provide a strong, reliable, low-loss attachment of the piezoelectric transducer to the interaction material, improving durability over broad operating temperature ranges. We use technology such as apodized electrodes and phased array electrode designs to optimize the shaping of the acoustic field for each application, and wirebond the control electronics for a reliable, environmentally durable, low loss connection. Wirebonding also minimizes acoustic absorption at the transducer connection points. Device packaging is designed to minimize thermally-induced wavefront distortion and beam wander during operation, and to extend product lifetime. Transducers are impedance matched to 50 Ω to allow
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for testing and use with industry standard RF equipment. RF drivers are specifically designed to drive our acousto-optic products at peak performance, with options customized to each application. Decades of experience working with OEM partners around the world has given us the understanding to develop, design, and manufacture for extremes of temperatures, radiation, shock, and vibration. AO Drive Power (Relative) 100
Diffraction efficiency (relative) [%]
This is a result of our control of every aspect of the design and fabrication of the entire acousto-optic product line, from growth of lithium niobate (LiNbO3) transducer material and tellurium dioxide (TeO2) crystals in-house, to polishing, antireflection coating, fabrication and device testing.
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RF drive power (relative) [%]
Graph showing relative diffraction efficiency (DE) and RF drive power for an AO modulator. The drive power and DE are normalised for peak efficiency (100% DE) at 100% drive power.
GOOCH & HOUSEGO
ACOUSTO-OPTICS
BEAM DEFLECTORS Designed for high speed, solid state scanning applications Acousto-optic beam deflectors (AOBD) offer precise angular control of an optical beam using RF drive frequency tuning. Up to two thousand spots can be resolved over an angular range of a few degrees for 1D and 2D scanning as well as beam deflection through a fixed angle. The scan speed can be as fast as a few microseconds. G&H beam deflectors offer highly uniform diffraction efficiency across the full scan angle, with consistent power throughput for scanning applications such as material processing and digital imaging. We manufacture devices based on tellurium dioxide crystals grown in-house for visible and near-infrared (NIR) wavelength applications. For optimal transmission in the ultraviolet (UV) we offer fused silica and crystal quartz products. For broad bandwidth applications, we use a longitudinal mode approach with a phased array of piezoelectric elements within the transducer. We achieve high efficiency with slow shear deflection using parallel tangents off-axis interaction. 2D UV beam scanning may be achieved by cascading two UV deflectors in series. Our flexible functionality Smart Dual Driver with phase synchronized outputs offers the optimum in RF driver control for 2D scanning. As high density material processing moves to smaller features written by shorter wavelengths, greater beam control is essential. Our deflectors meet these needs with highly accurate, repeatable positioning as well as rapid, agile, random access control for higher throughput.
Applications Digital imaging, heterodyne interferometry, laser cooling, laser marking, laser tweezers, material processing, micromachining, microscopy, on-line process control, optical inspection, photolithography, printing.
Contact us to discuss customized beam deflection solutions or multi-channel beam deflectors with high speed for volume OEM applications. PRODUCT CODE
WAVELENGTH
SCAN ANGLE
ACTIVE APERTURE
OPERATING FREQUENCY
OPTICAL MATERIAL
AOBD 2960-UV
266 nm
NA
0.8x67 mm
230-430 MHz
Sapphire
AOBD 4200-UV
266 nm
10.3 mrad
1.0x60.0 mm
135-265 MHz
Fused silica
AOBD 4170
355 nm
4.9 mrad
7 mm
130-210 MHz
Crystalline quartz
AOBD 4100-UV
364 nm
29.5 mrad
4.0x14.0 mm
75-125 MHz
Tellurium dioxide
AOBD 4090-7
440-530 nm
44 mrad
8.5 mm
60-115 MHz
Tellurium dioxide
AOBD 4200-VI
442-488 nm
29.5 mrad
4.8 mm
150-250 MHz
Tellurium dioxide
AOBD 4100-VI
488 nm
39.5 mrad
4.0-14 mm
75-125 MHz
Tellurium dioxide
AOBD 4080-13
635 nm
8.2 mrad
2 mm
76-84 MHz
Tellurium dioxide
AOBD 4055-4
780-980 nm
44.3 mrad
3.5x14 mm
35-70 MHz
Tellurium dioxide
AOBD 4210-IR
830 nm
27.6 mrad
2.0-6.0 mm
140-280 MHz
Tellurium dioxide
AOBD 4090-6
1064 nm
56 mrad
2 mm
72.5-107.5 MHz
Tellurium dioxide
AOBD 4075-IR
1065-1100 nm
8.1 mrad
2.5 mm
59-91 MHz
Tellurium dioxide
AOBD 4070
9.4 µm
60 mrad
9 mm
50-90 MHz
Germanium
GOOCH & HOUSEGO
15
ACOUSTO-OPTICS
FREQUENCY SHIFTERS Dependable shift with high extinction ratio Like other acousto-optic devices, an acousto-optic frequency shifter (AOFS) Doppler-shifts the frequency of input light by an amount equal to the RF drive frequency, but is optimized specifically for this purpose. Typically our frequency shifters will use the anisotropic interaction of the slow shear mode in tellurium dioxide (TeO2). Applications such as interference-based optical techniques require a high extinction ratio between the diffracted and undiffracted beam; this can be achieved with a high-quality optical finish to minimize optical scatter. We offer standard products with frequency shifts of 40-350 MHz, many of which can be operated in double-pass configurations. In addition we can design for custom frequency shifts where required. Frequency shifters are fabricated using high quality TeO2, grown and polished in-house, for lowest insertion loss and excellent power handling. Other acousto-optic materials are available and may be more appropriate for some applications. TeO2 based frequency shifters are highly efficient acousto-optic devices, requiring very low drive power to achieve the desired frequency shift. Our designs consume minimal power (generally <100 mW power draw), often allowing us to package the driver with the AOFS for a more compact and power-efficient solution.
Applications Interferometry, laser cooling, laser Doppler velocimetry, laser Doppler vibrometry (LDV), optical heterodyne detection.
The products listed below illustrate a range of typical specifications. Our product managers and application engineers routinely work with customers, applying our expertise to customize products to meet the demands of their specific applications. PRODUCT CODE
WAVELENGTH
OPERATING FREQUENCY
ACTIVE APERTURE
INTEGRATED DRIVER
OPTICAL MATERIAL
I-M110-3C10BB-3-GH27
300-400 nm
110 MHz
3.0 mm
No
Crystal quartz
AOMO 3080-125
440-850 nm
80 MHz
2 mm
No
Tellurium dioxide
AOMO 3100-125
440-850 nm
100 MHz
1.5 mm
No
Tellurium dioxide
AOMO 3200-125
440-850 nm
200 MHz
1.5 mm
No
Tellurium dioxide
AOMO 3270-125
440-850 nm
270 MHz
1.5 mm
No
Tellurium dioxide
AOMO 3350-125
440-850 nm
350 MHz
1.5 mm
No
Tellurium dioxide
I-FS040-1.5S2C-3-GH83
532 nm
40 MHz
1.5 mm
No
Tellurium dioxide
I-FS040-1.5S2C-1-GH66
532 nm
40 MHz
1.5 mm
Yes
Tellurium dioxide
I-FS080-3S2E-1-GH39
633 nm
80 MHz
3 mm
Yes
Tellurium dioxide
I-FS080-3S2E-3-LG5
633 nm
80 MHz
3 mm
No
Tellurium dioxide
I-FS040-2S2E-1-GH66
630-690 nm
40 MHz
2 mm
Yes
Tellurium dioxide
I-FS040-2S2E-3-OL3
630-690 nm
40 MHz
2 mm
No
Tellurium dioxide
AOFS 4040-191
633-1064 nm
40 MHz
2x6 mm
No
Tellurium dioxide
I-FS080-2S2G-3-LV1
1064 nm
80 MHz
2 mm
No
Tellurium dioxide
I-FS040-2S2J-3-GH53
1550 nm
40 MHz
2 mm
No
Tellurium dioxide
I-M040-2C8J-3-GH84
1550 nm
40 MHz
2 mm
No
AMTIR
I-M040-2C8B1-3-GH84
1900-2100 nm
40 MHz
2 mm
No
AMTIR
16
GOOCH & HOUSEGO
ACOUSTO-OPTICS
MODE LOCKERS For high power, high-Q mode locking of ultrafast laser pulses An acousto-optic mode locker (AOML) modulates the loss within a laser cavity at its resonant frequency, effectively “locking” the phase of the longitudinal modes to generate very narrow laser pulses of high intensity. G&H standing wave mode lockers yield near-theoretical mode locked laser pulse widths, with industry-leading transmission performance. Available in antireflection (AR) coated and Brewster angle options, they can also be customized for demanding one-off scientific and OEM applications. We combine extensive AO device design experience with strict manufacturing controls to deliver high-Q (very low loss) mode lockers with minimal extraneous modes, achieving picosecond and femtosecond length pulses at repetition rates of up to 200 MHz. To ensure high quality and reliability, our mode lockers use high quality fused silica, polished and fabricated in-house. Greater than 99% transmission at 1064 nm is achieved with our own durable antireflection V-coat. Transmission over a broader range of wavelengths (700-1100 nm) can be achieved using windows cut to the Brewster angle. Low scatter and tight quality controls ensure that every mode locker is capable of handling high peak laser power over the long term without damage. RF driver selection impacts mode locking system performance, as active temperature control of the acoustic resonator can assist in controlling resonant frequency such that resonance at the precise frequency of the driver’s oscillator can be maintained. G&H can assist in choosing the right driver for your application, advising on how performance of each RF driver will influence mode locking efficiency and pulse width.
Applications Femtosecond micromachining, fs/ps lasers (Nd:YAG, Nd:YLF, Ti:Sapphire, Argon ion), LIDAR, multiphoton microscopy, nonlinear optics, optical data storage, optical heterodyne detection for spectroscopy, telecommunications.
From custom wavelengths to high repetition rates, we offer a wide range of standard and custom options for high performance, high-reliability mode lockers to achieve the shortest, most intense pulses possible. PRODUCT CODE
WAVELENGTH
OPERATING FREQUENCY
ACTIVE APERTURE
WINDOW TYPE
OPTICAL MATERIAL
I-ML041-3C4G-3-GH101
1064 nm
41 MHz
3 mm
AR coated
Fused silica
I-ML080-3C4G-3-GH101
1064 nm
80 MHz
3 mm
AR coated
Fused silica
I-ML041-4.5C4R4-3-GH102
700-1100 nm
41 MHz
4.5 mm
Brewster
Fused silica
I-ML080-4.5C4R4-3-GH102
700-1100 nm
80 MHz
4.5 mm
Brewster
Fused silica
GOOCH & HOUSEGO
17
ACOUSTO-OPTICS
MODULATORS Single frequency devices allowing intensity modulation of collimated light Acousto-optic modulators (AOM) allow the intensity of light to be controlled and modulated at rates that far exceed mechanical shutters. AOMs can be used like a shutter (cycling light on and off at a set frequency), or as a variable attenuator (controlling the intensity of transmitted light dynamically). The laser modulation is effected by means of RF interference induced sound waves in an acousto-optic crystal. G&H acousto-optic modulators are optimized for low scatter and high laser damage threshold, and can be matched to the rise time, modulation rate, beam diameter, and power handling needs of each application. Rise time is proportional to the time required for the acoustic wave to traverse the optical beam and for this reason is influenced by the beam diameter within the AOM. We offer very fast modulators with modulation frequencies up to ~80 MHz and rise time as low as 4 ns, requiring the input beam to be very tightly focused. Lower frequency modulators do not have this constraint, and can accept larger input beams. Their rise time is usually specified relative to the input beam diameter, in ns/mm. Our modulators typically achieve extinction ratios of >50 dB, usually with a deflected beam throughput of 85-90%. For applications such as intensity leveling where a lower contrast ratio of ~10 dB is acceptable, we offer modulators with >99% light throughput. Applications Heterodyne interferometry, intensity levelling, intensity modulation, laser cooling, laser Doppler velocimetry, laser Doppler vibrometry (LDV), laser linewidth measurements, LIDAR, marking, material processing, micromachining, printing, via drilling.
The standard products listed below and on the following page illustrate a range of typical G&H AOM specifications. Our product managers and application engineers routinely work with customers, applying our expertise to customize products to meet the demands of their specific applications. PRODUCT CODE
WAVELENGTH
RISE/FALL TIME
ACTIVE APERTURE
OPERATING FREQUENCY
OPTICAL MATERIAL
I-M110-5C10R19-4-GH116
193-266 nm
110 ns/mm
5 mm
110 MHz
Crystalline quartz
AOMO 3200-1220
257 nm
113 ns/mm
0.25 mm
200 MHz
Crystalline quartz
I-M110-3C10BB-3-GH27
300-400 nm
113 ns/mm
3 mm
110 MHz
Crystalline quartz
I-M110-3C10T-3-GH72
355 nm
113 ns/mm
3 mm
110 MHz
Crystalline quartz
I-M110-6.5C10T-4-GH112
355 nm
113 ns/mm
6.5 mm
110 MHz
Crystalline quartz
I-M110-2C10B6-3-GH26
400-540 nm
113 ns/mm
2 mm
110 MHz
Crystalline quartz
AOMO 3200-121
442-488 nm
153 ns/mm
0.32 mm
200 MHz
Tellurium dioxide
AOMO 3200-120
442-488 nm
153 ns/mm
0.45 mm
200 MHz
Tellurium dioxide
AOMO 3110-121
442-488 nm
153 ns/mm
0.6 mm
110 MHz
Tellurium dioxide
AOMO/AOFS 3080-125
440-850 nm
153 ns/mm
2 mm
80 MHz
Tellurium dioxide
AOMO/AOFS 3100-125
440-850 nm
153 ns/mm
1.5 mm
100 MHz
Tellurium dioxide
AOMO/AOFS 3200-125
440-850 nm
153 ns/mm
1.5 mm
200 MHz
Tellurium dioxide
18
GOOCH & HOUSEGO
ACOUSTO-OPTICS
PRODUCT CODE
WAVELENGTH
RISE/FALL TIME
ACTIVE APERTURE
OPERATING FREQUENCY
OPTICAL MATERIAL
AOMO/AOFS 3270-125
440-850 nm
153 ns/mm
1.5 mm
270 MHz
Tellurium dioxide
AOMO/AOFS 3350-125
440-850 nm
153 ns/mm
1.5 mm
350 MHz
Tellurium dioxide
AOMO 3110-120
440-850 nm
153 ns/mm
0.6 mm
110 MHz
Tellurium dioxide
AOMO 3080-120
440-850 nm
153 ns/mm
1 mm
80 MHz
Tellurium dioxide
AOMO 3350-120
488-532 nm
153 ns/mm
0.1 mm
350 MHz
Tellurium dioxide
I-M080-2C10B11-4-GH95
700-1000 nm
113 ns/mm
2 mm
80 MHz
Crystalline quartz
AOMO 3200-124
780-850 nm
153 ns/mm
0.32 mm
200 MHz
Tellurium dioxide
AOMO 3080-122
780-850 nm
153 ns/mm
1 mm
80 MHz
Tellurium dioxide
AOMO 3200-1113
870-1250 nm
153 ns/mm
0.1 mm
200 MHz
Tellurium dioxide
I-M080-2C10G-4-AM3
1030-1064 nm
113 ns/mm
2 mm
80 MHz
Crystalline quartz
I-M080-4C10G-4-GH60
1030-1064 nm
113 ns/mm
4 mm
80 MHz
Crystalline quartz
I-M068-5C10G-U5-GH100
1030-1064 nm
113 ns/mm
5 mm
68 MHz
Crystalline quartz
AOMO 3110-197
1030-1090 nm
153 ns/mm
1.25 mm
110 MHz
Tellurium dioxide
AOMO 3080-194
1060 nm
153 ns/mm
1.75 mm
80 MHz
Tellurium dioxide
AOMO/AOFS 3165-1
1300-1550 nm
153 ns/mm
0.6 mm
165 MHz
Tellurium dioxide
I-M040-2C8J-3-GH84
1550 nm
260 ns/mm
2 mm
40 MHz
AMTIR
I-M041-3C2V5-4-IS8
2000 nm
153 ns/mm
3 mm
40.68 MHz
Tellurium dioxide
I-M041-1.4C10V5-4-GH49
1900-2100 nm
113 ns/mm
1.4 mm
40.68 MHz
Crystalline quartz
I-M040-2C8B1-3-GH84
1900-2100 nm
260 ns/mm
2 mm
40 MHz
AMTIR
I-M0xx-xxC11B76-P5-GH105
5.5 µm
120 ns/mm
7.0, 9.6 mm
40/60 MHz
Germanium
I-M050-xxC11V41-P3-GH75
9.4 µm
120 ns/mm
9.6, 11.6 mm
40/60 MHz
Germanium
I-M041-xxC11xxx-P5-GH77
9.4/10.6 µm
120 ns/mm
3.5, 7.0, 9.6, 11.6 mm
40.68 MHz
Germanium
GOOCH & HOUSEGO
19
ACOUSTO-OPTICS
FIBER-Q® FIBER-COUPLED MODULATORS Reliable, high performance fiber-coupled modulators Fiber-coupled acousto-optic modulators (AOMs) are a compact, robust solution for fiber laser modulation and frequency shifting, allowing direct control of the timing, intensity, and temporal shape of the laser output. Direct integration of a fiber optic acousto-optic modulator into a fiber-based system allows the optical path to remain closed for better power handling and reliability, in addition to lower loss. Our award winning Fiber-Q® modulators offer high extinction ratio, low insertion loss, and excellent stability in both polarization-maintaining (PM) and non-PM formats at modulation frequencies up to 80 MHz. Built for reliability, these products feature rugged hermetic designs in compact, low-profile packages, ideal for ease of integration into all-fiber and OEM systems, including medical laser systems. We grow our own tellurium dioxide (TeO2) crystals in-house, polishing and performing all stages of fabrication to achieve low scatter and rigorous quality standards throughout the manufacturing process. This ensures consistently high reliability, high laser damage threshold and high optical performance. G&H continues to lead the market in the development of fiber-coupled modulators, offering the first devices for visible wavelengths from 450 nm to 780 nm to meet the needs of biomedical and sensing applications. Our new fast switch rate Fiber-Q® devices enable efficient, high speed optical pulse picking at infrared wavelengths for all-fiber laser systems. Many devices are now also offered in 3-port configurations. In addition to our standard line of Fiber-Q® modulators, we customize, design, and manufacture in volume for OEM needs. Our technical support team works with customers to identify the best RF driver for the application, taking into consideration the type of modulation required (digital or analog) as well as any specific pulse shaping needs.
Applications Biomedicine, industrial laser, sensing, scientific research, telecommunication.
Winner of the prestigious Queen’s Award for Enterprise: Innovation, and Institute of Physics Innovation Award.
Insertion Loss Distribution
Extinction Ratio Distribution
Fiber-Q® (1060 nm - 150 MHz)
Fiber-Q® (1060 nm - 150 MHz) 300
400 350
250 200
Number
Number
300
150
250 200 150
100
2
More
1.7
1.9
1.8
1.5
1.6
1.3
1.4
1
1.1
1.2
0.9
0.7
0.8
0.5
0.4
80
More
76
78
72
74
70
66
68
62
64
60
56
58
52
54
50
0 50
50
0.6
100
Insertion loss [dB]
Extinction ratio [dB]
Voltage Standing Wave Ratio Distribution
Frequency Dependence Distribution
Fiber-Q® (1060 nm - 150 MHz)
Fiber-Q® (1550 nm - 80 MHz)
120
5 4.5
Insertion loss [dB]
Number
100 80 60 40
4 3.5 3 2.5 2 1.5 1
20
0.5 0
Voltage standing wave ratio
20
1.3
More
1.26
1.28
1.24
1.2
1.22
1.16
1.18
1.14
1.1
1.12
1.06
1.08
1.04
1
1.02
70
72
74
76
78
80
82
84
86
88
90
Radio frequency [MHz]
GOOCH & HOUSEGO
NEW
ACOUSTO-OPTICS
1
PRODUCT CODE1
WAVELENGTH
FIBER
RISE/FALL TIME
OPERATING FREQUENCY
PACKAGE
TBC
400 nm
SM/PM
<25 ns
200 MHz
TBC
S-M200-0.4C2A-3-F2S
450 nm
SM
25 ns
200 MHz
Non-hermetic
S-M200-0.4C2A-3-F2P
450 nm
PM
25 ns
200 MHz
Non-hermetic
S-M200-0.4C2C-3-F2S
532 nm
SM
25 ns
200 MHz
Non-hermetic
S-M200-0.4C2C-3-F2P
532 nm
PM
25 ns
200 MHz
Non-hermetic
S-M200-0.4C2E-3-F2S
633 nm
SM
25 ns
200 MHz
Non-hermetic
S-M200-0.4C2E-3-F2P
633 nm
PM
25 ns
200 MHz
Non-hermetic
T-M150-0.5C2W-3-F2S
780 nm
SM
50 ns
200 MHz
Hermetic
T-M150-0.5C2W-3-F2P
780 nm
PM
50 ns
200 MHz
Hermetic
T-M300-0.1C2G-3-F2S
1060 nm
SM
6 ns
300 MHz
Hermetic
T-M300-0.1C2G-3-F2P
1060 nm
PM
6 ns
300 MHz
Hermetic
T-M200-0.1C2G-3-F2S
1060 nm
SM
10 ns
200 MHz
Hermetic
T-M200-0.1C2G-3-F2P
1060 nm
PM
10 ns
200 MHz
Hermetic
T-M150-0.4C2G-3-F2S
1060 nm
SM
30 ns
150 MHz
Hermetic
T-M150-0.4C2G-3-F2P
1060 nm
PM
30 ns
150 MHz
Hermetic
S-M150-0.4C2G-3-F2S
1060 nm
SM
30 ns
150 MHz
Non-hermetic
T-M300-0.1C16J-3-F2P
1550 nm
PM
6 ns
300 MHz
Hermetic
T-M200-0.1C2J-3-F2S
1550 nm
SM
10 ns
200 MHz
Hermetic
T-M200-0.1C2J-3-F2P
1550 nm
PM
10 ns
200 MHz
Hermetic
T-M110-0.2C2J-3-F2S
1550 nm
SM
25 ns
110 MHz
Hermetic
T-M110-0.2C2J-3-F2P
1550 nm
PM
25 ns
110 MHz
Hermetic
T-M080-0.4C2J-3-F2S
1550 nm
SM
35 ns
80 MHz
Hermetic
T-M080-0.4C2J-3-F2P
1550 nm
PM
35 ns
80 MHz
Hermetic
T-M080-0.5C8J-3-F2S
1550 nm
SM
100 ns
80 MHz
Hermetic, low power consumption
T-M080-0.5C8J-3-F2P
1550 nm
PM
100 ns
80 MHz
Hermetic, low power consumption
T-M040-0.5C8J-3-F2S
1550 nm
SM
100 ns
40 MHz
Hermetic, low power consumption
T-M040-0.5C8J-3-F2P
1550 nm
PM
100 ns
40 MHz
Hermetic, low power consumption
T-M250-0.3C16Z-3-F2P
2000 nm
PM
15 ns
250 MHz
Hermetic
T-M080-0.3C2Z-3-F2S
2000 nm
SM
100 ns
80 MHz
Hermetic
T-M080-0.3C2Z-3-F2P
2000 nm
PM
100 ns
80 MHz
Hermetic
Most devices available in 3-port configuration. Custom devices and fiber connectors available upon request.
GOOCH & HOUSEGO
21
ACOUSTO-OPTICS
MULTI-CHANNEL MODULATORS Independent control of multiple beams or a sheet of collimated light Acousto-optic multi-channel modulators (AOMC) allow multiple beams to be modulated or deflected independently by integrating an array of transducers with a single acousto-optic crystal. Our proprietary optical and electrical designs minimize crosstalk, allowing concurrent operation of up to 48 channels for modulation and up to eight channels for beam deflection. Our AOMCs are known for their reliable operation and high performance. Multi-channel modulators have parallel beams as input, each beam independently controlled by a different transducer to modulate its intensity. Multi-channel modulators are most often used for high speed applications like micromachining and direct-write lithography, as each beam can be modulated independently. These devices can also be used to increase throughput when writing large media by writing multiple beams at the same time. Our multi-channel modulators equal the performance available with our single channel modulators, and can be customized for large aperture applications as well as high speed, small aperture applications. A multi-channel beam deflector however, generates multiple diffracted beams from a single input beam at specific locations by simultaneously applying multiple frequencies to a single transducer. Each individual channel is a deflector that can either scan the beam or produce multiple spots. This makes it possible to create a two-dimensional grid. For example, if a four channel beam deflector were configured so that each channel diffracted three spots, the result would be a 4x3 grid. High laser damage threshold is achieved using low-scatter materials. These are inspected to rigorous quality standards. We grow our own tellurium dioxide and source high quality fused silica and crystalline quartz to ensure low insertion loss and excellent optical power handling. Applications Marking, material processing, micromachining, printing.
G&H engineers apply their knowledge to design custom products for our customers, to meet their unique needs. The table below shows a range of typical AOMC product specifications. PRODUCT CODE
WAVELENGTH
NUMBER OF CHANNELS
RISE/FALL TIME
ACTIVE APERTURE
OPERATING FREQUENCY
OPTICAL MATERIAL
AOMC 220-4
350-365 nm
4
16 ns
0.24 mm
190-250 MHz
Crystalline quartz
AOMC 125/24-3
350-365 nm
24
23 ns
0.5 mm
125 MHz
Crystalline quartz
AOMC 3160-8
364 nm
8
21 ns
0.18 mm
160 MHz
Fused silica
AOMC 300-5
413 nm
5
10 ns
0.2 mm
300 MHz
Crystalline quartz
AOMC 220-5
413 nm
5
16 ns
0.24 mm
220 MHz
Crystalline quartz
AOMC 3350-6
350-850 nm
6
30 ns
0.33 mm
350 MHz
Tellurium dioxide
22
GOOCH & HOUSEGO
ACOUSTO-OPTICS
PULSE PICKERS/CAVITY DUMPERS Rapid, synchronized pulse selection; internal or external to the laser cavity Pulse pickers and cavity dumpers are high speed acousto-optic modulators which separate and divert a single laser pulse within a pulse train to a new optical path. A cavity dumper is used inside the cavity of a mode locked laser, while a pulse picker describes the same function when used externally. Both use a high speed acousto-optic crystal and specialized design techniques to keep rise time to a minimum while operating at a low duty cycle to select individual laser pulses with speed and synchronization. Tight focusing of the beam within the device is required to achieve the desired speed (typically <0.1 mm), resulting in very high input power density. Our rigorous manufacturing standards and high crystal quality minimize scatter and enable industry-leading optical power handling. Antireflection (AR) coatings minimize insertion loss. By using a high RF carrier frequency and an optimized lens design, G&H pulse pickers and cavity dumpers provide large angular separation between the deflected and undeflected beams (up to 75 mrad). This makes it easy to separate the two beams in space and maintain a static contrast ratio of at least 500:1. The choice of RF driver is particularly important to achieve accurate synchronization with the laser pulse train. Controls on the driver optimize the RF drive pulse shape and delay. The modulation signal is synchronized and optimized using a control loop to select the best time at which to pick off the pulse. Applications Generation of high energy pulses, injection and extraction of pulses from regenerative amplifiers, femtosecond/picosecond lasers, reduction of pulse repetition rates.
G&H engineers apply their knowledge to design custom products for our customers, to meet their unique needs. The table below shows a range of typical pulse pickers and cavity dumpers product specifications. PRODUCT CODE
WAVELENGTH
RISE/FALL TIME
ACTIVE APERTURE
OPERATING FREQUENCY
OPTICAL MATERIAL
13389-BR AOCD/AOPP
350-850 nm
6 ns
60 µm
389 MHz
Fused silica
17389-.93-FOA AOPP
700-1064 nm
7 ns
70 µm
389 MHz
Tellurium dioxide
I-M080-2C10G-4-AM3
1030-1064 nm
113 ns/mm
2 mm
80 MHz
Crystalline quartz
I-M080-4C10G-4-GH60
1030-1064 nm
113 ns/mm
4 mm
80 MHz
Crystalline quartz
I-M150-0.5C10G-8-GH48
1064 nm
30 ns
0.5 mm
150 MHz
Crystalline quartz
I-M110-1C10G-8-GH48
1064 nm
60 ns
1 mm
110 MHz
Crystalline quartz
GOOCH & HOUSEGO
23
ACOUSTO-OPTICS
Q-SWITCHES High power and low loss for lowering the cavity Q-factor and holding off lasing An acousto-optic Q‑switch (AOQS) works within a laser cavity to generate high intensity, short-pulse light by actively controlling the Q‑factor (loss) of the cavity. Our products are rugged, reliable, and long-lasting, backed by millions of hours of service in the field. We offer low insertion loss, highly efficient Q‑switches capable of handling very high peak power. We have off-the-shelf solutions for polarized or unpolarized lasers, and can accommodate large lamp-pumped multi-mode laser beam diameters as well as small, compact diode-pumped beam diameters. Specialized designs meet unique needs such as ultra-high single pass loss (up to 96%), high switching speeds, and premium pulse-to-pulse stability. Most AO Q-switch products utilize materials with high optical power handling such as fused silica or crystal quartz. In order to maintain high efficiency (i.e. loss modulation) with these materials, higher RF powers are necessary and therefore require adequate conduction or water cooling. All of our Q-switch products offer very low loss in the “off” state to maximize output intensity, and excellent transducer reliability to allow long-term use without maintenance. We also offer a full line of RF drivers designed specifically for Q‑switching, with rapid fall times, tight synchronization, operation in either fixed or variable mode, and advanced capabilities like first pulse suppression or multi-channel operation to drive multiple Q‑switches within the same cavity.
Applications Laser marking, lithography, material processing, medical surgery, micromachining.
The products listed below illustrate a range of typical G&H AOQS specifications. Products can be customized to meet the demands of specific applications.
PRODUCT CODE
WAVELENGTH
ACTIVE APERTURE
OPERATING FREQUENCY
OPTICAL MATERIAL
COOLING
I-QS080-1C10G-8-GH28
1030-1064 nm
1 mm
80 MHz
Crystalline quartz
Conduction-cooled
I-QS080-1C10G-4-OS13
1030-1064 nm
1 mm
80 MHz
Crystalline quartz
Conduction-cooled
I-QS080-1.2C10G-4-GH64
1030-1064 nm
1.2 mm
80 MHz
Crystalline quartz
Conduction-cooled
I-QS080-0.5C10G-8-GH48
1064 nm
0.5 mm
80 MHz
Crystalline quartz
Conduction-cooled
I-QS041-1.8C10G-4-GH21
1064 nm
1.8 mm
40.68 MHz
Crystalline quartz
Conduction-cooled
I-QS041-2.1C5G-4-GH88
1064 nm
2.1 mm
40.68 MHz
SF10 flint glass
Conduction-cooled
Industry Standard Q-Switch
1064 nm
1.6, 2, 3, 4, 5, 6.5, 8 mm
24, 27.12, 40.68, 68 MHz
Fused silica
Water-cooled
Stallion Q-Switch
1064 nm
1.6, 2, 3, 4, 5, 6.5, 8 mm
24, 27.12, 40.68, 68 MHz
Fused silica
Water-cooled
Super Q-Switch
1064 nm
1.6, 2, 3, 4, 5, 6.5 mm
24, 27.12 MHz
Crystalline quartz
Water-cooled
VHE Q-Switch
1064 nm
1.6, 2.5, 2, 3, 4 mm
68 MHz
Crystalline quartz
Water-cooled
I-QS080-1C10H-4-OS14
1319-1342 nm
1 mm
80 MHz
Crystalline quartz
Conduction-cooled
I-QS041-1.5C10V23-4-HC1
1535 nm
1.5 mm
40.68 MHz
Crystalline quartz
Conduction-cooled
I-QS080-1C10J-8-GH28
1550 nm
1 mm
80 MHz
Crystalline quartz
Conduction-cooled
I-QS041-1.8C10R3-8-SO7
1800-2200 nm
1.8 mm
40.68 MHz
Crystalline quartz
Conduction-cooled
I-QS027-4C10R3-U5-IS6
1800-2200 nm
4 mm
27.12 MHz
Crystalline quartz
Water-cooled
I-QS041-2C10V5-4-HC1
1900-2100 nm
2 mm
40.68 MHz
Crystalline quartz
Conduction-cooled
I-QS027-3C10V5-U5-ST3
1900-2100 nm
3 mm
27.12 MHz
Crystalline quartz
Water-cooled
I-QS041-3C2P-4-SO11
2800-3000 nm
3 mm
40.68 MHz
Tellurium dioxide
Conduction-cooled
24
GOOCH & HOUSEGO
ACOUSTO-OPTICS
TUNABLE FILTERS Precise, rapid wavelength selection and tuning An acousto-optic tunable filter (AOTF) is a solid-state, electronically-addressable random-access optical passband filter. It may be used to rapidly and dynamically select a specific wavelength from a broadband or multi-line source. When specific matching conditions between the acoustic and optical beams are met, diffraction will occur. As a result it is possible to electronically control key filter parameters such as wavelength, modulation-depth and even bandwidth, thus providing rapid (typically µs), dynamic, random access optical filtering. Resolution bandwidths down to <0.1% are available with exceptional performance and with aperture sizes up to 25 mm and beyond. We have developed and patented techniques to allow us to offer options such as large-aperture imaging filtering, sideband suppression, and transmission of multiple discrete wavelengths. G&H AOTFs are based on our in-house grown high quality tellurium dioxide polished and fabricated to rigorous standards.
80
Drive frequency [MHz]
We offer a range of AOTFs to suit a variety of applications. For scanning an entire image in wavelength at speeds sufficient for real-time video rate spectral imaging, high optical throughput is required. For this purpose devices with large aperture and/ or field of view are recommended. When narrow resolution is required and the light source is well collimated, a “quasi-collinear” AOTF may be more appropriate.
Tuning Relation TF1875-1250-10-6-GH59A
75 70 65 60 55 50 45 40 1200
1400
1600
1800
2000
2200
2400
2200
2400
Selected wavelength [nm]
For best performance, we recommend a matched RF driver, including the latest digital frequency synthesizer (DFS) driver technology and random access wavelength control.
Resolution TF1875-1250-10-6-GH59A 18
Confocal microscopy, fluorescence imaging, hyperspectral imaging, imaging spectroscopy, laser wavelength tuning, on-line process control, spectroscopy, wavelength selection.
FWHM line width [nm]
16
Applications
14 12 10 8 6 4 1200
1400
1600
1800
2000
Selected wavelength [nm]
The table below and on the following page shows a range of typical AOTF product specifications. G&H engineers apply their knowledge to design custom products for our customers, to meet their unique needs. Fiber-coupled AOTF devices are available upon request. PRODUCT CODE
WAVELENGTH
ACTIVE APERTURE
RESOLUTION
AOTF 2837-31
351-430 nm
2.5 mm
1.0 nm
AOTF 3151-01
400-650nm
2.5 mm
2.5 nm
TF525-250-6-3-GH19A
400-650 nm
3 mm
5 nm
TF550-300-4-6-GH57A
400-700 nm
6 mm
4 nm
TF560-280-1-5-NT2
420-700 nm
5 mm
0.3 nm
AOTF 2838-01
450-670 nm
2.5 mm
1.3 nm
AOTF 2885-02
450-670 nm
2.5 mm
2 nm
AOTF 2885-04
450-670 nm
2.5 mm
4 nm
GOOCH & HOUSEGO
25
ACOUSTO-OPTICS
WAVELENGTH
ACTIVE APERTURE
RESOLUTION
Tuning Relation TF950-500-1-5-NT2 65
TF625-350-2-11-BR1A
450-800 nm
11 mm
1.5 nm
TF850-500-1-3-PF3
600-1100 nm
3 mm
1.5 nm
TF850-500-10-6-GH58A
600-1100 nm
6 mm
10 nm
AOTF 2986-01
640-1100 nm
2.5 mm
5 nm
TF925-550-10-3-GH29A
650-1200 nm
3 mm
9 nm
TF950-500-1-2-GH96
700-1200 nm
2 mm
0.6 nm
TF950-500-0.2-3-GH108
700-1200 nm
3 mm
0.2 nm
TF950-500-1-5-NT2
700-1200 nm
5 mm
0.8 nm
TF1300-800-16-11-NO1A
900-1700 nm
11 mm
16 nm
TF2270-2560-5-5-GH65
990-3550 nm
5 mm
5 nm
AOTF 2996-01
1100-2000 nm
2.5 mm
12 nm
TF1650-1100-1-3-GH107
1100-2200 nm
3 mm
1.0 nm
TF1650-1100-2-3-GH40
1100-2200 nm
3 mm
1.6 nm
TF1650-1100-9-3-GH30A
1100-2200 nm
3 mm
8 nm
TF1875-1250-10-6-GH59A
1250-2500 nm
6 mm
10 nm
TF1900-1100-6-11-GH54A
1300-2500 nm
11 mm
6 nm
TF1900-1100-6-25-GH87A
1350-2450 nm
25 mm
6 nm
TF2000-1000-2-6-GH78
1500-2500 nm
6 mm
1.2 nm
TF2250-1500-12-7-GH61A
1500-3000 nm
7 mm
12 nm
TF2900-2200-5-3-GH40
1800-4000 nm
3 mm
5 nm
TF3000-2000-3-7-GH78
2000-4000 nm
7 mm
2.6 nm
TF3300-2200-xxx
2200-4400 nm
Up to 15 mm
~20 mm
Drive frequency [MHz]
PRODUCT CODE
60 55 50 45 40 35 700
800
900
1000
1100
1200
1100
1200
Selected wavelength [nm]
Resolution TF950-500-1-5-NT2 1.2
FWHM line width
1.1 1 0.9 0.8 0.7 0.6 0.5 0.4 700
26
800
900
1000
Selected wavelength [nm]
GOOCH & HOUSEGO
ACOUSTO-OPTICS
RF DRIVERS Stable, versatile electronic control options for acousto-optic devices An RF driver generates the fixed or variable frequency signal supplied to a device to induce the acousto-optic effect. The frequency and intensity of the applied signal will determine how much an optical beam is modulated, deflected, or tuned. An acousto-optic device and its RF driver should be selected as a unit to optimize speed and stability for each application. G&H offers a wide variety of stable high frequency drivers with analog and digital modulation capability, optimized by application with features such as first pulse suppression, synchronization, pulse shaping, and multi-channel operation. As our AO product lines expand, we are creating more flexible, adaptive drivers with dual analog/digital operation and configurable firmware to accommodate functionality like triggering and temperature control without the need for new hardware. Our OEM designs, in contrast, are optimized to each customer’s application, maximizing performance in the required form factor.
CHOOSING AN RF DRIVER The needs of the AO device dictate the choice of RF driver. Primary factors to consider are shown below, though speed, duty cycle, and special functions are also important. • • • • • •
RF power: ranges from <0.1 W to >150 W Modulation: digital or analog Frequency of operation: may be fixed, variable (linearly swept), or programmable Stability: influencing choice of VCO vs. DDS when frequency is not fixed Number of channels: number of output ports or output tones from a single port Special functions: pulse-killing, synchronization, etc.
Applications Driving and controlling acoustooptic devices: beam deflectors, cavity dumpers, frequency shifters, mode lockers, modulators (fibercoupled and free space), multichannel modulators, pulse pickers, Q-switches, tunable filters.
Modulation: Digital vs. Analog The modulation mode determines how the applied RF power is varied, and thus the intensity of diffracted light. In digital modulation, the RF power is applied in an on/ off state via an applied TTL signal, thus controlling whether the beam is diffracted. In analog modulation, the RF power is controlled through application of a voltage within a specified range, yielding control over the diffraction efficiency and allowing shaping of that waveform in time. Fixed vs. Variable Frequency Drivers Fixed frequency drivers provide a single output frequency which is matched to the AO device. Offered from 24-440 MHz, fixed frequency drivers may be controlled via analog or TTL input, some with manually adjustable output RF power. These are used most often for modulation applications. Variable and programmable frequency RF drivers allow active control of output frequency. Voltage controlled oscillators (VCOs) provide a linearly swept (variable) RF drive frequency, and are flexible enough to be used for any AO device. Direct digital synthesizer (DDS) drivers offer programmable frequency. They can create random waveforms from a single, fixed-frequency reference clock, and thus are ideal for pulse shaping and special functions. DDS drivers are software driven, and can be run from a user-friendly interface (a GUI), or controlled directly via computer driver commands. Our high-performance multi-frequency DDS drivers generate up to eight channels of RF frequencies simultaneously. Smart Drivers Smart drivers allow simple or complex digital waveforms to be synthesized, converted to analog signals, and amplified to drive the AO device. This gives great flexibility; for example, allowing the driver to provide multiple programmable frequencies or to swap freely between multiple, complex, customized waveforms. GOOCH & HOUSEGO
27
ACOUSTO-OPTICS
Frequency Agility and Control We manufacture Direct Digital Synthesizer (DDS) drivers that offer high stability and linearity, with fast switching time and high resolution. They are capable of creating arbitrary waveforms from a single, fixed-frequency reference clock, and thus are ideal for pulse shaping and special functions. DDS drivers can be run from a GUI or via driver commands in two modes: 1) random access, with digital words mapping to specific frequencies, and 2) chirped mode for continuous scanning in frequency increments. DDS drivers are also referred to as DFS (digital frequency synthesizer) drivers.
The products listed below illustrate a range of typical G&H AO device driver specifications. Our technical support team is available to advise on selection and optimization of RF drivers for specific applications, as well as customization of products for OEM integration.
PRODUCT CODE
COMPATIBLE AO DEVICES
OPERATING FREQUENCY
RF POWER
OPERATION MODE
KEY FEATURES
Smart Dual Driver
Beam deflector, tunable filter
50-450 MHz
15-20 W
Smart
2 channel; flexible functionality; phase synchronized outputs
64020-250-1ADMDFS-A
Beam deflector, special modulator, tunable filter
20-250 MHz
1.0 W
Programmable frequency
Single channel DDS
64020-200-2ADMDFS-A
Beam deflector, special modulator, tunable filter
20-200 MHz
2.0 W
Programmable frequency
Single channel DDS
97-02925-32
Beam deflector, tunable filter
20-160 MHz
0.4 W
Programmable frequency
Single channel DDS
97-03926-12
Beam deflector, tunable filter
20-160 MHz
3.2 W
Programmable frequency
8 channel DDS
97-02910-xx
Fiber-Q®
80, 150, 200 MHz
2.5-3.0 W
Fixed single frequency
Low power draw
SD020-200-5UC-4x1
Tunable filter
20-200 MHz
5.0 W
Programmable frequency
Single or multi-channel DDS
A35xxx-S-1/50-p4k7u
Fiber-Q®, modulator, frequency shifter
40, 80, 110, 150, 200, 300 MHz
0.5-5.0 W
Fixed single frequency
Analog & digital modulation
MHPXXX-YYADM-A1
Fiber-Q®, modulator
24-260 MHz
2-20 W
Fixed single frequency
3910 series
Fiber-Q®, modulator, frequency shifter
80-350 MHz
0.5-8.0 W
Fixed single frequency
MCX0XX-Y.YZC-MINx
Modulator, frequency shifter
40-80 MHz
0.5-2.5 W
Fixed single frequency
Ultra-compact size
HP041-125ADG-A10
Modulator
40.68 MHz
125 W
Fixed single frequency
Ge AO devices
HP040-060-150ADGA10-2X
Modulator
40/60 MHz
2x75 W
Fixed dual frequencies
Dual channel Ge AO devices
MQH0XX-YYDM-ZZZ
Q-switch, modulator
24, 27.12, 40.68, 68, 80 MHz
25-100 W
Fixed single frequency
Fixed/variable pulse width
MQH0XX-YYDM-ZZZ-2S
Q-switch
24, 27.12, 40.68, 68, 80 MHz
25-50 W per channel
Fixed single frequency
2 channel; fixed/variable pulse width
QC0XX-YYDC-ZZZ-AAV
Q-switch, modulator
24, 27.12, 40.68, 68, 80, 110 MHz
2-24 W
Fixed single frequency
Compact, low power; fixed/ variable pulse width
28
GOOCH & HOUSEGO
CO CRYSTAL OPTICS Gooch & Housego is a pioneer in crystal growth techniques and a supplier of special crystalline materials for use in high power applications. Many of our precision optic components are manufactured from our own in-house grown crystals, including achromats, harmonic generating optics, prisms, and waveplates.
Capabilities
30
Products Lithium Niobate Wafers
31
Crystals and Nonlinear Optics
32
Periodically-Poled Lithium Niobate
33
GOOCH & HOUSEGO
29
CRYSTAL OPTICS
TECHNICAL EXPERTISE AND MANUFACTURING CAPABILITIES G&H’s crystal growth capabilities extend over a significant number of materials; our crystals comprise the basis for many of our own products. Our experience growing lithium niobate (LiNbO3) dates back to 1967, when we produced the first commercially available material. Since that time we have constantly refined the growth and material processing to be able to produce the highest quality LiNbO3, providing the most consistent performance of acousto-optic and electro-optic devices such as modulators, Q-switches, Pockels cells. We also offer LiNbO3 as wafers, AR coated Pockels cell crystals with electrodes, and as periodically poled (PPLN) harmonic generators. Beginning with the raw chemicals, we grow, orient, fabricate, finish, coat, and mount ß-barium borate (BBO), cadmium sulfide (CdS), cadmium selenide (CdSe), potassium dihydrogen phosphate (KDP), and potassium dideuterium phosphate (KD*P) crystals in housings with apertures from 3 mm to larger than 300 mm. Additionally, we grow tellurium dioxide (TeO2) for our acousto-optic devices.
Laser manufacturers rely on us to provide the highest quality crystal optical components manufactured to specification. They benefit from our expertise with design recommendations to arrive at technically advanced, innovative, and cost effective solutions to meet the demanding requirements of modern laser systems and optical instrumentation. G&H customers include manufacturers and research laboratories that require the highest quality components for cutting edge applications. Large KDP and KD*P crystal plates grown, cut, and finished by G&H are in use at National Ignition Facility (NIF) and the Commissariat à l'énergie atomique et aux énergies alternatives (CEA).
Proprietary crystal growth optimization software enables us to supply custom crystal solutions for your project. We routinely produce crystals as large as 0.4x0.4 m for internal confinement fusion (ICF) applications, as well as crystals as small as a few mm in cross-section for microchip laser applications.
30
GOOCH & HOUSEGO
CRYSTAL OPTICS
LITHIUM NIOBATE WAFERS High quality congruent and MgO doped wafers Lithium niobate (LiNbO3 or LN) is used in electro-optics, acousto-optics, nonlinear optics and guided-wave optics due to its attractive fundamental properties. These properties include wide transparency range, high electro-optic and nonlinear optic coefficients, very high electro-mechanical coupling coefficients, and chemical and mechanical stability. G&H offers X-axis and Z-axis orientation LN in congruent and 5.0 mol% magnesium doped compositions. We have refined our proprietary techniques for growth and processing to produce consistently high quality LN for one-off scientific and volume OEM applications.
Applications Isolators, low pass filters, ophthalmic surgery systems, use in Pockels cells, Q-switching, range-finders, target designators, waveguides, Wollaston prisms.
We provide congruent lithium niobate wafers for infrared light applications, and magnesium-doped periodically-poled LN (MgO:PPLN) for improved resistance to photorefractive damage at visible wavelengths. Our optical wafers undergo many stages of precision processing to ensure the highest quality is provided to the customer. Poling of the lithium niobate boules grown in-house aligns the ferroelectric domains along a single axis, after which the boule is shaped; slices are cut to within 6 minutes of the x- or z-axis with the assistance of X-ray orientation. A curved radius is ground on the outside edge of the wafer to reduce cracking and chipping, followed by lapping and chemical etching. Polishing of one or both sides brings the finish to within Ra <0.2 nm, and to a front surface quality of 10-5. We perform 100% visual inspection on finished wafers, and characterize stress and strain prior to packaging in a cleanroom environment.
PRODUCT CODE
DIAMETER
THICKNESS
ORIENTATION
SIDE 1
SIDE 2
OPTICAL MATERIAL
97-01514-10
100 mm
1.00 mm
Z-axis
10-5
20-10
LN
97-01763-01
100 mm
1.00 mm
X-axis
10-5
60-30
LN
97-01912-01
100 mm
1.00 mm
X-axis
10-5
Ground
LN
97-02641-01
125 mm
1.00 mm
Z-axis
10-5
60-30
LN
97-02604-01
125 mm
1.00 mm
X-axis
10-5
60-30
LN
97-03044-02
76.2 mm
1.00 mm
Z-axis
10-5
20-10
MgO:LN
97-03044-01
76.2 mm
0.51 mm
Z-axis
10-5
20-10
MgO:LN
97-00567-01
76.2 mm
1.00 mm
Z-axis
10-5
Ground
LN
97-00567-03
76.2 mm
0.51 mm
Z-axis
10-5
Ground
LN
97-00663-01
76.2 mm
1.00 mm
X-axis
Polished
Ground
LN
99-00629-01
76.2 mm
0.50 mm
X-axis
Polished
Polished
LN
99-00630-01
76.2 mm
1.00 mm
X-axis
Polished
Polished
LN
97-01183-01
76.2 mm
0.50 mm
X-axis
10-5
Ground
LN
99-00042-01
76.2 mm
0.51 mm
Z-axis
10-5
60-30
LN
99-60011-01
76.2 mm
1.00 mm
Z-axis
10-5
60-30
LN
GOOCH & HOUSEGO
31
CRYSTAL OPTICS
CRYSTALS AND NONLINEAR OPTICS Crystals for polarization and frequency conversion, from DUV to FIR Nonlinear optic (NLO) crystals are used for polarization control and frequency conversion applications. We offer a wide selection of crystals for use from the deep ultraviolet (DUV) to the far infrared (FIR). All are fabricated on a made-to-order basis in-house using advanced orienting, sawing, grinding, and lapping technologies. From one-off to volume OEM applications, we supply bespoke crystals for research and industry use. We offer ß-barium borate (BBO) for use in for Pockels cells and harmonic generators, cadmium selenide (CdSe) for infrared waveplates and MIR harmonic generation, and cadmium sulfide (CdS) for infrared waveplates. Our potassium dihydrogen phosphate (KDP) and potassium dideuterium phosphate (KD*P) crystals are used in harmonic generators, electro-optical Q-switches (Pockels cells), and waveplates, while LiNbO3 and TeO2 are used in acousto-optic devices. LiNbO3 is also used to produce waveguides, low pass filters, isolators, and Wollaston prisms. Proprietary software routines and unique crystal growth capabilities enable us to supply customized crystals for a variety of applications. G&H provides KDP boules with masses greater than 635 kg, crystals with cross sections as large as 43 cm square for inertial confinement fusion (ICF) applications, and large single crystal CdS and CdSe crystals for IR waveplates.
Applications Nonlinear optics are used to create beam deflectors, harmonic generators, IR waveplates, isolators, low pass filters, modulators, Pockels cells, pulse pickers, Q-switches, waveguides, windows, Wollaston prisms.
Precision polishing techniques achieve large diameter or high aspect ratio optics with excellent transmitted wavefront characteristics. We offer special geometrical shapes with aspect ratios better than 100:1 including large diameter thin plates and smaller diameter plates as thin as 400 µm. Brewster-cut bars are also available for low-loss intra-cavity laser applications. Vapor deposition and IBS coating systems provide antireflective (AR) coatings as needed. We have developed our own proprietary solgel process to provide high laser-damage threshold AR coatings for laser systems requiring high transmission and broadband performance for crystal diameters ranging in size from 5 mm to over 300 mm. Vacuum deposition processes can be used to apply metal electrodes to flat polished or fine-lapped surfaces as well as cylindrical surfaces. Our line of crystal holders accommodate a wide range of crystal sizes and apertures. Designed to minimize mechanical stress and strain, our standard and custom fixtures and housings are supported by our own machine shop, providing tight tolerance and high quality manufacturing. In-house metrology capabilities range from transmission and reflection interferometry to measurement of contrast ratio, insertion loss, uniformity of birefringence, and other important crystal characteristics. Our product managers and sales engineers routinely work with customers, applying our expertise to develop custom products to meet the demands of specific applications. CRYSTAL HOLDER TYPE
OUTER DIAMETER
APERTURE
HOUSING THICKNESS
XH Series
25.3 mm
5x5, 6x8, 8x8, 10x10 mm
22.2, 24.7, 27.2 mm
XC Series
25.3 mm
4, 6, 8, 10, 13 mm
6.35 mm
XCL Series
25.3 mm
4, 6, 8, 10, 13 mm
12.7 mm
XTP Series
50.67-356 mm
30-322 mm
Varies
32
GOOCH & HOUSEGO
CRYSTAL OPTICS
PERIODICALLY-POLED LITHIUM NIOBATE High efficiency quasi phase-matching for OPO, SHG and DFG applications Periodically-poled lithium niobate (PPLN) nonlinear crystals are efficient wavelength converters from the visible region to 5 µm. By using lithography to define the poling pattern, it can easily be customized to a wide range of applications. Phase-matching over very long propagation lengths at infrared wavelengths is possible with our congruently grown undoped PPLN manufactured from highly uniform Z-axis wafers. Visible wavelengths are better served by magnesium-doped PPLN (MgO:PPLN), as the 5 mol% doping prevents photorefractive damage. Average powers of up to 1 W can be produced at 532 nm in our MgO:PPLN crystals without causing beam distortion. To achieve optimal conversion efficiency, the interacting waves need to be phasematched by choosing the proper poling period. Typical periods range from about 7 µm for second harmonic generation (SHG) producing 532 nm to around 30 µm for optical parametric oscillators (OPOs) pumped by Nd:YAG lasers. The poling is done in wafer form before the chip is cut and polished, allowing the configuration to be specifically tailored to each application. We can design fan-out gratings to allow continuous tuning as beam position is moved across the aperture, chips up to 80 mm in length to allow for maximum gain, and chips up to 40 mm in width to achieve fine tuning of the signal wavelength.
Applications Chemical fingerprinting, compact laser displays, countermeasures, difference frequency generation (DFG), laser cooling, laser display, microscopy, range-finding, second harmonic generation (SHG), sensing, target illumination, telecommunications, wavelength conversion.
Patterns with multiple gratings along the beam direction enable multiple nonlinear interactions in the same crystal. This can be used to increase the quantum efficiency of OPOs or to generate various different wavelengths at once. Chirped gratings are used to widen the wavelength acceptance or to compensate for group velocity walkoff in ultra-short pulses.
1
PRODUCT CODE
WAVELENGTH1
ACTIVE APERTURE
OPTICAL MATERIAL
PERIOD
AR COATING
LENGTH
97-03038-xx
0.532 µm
0.75x0.5 mm
MgO:PPLN
6.9-6.96 µm
Yes
1, 3, 10 mm
97-03040-xx
0.532 µm
0.75x0.5 mm
MgO:PPLN
6.9-6.96 µm
No
1, 3, 10 mm
97-02384-xx
1.3-1.6 µm
1.3x1 mm
PPLN
25.5-28.7 µm
No
19, 50 mm
97-02383-xx
1.6-2.1 µm
1.3x1 mm
PPLN
30.0-31.2 µm
No
19, 50 mm
97-03224-01
0.755 µm (1.55 µm pump)
10x1 mm
MgO:PPLN
19.25 µm
Yes
20 mm
97-03196-xx
1.45-1.55 µm
10x1 mm
MgO:PPLN
28.8-30.15 µm fan
Yes
20, 50 mm
97-03197-xx
1.55-2.128 µm
10x1 mm
MgO:PPLN
30.6-32.0 µm fan
Yes
20, 50 mm
Assumes a 1064 nm pump laser unless otherwise stated Signal Tuning in PPLN OPO 2.1
31.2 µm
Signal wavelength [µm]
31.1 µm
2.0
30.95 µm 30.8 µm
1.9
30.6 µm 30.4 µm 30.2 µm
1.8
30 µm
1.7 1.6 1.5 50
60
70
80
90
100
110
120
130
140
150
160
170
180
190
200
Temperature [°C]
Signal wavelength tuning with temperature for different QPM periods in a 1.064 µm pumped PPLN OPO GOOCH & HOUSEGO
33
EO ELECTRO-OPTICS Gooch & Housego’s electro-optic and crystal growth facility was founded in 1973. We now offer a comprehensive range of electrooptic solutions for a diverse range of applications in the ultraviolet through infrared wavelengths. With over four decades of experience in device design and internal crystal growth capabilities, we are uniquely qualified to support Pockels cell requirements.
Capabilities
34
Products Pockels Cells
35
Pockels Cell Drivers
36
Lithium Niobate Q-Switches
37
GOOCH & HOUSEGO
35
ELECTRO-OPTICS
TECHNICAL EXPERTISE AND MANUFACTURING CAPABILITIES G&H offers an extensive range of electro-optic devices based on potassium dihydrogen phosphate (KDP), potassium dideuterium phosphate (KD*P), ß-barium borate (BBO), and cadmium telluride (CdTe). Utilizing proprietary crystal growth, fabrication, and polishing techniques, we manufacture both longitudinal and transverse electrode configuration Pockels cells with clear aperture diameters ranging from 1.8 to 100 mm. Our unique KDP and KD*P crystal growth, Pockels cell design, and device manufacturing capacity allows us to support the needs of even the most demanding OEM or scientific laser system. The Commissariat à l'énergie atomique et aux énergies alternatives (CEA) and National Ignition Facility (NIF) both selected G&H as their primary supplier of large aperture Pockels cells for optical isolators in the high fluence lasers in their inertial confinement fusion programs. These laser systems are effectively the most powerful in existence and require extraordinarily low absorption KD*P. For high-average power and high repetition rate applications, we provide BBO Pockels cells, the preferred alternative to KD*P. The use of oxide based crystals and water-cooled designs allow for increased average power handling capacity. We offer CdTe devices for operation at longer wavelengths, which benefit from CdTe’s high electro-optic coefficient and non-hygroscopic nature.
36
Antireflective (AR) coating offerings for standard and custom wavelengths include dielectric anti-reflection coatings on fused silica windows for high laser damage threshold applications. High transmission solgel AR coatings on KD*P eliminate the need for index-matching fluid. Q-switches for high power lasers are based on lithium niobate (LiNbO3) grown in-house. LiNbO3 Q-switches provide low loss and high contrast ratio, and are preferred for rugged military and industrial applications.
DRIVERS G&H has also designed a range of Pockels cell drivers for these devices, suitable for incorporation into lasers and laser systems. The Q-Drive Q-switch driver is engineered for performance and durability, and is also available as a compact, packaged benchtop model or unpackaged for OEM integration. The R-Drive is available for regenerative amplifier requirements in an OEM or customizable design.
GOOCH & HOUSEGO
ELECTRO-OPTICS
POCKELS CELLS Reliable Q-switching for high power and repetition rates Based on the Pockels effect, a Pockels cell alters the polarization state of light in an in an electro-optic crystal due to birefringence induced by an applied voltage. An optical switch can be created by adding polarizing elements to perform very rapid Q-switching of a laser. Drawing on proprietary crystal growth and fabrication techniques and decades of experience in electro-optic device design, G&H manufactures high quality longitudinal and transverse electrode configuration Pockels cells in ß-barium (BBO), cadmium telluride (CdTe), potassium dihydrogen phosphate (KDP) and potassium dideuterium phosphate (KD*P). Factors such as wavelength, average power, repetition rate, and aperture size determine the best material and design for each application.
KD*P POCKELS CELLS We offer small and large aperture model KD*P Pockels cells, generally used for applications under 10 kHz repetition rate. The highly popular and compact IMPACT series delivers reliable performance at high contrast ratios for OEM integration, while the CQX series packages the same performance in a larger footprint as a drop-in replacement for the QX series (already widely deployed in the field for decades). Devices in the large aperture TX series are designed for use as optical isolators, protecting beam lines in ultra-high power laser systems.
Section through a Pockels cell, illustrating the Pockels effect
Polarization as Related to Applied Voltage
We recommend BBO Pockels cells for applications over 10 W average power and for repetition rates up to 600 kHz. Our low-loss designs employ transverse electric field geometry with dual crystals to minimize drive voltage, and are not subject to tracking degradation. Custom options include single crystal cells, longer cells requiring 50% less voltage, attenuated cells for applications requiring ultra-low piezoelectric response, and cells with water-cooled apertures for high average power operation.
Voltage in fractions of a wave
BBO POCKELS CELLS 0.5 0.375 0.25 0.125 0 0
0.125
0.25
0.375
0.5
Polarization in fractions of a wave
CADMIUM TELLURIDE POCKELS CELLS
Applications Amplifiers, CO2 lasers, laser fusion, materials processing, medical and aesthetic laser systems, metal annealing, micro-machining, optical switching, petawatt lasers, regenerative amplifiers.
Comparison of Frequency Responses LightGate 4 1.0
Normalized pezoelectric response
Mid-infrared Q-switching applications use CdTe for wavelengths up to 12 µm and repetition rates up to 100 kHz. Our water-cooled designs feature packaging with reduced ambient light sensitivity to allow power handling in excess of 10 W, and are available with application specific anti-reflection (AR) coatings. Optional patentpending designs for environmental protection and high average power are available.
0.8
0.6
0.4
0.2
0.0 0
100
200
300
400
500
600
700
800
900 1000
Frequency [KHz] Standard LG4
Attenuated LG4
PRODUCT SERIES
WAVELENGTH
VOLTAGE CONTRAST RATIO
APERTURE
OPTICAL MATERIAL
PRODUCT CODE
IMPACT Series
300-1300 nm
>2000:1 @1064 nm
8-13 mm
KD*P
IMPACT xx
CQX Series
300-1300 nm
>2000:1 @1064 nm
8-25 mm
KD*P
CQX xx, CQX xx.x
QX Series
300-1300 nm
Varies by model
9.25-19.5 mm
KD*P
QXxxxx
TX Series
300-1300 nm
Varies by model
19.5-99 mm
KD*P
TXxxxx
LightGate Series
300-1600 nm
>1000:1 @1064 nm
2.6-7 mm
BBO
LG x
IRX Series
5-12 µm
>500:1 @10.6 µm
3-7, 4x10 mm
CdTe
IRXx
GOOCH & HOUSEGO
37
ELECTRO-OPTICS
POCKELS CELL DRIVERS Robust, compact packaged drivers for light switching applications The G&H series of Pockels cell drivers complement our full range of available Pockels cells, and are available in several configurations: benchtop drivers, unpackaged, or customized. High quality components are integrated into our short circuit proof designs to maximize lifetime, safety, and reliability, whether operating in commercial, military, or scientific Q-switched laser systems, or in regenerative amplifiers. When selecting a Pockels cell driver, it is important to know the required switching voltage, as it is typically higher for BBO than KD*P, and half-wave operation requires twice the voltage of quarter-wave. Our compact line of drivers achieve high typical switching voltages by applying opposing voltages to each lead (i.e., a high differential voltage). Switching speed and repetition rate also determine choice of driver.
Q-DRIVE FOR Q-SWITCHED LASERS The Q-Drive series offers a fast rise-time for KD*P Pockels cells used in Q-switched lasers with modest repetition rates. It has been designed for high noise immunity and optimum signal integrity, and can be placed close to the Pockels cell to minimize the output pulse rise time. A remote control connector allows convenient single-point access to all driver functions, with remote high voltage (HV) control and signal monitoring.
R-DRIVE FOR REGENERATIVE AMPLIFIERS The compact, cost-effective R-Drive series is designed specifically for use with BBO Pockels cells at quarter wave voltage. Offering both a fast rise and fall time, it allows laser pulses to be injected into or coupled out of an amplifier cavity quickly. Ideal for pulse selection and ultrafast laser regenerative amplifier designs up to 200 kHz, it can be incorporated into new systems or retrofitted as an upgrade to existing designs.
Fall time voltage across cell
OEM CUSTOMIZATION G&H Pockels cell drivers may be customized for each application, from wiring and signal interfaces to cooling by air, water, or conduction/convection. Options for enhanced reliability include complex voltage traces for the Q-Drive to avoid crystal degradation, and custom triggering logic with precisely controlled delays for the R-Drive MOSFETs to prevent damage in operation. All OEM designs are built to the desired form factor and mounting requirements. Applications Q-switching, regenerative amplifiers, laser pulse selection and management.
Typical waveform using EO driver
PRODUCT
RISE/FALL TIME
VOLTAGE OUTPUT
REPETITION RATE
APPLICATIONS
PRODUCT CODE
Benchtop KD*P Pockels Cell Driver
4-7 ns
1.5-4.5 kV
1-4.5 kHz
Laboratory Q-switching
Q-Drive 551
OEM KD*P Pockels Cell Driver
4-7 ns
1.5-4.5 kV
1-4.5 kHz
OEM Q-switching
Q-Drive OEM
R-Drive OEM BBO Pockels Cell Driver
4-7 ns
0-2.5 kV
0-200 kHz
OEM regenerative amplifiers, pulse selection
R-100 OEM
38
GOOCH & HOUSEGO
ELECTRO-OPTICS
LITHIUM NIOBATE Q-SWITCHES Q-switching for rugged military and industrial applications An electro-optic Q-switch can be used to modulate the loss in a laser cavity at GHz switching speeds to generate high intensity, pulsed laser light. Q-switch lithium niobate (LiNbO3 or LN), crystals operate on the Pockels effect, altering the polarization state of light via electrically-induced birefringence. By placing the crystal between a pair of cross-polarizers, light can be passed or blocked at very fast switching speeds. G&H grows and polishes high quality lithium niobate crystals in-house for low wavefront distortion, applying electrodes for use in the transverse mode (i.e., electric field perpendicular to the optic or z-axis). Our LN crystals offer high extinction ratio, very low transmission loss, low switching voltage and temperature stability throughout a wide temperature range. High-performance antireflective (AR) coatings are applied to each face, reducing loss to ≤0.2% per surface while withstanding high optical power (500 MW/cm2 upon request). We have developed proprietary temperature-stable (TS and XTS) versions of our Q-switch products to allow operation over a wide range of temperatures while maintaining excellent contrast ratio. Typical lithium niobate Q-switches suffer from pyro-electric charge buildup at low temperatures, leading to premature lasing if radioactive americium is not used to ionize the air around the crystal and bleed off the charge. We use a proprietary thermo-chemical reduction technique to increase conductivity of our lithium niobate crystal faces, thus dissipating charge and eliminating the premature lasing effect. While this process increases insertion loss slightly, it allows our XTS series to be used in low-temperature environments such as aerospace. Applications Ophthalmic surgery systems, range-finders, target designators.
PRODUCT SERIES
WAVELENGTH
DAMAGE THRESHOLD
SIZE
EXTINCTION RATIO
WAVEFRONT DISTORTION/ FLATNESS
PRODUCT CODE
7100-2
1064 nm
200 MW/cm
9x9x25 mm
≥20:1 @ 633 nm
≤λ/8 @ 633 nm
99-48205-01
7100-4
1064 nm
300 MW/cm2
7.4x7.4x21 mm
≥20:1 @ 633 nm
≤λ/8 @ 633 nm
99-48202-01
7100-11A
1064 nm
300 MW/cm2
9x9x25 mm
≥20:1 @ 633 nm
≤λ/8 @ 633 nm
97-00970-03
7100-4 TS
1064 nm
300 MW/cm2
7.4x7.4x21 mm
≥20:1 @ 633 nm
≤λ/8 @ 633 nm
99-48302-12
7100-01 XTS
1064 nm
300 MW/cm2
9x9x25 mm
≥20:1 @ 633 nm
≤λ/8 @ 633 nm
97-00970-13
7100-11
1064 nm
500 MW/cm2
9x9x25 mm
≥20:1 @ 633 nm
≤λ/8 @ 633 nm
97-00970-10
GOOCH & HOUSEGO
2
39
FO FIBER OPTICS Gooch & Housego has been manufacturing the highest quality fiber optics since 1985. Our fiber optic group comprises two manufacturing and engineering centers, each known for its photonic engineering services and creating products for applications when reliability cannot be compromised. Environments where such consistency and longevity of performance are requisite include undersea and space. Components operating in such conditions have to be guaranteed not to fail.
Capabilities
42
Products Active Components Fiber-Coupled Pump Lasers
43
DFB Lasers and Modules
44
High Speed Detectors
46
Laser Controllers
47
Passive Components Fused Fiber Optic Components
48
Assemblies Fiber Optic Assemblies
50
Application-Specific Solutions OCT Components and Subsystems
51
High Reliability Fused Fiber Optic Components
52
High Reliability Erbium-Doped Fiber Amplifiers
53
GOOCH & HOUSEGO
41
FIBER OPTICS
TECHNICAL EXPERTISE AND MANUFACTURING CAPABILITIES G&H offers a range of space and Telcordia-qualified high performance active and passive fiber optic components and optical modules for use in laser, sensing, and communication (avionic, submarine, and space) applications. We develop and qualify fiber optic and semiconductor laser technology originally used in the telecom industry, adapting it for defense applications and deep space deployment – environments where the benefits of reliability, light weight, small size, and lower cost of ownership are compelling. We offer products and services from proof of concept through full scale volume production, lending customers our expertise in integration of end-to-end fiber optic systems and design for harsh environments. From custom packaging of semiconductor devices to fiber optic assemblies and fused biconical tapering, best-in-class design and manufacturing techniques optimize performance and reliability. Drawing on our expertise in fiber fusion, we have developed proficiency in the processing of photonic crystal fiber (PCF), enabling the incorporation of this advanced material into fiber lasers and supercontinuum sources. The standard fiber techniques of cleaving, splicing and mode adaption are more complex tasks when using PCF. Along with these more fundamental processes, we are also able to end cap, AR coat, and mode strip photonic crystal fiber for high power beam delivery. We support customers in systems development, components selection, manufacturing, and testing. Our engineering expertise includes passive and active fiber optics design, optoelectronics design, thermo-optic mechanical design, electrical design, RF design, material systems, hardware selection, process development, advanced micro-optic assembly, integration, laser welded photonic packaging, and testing.
QUALIFIED FOR SPACE, TELCORDIA, AND MIL-STD Many of our photonic solutions are deployed in or are currently being qualified for space. We understand how to develop, design, and manufacture for extremes of temperature, radiation, shock, and vibration. Our photonic components are qualified to Telcordia, MIL-STD, or Space (ESCC) standards. Active components are hermetically sealed using best industry practices, and many are RoHS compliant. As one of the first providers of fused fiber couplers, we have developed proprietary manufacturing equipment and processes, honed to deliver leading edge performance and reliability. We have a track record in the design and development of highreliability photonic components that are based on our enabling technologies. Our fiber optic, precision optic and acousto-optic components have flown on board various ESA and NASA missions including SMOS, ExoMars, Lisa Pathfinder, IRIS and Mars Curiosity.
ITAR COMPLIANT We have extensive capabilities and experience supporting and managing the unique needs of government sponsored development programs. US customers can work with and source directly from a US-based supplier who can leverage capabilities and products across all worldwide divisions of G&H.
In our HI REL component production we employ submicron alignment, and efficient light coupling is maintained throughout product lifetime. This precision, combined with the ability to hermetically seal devices in a dry, inert atmosphere enables us to supply customers with reliable and robust packaged devices.
42
GOOCH & HOUSEGO
FIBER OPTICS
THE AWARD-WINNING FIBER-Q® Combining micro-optical packaging capabilities and acousto-optic expertise How G&H used its photonic packaging expertise to develop a much needed device for the fiber laser industry. Our R&D engineers took an innovative approach to the development of a laser modulation device for the fiber laser community. The resulting Fiber-Q® can be used to reproducibly switch a fiber laser, modulate the amplitude or frequency shift the wavelength with precise electronic control. G&H’s expertise in photonic packaging brought for the first time, the flexibility and reliability of acousto-optics to the fiber optic industry. The resulting compact, robust, low loss device can easily be incorporated into all-fiber laser architecture without compromising the key benefits offered by fiber based systems. The rapid adoption of fiber laser technology for material processing in manufacturing has led to massive advances in technology, enabling high performance, low cost manufacture of many of the products consumers take for granted today (e.g. smart phones and flat panel displays). Compared to other laser technologies used in materials processing, fiber lasers provide a lower cost, low maintenance, solid state solution.
Since its introduction in 2009, many fiber laser applications have come to rely on the Fiber-Q®: “The Fiber-Q® product developed by G&H is a critical component in our amplified systems. The fast-response afforded by acoustooptic technology makes for an ideal switching device, enabling us to pick pulses with an excellent extinction ratio from our mode-locked seed oscillators, which have pulse repetition rates in the order of 10s of MHz and no other solution provides the performance balanced with the practicality and cost. The stability of the fiber-coupled solution allows us to maintain the critical holistic "all-fiber" approach to building our fiber laser platforms, which, in turn, provides the cost, flexibility, and reliability benefits when compared to competing laser technologies.” John Clowes, Director of Business Development at Fianium.
Now available in wavelengths from 400-2000 nm, hermetic and non-hermetic versions and with three port versions offered as well as the standard two port. The list of situations in which the device is used continues to grow and now in addition to industrial laser materials processing now includes biomedical and sensing applications. Developed to service this market, Fiber-Q® can be easily integrated into any fiber laser system to modulate the laser output with stable high efficiency performance delivering superior machining effects. Providing fast switch speed, with high peak diffraction efficiency and reliable performance, it has become the first choice for most ultra-fast fiber laser system manufactures.
Gooch & Housego (Torquay) received the Institute of Physics Award for Innovation and in 2016, the Queen’s Award for Enterprise: Innovation. GOOCH & HOUSEGO
The Fiber-Q® story illustrates how G&H is able to take one its core areas of expertise – in this case acousto-optics – and combine it with its micro-optical packaging capabilities to produce a world class, market leading device.
The Fiber-Q® team at G&H (Torquay) 43
FIBER OPTICS
FIBER-COUPLED PUMP LASERS Ruggedized, high power multi-mode and single-mode fiber-coupled lasers Our high power diode lasers feature ruggedized, epoxy-free designs intended for use in a wide range of harsh, long-life environments. Cooled and uncooled options are available to meet the most demanding diode laser applications. Single-mode (SM) pump lasers emit a low noise, precisely controlled, polarizationmaintained level of light at a specific wavelength out of a small-core fiber. Our series of cooled and uncooled diode laser products are designed with precise micro-alignment that stays true and stable through wide temperature ranges and high shock/vibration environments. All SM lasers feature a fiber Bragg grating (FBG) for stable, low noise operation. Customers may select to use the laser without the grating to enable temperature tuning of the central wavelength. The latest series of AC1409 SM lasers from G&H feature high polarization extinction ratio (PER) performance, enabling superior PM pump combining and other PER sensitive applications. In addition to standard products, output wavelength and other options can be customized for new applications.
Applications Fiber lasers, fiber optic gyroscopes, infrared sensing, life sciences, marking.
Multi-mode (MM) lasers offer high output power. G&H offers standard 14-pin fibercoupled package designs and other formats upon request. Cooled designs allow for wavelength tuning of the output for even greater wavelength control of the laser, while uncooled options feature higher power output.
A variety of low size, weight, and power custom designs can be employed to meet demanding aerospace and space mission applications. We also offer design and qualification services to ensure high reliability and long life under launch conditions for space mission applications.
Output power [mW]
G&H lasers are designed to ensure highly reliable operation across wide temperature and environmental conditions.
2.5
6 2
5 4
1.5
3
1
2 0.5
1 0
0 0
1
2
3
4
5
6
7
8
9
10
Current [mA] Power [W]
Voltage [V]
IPD [mA]
Typical Output Power and Forward Voltage vs Current (AC1409)
Typical Spectrum (AC1409 - 976 nm) 0
800
2.5
-20 -30 -40 -50
2
600 500
1.5
400 1
300 200
0.5
100 1100
1200
900
700
800
1000
Wavelength [nm]
500
0 600
1000
300
990
400
980
200
970
960
100
950
Forward voltage [V]
700
-10
Output power [mW]
Normalized power [dB]
3
7
Current [mA] P [mW]
V [V]
PRODUCT CODE
FIBER
PACKAGE
WAVELENGTH
COOLING
POWER
AC1409
PM or SM
14-pin
974, 976, 980 nm
Active
600, 700 mW
EM278
PM or SM
mini-DIL
976 nm
None
200 mW
EM322 through EM327
0.15 or 0.22 NA
14-pin
915, 940, 960 nm
None
7W
EM328, EM329
0.15 or 0.22 NA
14-pin
975 nm
None
6W
EM330 through EM337
0.15 or 0.22 NA
14-pin
915, 940, 960, 975 nm
Active
5W
EM339
0.15 or 0.22 NA
14-pin
808 nm
Active
3W
44
Voltage [V] & monitor current [mA]
Light-Current-Voltage (LIV) Curve 8
GOOCH & HOUSEGO
FIBER OPTICS
DFB LASERS AND MODULES High power and bandwidth in ruggedized butterfly packages or OEM modules Distributed feedback (DFB) lasers provide tunable wavelength output with extremely narrow spectral width and long coherence length. Integrated modules offer further narrowing of the spectral line in a compact OEM package with a simple tuning interface. DFB lasers feature a grating on the chip level structure to generate feedback into the cavity which ultimately enables stable, smooth, and precise wavelength tuning via temperature control of the chip. Additional feedback or external locking methods can ensure extremely stable wavelength control through many years or decades of use. Our DFB lasers serve a wide range of industrial, defense, medical, and scientific applications, with performance-enhancing design features that include: •
Integrated thermoelectric coolers (TECs) to reduce current consumption and extend operating temperature range Precision thermistors for accurate feedback and control of chip temperature Internal isolators to protect against back reflections and to reduce noise perturbations into the laser
• •
DFB LASERS IN 14-PIN OR 7-PIN PACKAGES DFB lasers provide precise single-frequency and single-spatial-mode performance with smooth tuning capability via temperature or current (chirp) tuning. We offer a range of products with high power and high bandwidth options in a rugged, singleemitter, fiber-coupled 14-pin or 7-pin butterfly package. Our high power series offers options up to 100 mW with >2.5 GHz direct modulation speeds, while our high bandwidth series offers up to 18 mW with >12 GHz direct modulation speeds.
Applications Distributed temperature sensing (DTS), fiber optic communications, gas sensing, interferometry, laser Doppler vibrometry (LDV), LIDAR, RF over fiber, seed lasers, spectroscopy.
Light-Current-Voltage (LIV) Curve
Relative Intensity Noise (RIN)
RF Performance
(AA1401 - 80 mW)
(AA1401 - 80 mW)
(AA0701 - High Bandwidth Series)
80
1.5
60 1
40
0.5
20 0
0 0
50
100
150 200 250 300 350 400 450 500
2
6
8
10
12
14
16
18
0 0
-147
-5
-149 -151 -153 -155
4
6
8
10
12
14 0 -5
-15
-10
-20
-157
-25 -30
-161
-35
-163
2
-10
-159
-15 -20 -25
-40
Frequency [GHz]
Current [mA] Power [mW]
4
-145
S11 [dB]
2
RIN [dBc/Hz]
Power [mW]
2.5
Voltage [V]
120 100
Frequency [GHz] S11 [dB]
Voltage [V]
S21 [dB]
PRODUCT CODE
WAVELENGTH
POWER OPTIONS
FIBER
AA1401, AA1406
1529-1610 nm
40, 50, 63, 80, 100 mW
PM or SM
AA1402
1617 nm
80 mW
PM or SM
AA1415
1529-1610 nm
40, 50, 63, 80, 100 mW
PM or SM
High isolation
AA1416
1537-1565 nm
40 mW
PM or SM
High isolation, high efficiency TEC
AA1411
1064 nm
50 mW
PM or SM
AA1409
1310 nm
18 mW
PM or SM
AA0701
1310, 1527-1565 nm
10, 18 mW
PM or SM
GOOCH & HOUSEGO
S21 [dB]
In addition to the variety of standard wavelength options in the 1-1.62 mm region, additional custom options are available upon request.
FEATURES
High bandwidth 45
FIBER OPTICS
DFB LASER MODULES Building upon our proven 14-pin packaged DFB lasers, G&H also offers compact OEM modules with excellent linewidth performance. All G&H modules comprise an integrated DFB laser, low noise diode driver, and TEC controller. To operate, the user need only provide a simple 5V power supply and voltage based tuning signals for temperature or current (chirp) adjustment, if required. The incorporation of an ultralow noise current source for the diode offers a vastly improved linewidth. The EM650 typically provides linewidth in the range of 100-350 kHz in a handsized package, approximately 66x64 mm (2.5”x2.5”) in size. The EM750 features an additional external cavity in a slightly larger package (3”x5”) to reduce the linewidth to approximately 10 kHz while emitting up to 50 mW out of the fiber. The expanded high bandwidth series of integrated modules includes two compact, easy to use models with direct modulation speeds in excess of 12 GHz. The EM655 offers the lowest linewidth at 1 MHz. The EM657 features an integrated internal switching power supply to remove the inherent voltage potential on the RF connector that is typically associated with laser diodes. The tuning port capacitive load on the EM657 is also lower, allowing for easier control via digital to analog converters.
PRODUCT CODE
WAVELENGTH
POWER OPTIONS
LINEWIDTH
FIBER
FEATURES
EM650
1064, 1310, 1529-1617 nm
40, 50, 63, 80, 100 mW
~ 200 kHz
PM or SM
Compact footprint
EM750
1532-1575 nm
30, 50 mW
~ 10 kHz
PM or SM
Reduced linewidth
EM655
1310, 1530-1570 nm
10, 18 mW
~ 1 MHz
PM or SM
>12 GHz direct modulation
EM657
1310, 1530-1570 nm
10, 18 mW
~ 4 MHz
PM or SM
>12 GHz direct modulation; floating RF connector
46
GOOCH & HOUSEGO
FIBER OPTICS
HIGH SPEED DETECTORS Ripple free, linear response from DC to 20 GHz High speed detectors (HSDs) are a crucial component at the interface between optical and electrical communications systems to achieve clean conversion of photonic RF signals to electrical RF signals at high bandwidth and fidelity. Our photodetector designs offer low dark current or noise, and perform with excellent responsivity. The EM169 photodetector series offers bandwidth rated to a minimum of 20 GHz over multiple wavelength bands with a single device, including 1310 nm, C-band, and L-band. The new EM530 photodetector further expands the product range with a dramatic increase in power handling over the same broad wavelength range, and features a bandwidth of 10 GHz. For a 50 mW input signal, the EM530 photodetector provides a 32 mA photocurrent level, thus increasing the level by a factor of 10 compared to the EM169 and other comparable photodetectors. Manufactured in volume, G&H’s two high speed photodetector devices are rated for performance over a wide temperature range. Our designs maximize photodetector performance to enable higher power and high speed ruggedized systems for defense and other demanding applications. Applications RF over fiber, infrared sensing, optical signal processing, phased arrays.
PRODUCT CODE
WAVELENGTH
AVERAGE POWER
RESPONSIVITY
BANDWIDTH
FIBER
FEATURES
EM169-xx
1280-1620 nm
3 mW
~ 0.95 A/W
20 GHz
PM or SM
High speed
EM530-xx
1280-1620 nm
50 mW
~ 0.65 A/W
10 GHz
PM or SM
High photocurrent
RF Performance
RF Performance
(EM169)
(EM530)
3
-8 -13
2
3
2
-10
1
-20
-28 0
2
4
6
8
10
12
14
16
-1
18
20
-33
-30 0
1
2
3
4
5
6
7
8
9
10
-1
-40
-2
-50
S22 [dB]
-23
S21 [dB]
1
S22 [dB]
S21 [dB]
-18
-38 -2
-43
-3
-48
Frequency [GHz] S21 [dB]
GOOCH & HOUSEGO
S22 [dB]
-3
-60
Frequency [GHz] S21 [dB]
S22 [dB]
47
FIBER OPTICS
LASER CONTROLLERS Convenient USB or touch-pad interface control of diode lasers Benchtop laser controllers provide a convenient interface for operation of diode lasers in production or laboratory environments. Our easy-to-use controller is compatible with single-mode (SM) and DFB lasers in standard 14-pin butterfly packages, allowing simple touch-pad or computer control of interchangeable lasers with different wavelength or power characteristics. The EM595 benchtop controller combines a laser driver and thermoelectric cooler (TEC) controller into a compact, benchtop device with an intuitive user interface. With 1.5 A of laser drive current available, the G&H EM595 laser diode driver can operate any 14-pin DFB or single-mode laser. The 3.0 A of current available for the TEC provides ample controlling capability for typical room or lab temperature environments, with the capability of operating single mode (SM) or distributed feedback (DFB) lasers over their full rated range. Precise temperature control results in accurate laser frequency control. The EM595 establishes a new level of low noise and linewidth performance in a benchtop device. The ability to easily swap lasers with different wavelength or power characteristics allows a single controller to operate several lasers. This is useful for experiments involving repetitive testing where users need to dynamically modify operational parameters to meet test objectives. In production environments, the benchtop EM595 unit allows quick and easy testing and verification of a variety of products flowing through a production line. The automation offered by our laser diode driver further saves time and money while maintaining quality, calibrated results. Applications Laboratory and production testing.
PRODUCT
PRODUCT CODE
DIODE CONTROL RANGE
NOISE/RIPPLE
Benchtop Laser Controller
EM595
0-1.5 A
<10 µA
48
GOOCH & HOUSEGO
FIBER OPTICS
FUSED FIBER OPTIC COMPONENTS The highest performance fused fiber couplers and high power combiners G&H manufactures a comprehensive line of optical taps, power combiners, attenuators, and WDMs based on fused fiber technology for wavelengths from the visible through near-infrared. Fused fiber couplers split and combine light signals by coupling light directly between the fiber cores, offering advantages in efficiency and reliability over filterbased couplers. By varying the parameters of the fusion and tapering process, our components precisely control the proportion of light split between fibers and the wavelength at which the split occurs. G&H fused fiber components are used for branching of optical signals and interfacing in telecommunications, sensor, and biomedical systems. We also offer devices to meet the needs of optical coherence tomography (OCT) based systems, and components for operation over a broad band centered at 2 µm. Our fused coupler production process has been honed over decades to achieve low insertion loss, high power handling, and high extinction ratio, with exacting manufacturing controls to ensure high quality and reliability.
SINGLE-MODE FIBER COMPONENTS G&H single-mode couplers are used to achieve accurate monitoring and splitting of optical signals from 1% to 50%. Polarization-maintaining (PM) couplers are available in slow axis, fast axis, and axis-independent variants. PRODUCT
FUNCTION
WAVELENGTH
Fixed Attenuator
Attenuator
C, L, C+L, S-band
Dual Window Wideband Coupler
Tap coupler
1310 nm, C-band
Visible Wavelength Coupler
Tap coupler
400-700 nm
Near Infrared Coupler
Tap coupler
700-1200 nm
Ultra Low Ratio Tap Coupler
Tap coupler
700-1600 nm
Fused Coupler
Tap coupler
980 nm, 2 µm
NXN Fused Coupler
Tap coupler
980, 1310, S, C, L-band
Fused Coupler, C or L band
Tap coupler
C, L-band
Subminiature Tap Coupler
Tap coupler
C, L, C+L, S-band
Fused Coupler, C+L or S band
Tap coupler
C+L, S-band
Visible Wavelength Combiner
WDM
400-700 nm
Near Infrared WDM
WDM
700-1199 nm
2 µm WDM
WDM
2 µm
Fused Pump Signal WDM
WDM
980 nm, C, L, C+L-band
Subminiature Pump Signal WDM
WDM
980 nm, C, L, C+L-band
Duplexing WDM, 1x2 or 2x2
WDM
1310 nm, C, L-band
Fused Pump Signal WDM
WDM
1480 nm, C, L-band
GOOCH & HOUSEGO
Applications Avionic and space communications, biomedical instrumentation, fiber laser systems, industrial micromachining, interferometry, LIDAR, medical diagnostics, optical coherence tomography (OCT), sensing, telecommunications.
We have extensive experience in the volume production of fused fiber components for telecommunications deployment, and can customize any of our designs to meet the needs of volume OEM applications. Our engineers routinely apply their knowledge to design custom products for our customers, to meet their unique needs. The tables show a range of typical G&H fused fiber components.
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FIBER OPTICS
PM FIBER COMPONENTS G&H polarization-maintaining (PM) couplers are available in ratios from 1% to 50%, and are manufactured using industry standard fiber. PM couplers are available in slow axis, fast axis, and axis-independent variants at wavelengths up to 2 μm. PRODUCT
FUNCTION
WAVELENGTH
PM Combiner
Combiner
980, 1060, 1450, 1550, 1650 nm
2+1x1 Power Combiner with PM signal feedthrough, 2 μm
N+1x1
750-850, 2000 nm
6+1x1 Power Combiner with signal feedthrough, 2 μm
N+1x1
750-850, 2000 nm
High Power Connectors and Patchcords
Connectors
750-2100 nm
PM Coupler
Tap coupler
750-1700 nm
PM Bow Tie Fiber Coupler
Tap coupler
900-1200 nm
Axis-Matched Low Ratio Tap
Tap coupler
900-1600 nm
Ultra Low Ratio Tap Coupler
Tap coupler
900-1700 nm
PM WDM
WDM
750-1600 nm, 2 µm
Polarization-Maintaining Coupler 1060 nm 30
PER [dB]
25 20 15 10 5 0 -10
10
20
30
40
50
60
70
80
Temperature [°C]
Polarization-Maintaining WDM 1120 nm/1178 nm - Low Loss, High Isolation
HIGH POWER MULTI-MODE PUMP COMBINERS
Insertion loss [dB]
20 15 10 5 0 1080
Our range of pump combiners for high power fiber lasers is based on precise fusion of multi-mode fiber techniques. For pumping of complex fiber amplifier designs, we have developed a signal feedthrough fiber at the center of the multi-mode fiber bundle, which is both single-mode and polarization-maintaining. All variants are available with custom pump, signal, and output fibers. PRODUCT
FUNCTION
WAVELENGTH
6+1X1 Power Combiner with signal feedthrough
N+1x1
900-1000, 1064, 1550 nm
6+1X1 Power Combiner with PM signal feedthrough
N+1x1
900-1000, 1064, 1550 nm
2+1x1 Power Combiner with PM signal feedthrough
N+1x1
900-1000, 1064, 1550 nm
2+1x1 Power Combiner with signal feedthrough
N+1x1
900-1000, 1064, 1550 nm
1140
1160
1180
1200
1220
Series 1
Series 2
19x1 Multi-Mode Combiner 980 nm - High Efficiency 0.45 0.4
N+1x1
900-1000, 1064, 1550 nm
2+1x1 Power Combiner with active signal feedthrough
N+1x1
900-1000, 1064, 1550 nm
Multi-mode Power Combiner
NX1
900-1000 nm
0.35 0.3 0.25 0.2 0.15 0.1 0.05 0 1
50
1120
Wavelength [nm]
Insertion loss [dB]
2+1x1 Power Combiner with active PM signal feedthrough
1100
2
3
4
5
6
7
8
9 10 11 12 13 14 15 16 17 18 19
Input port [#]
GOOCH & HOUSEGO
FIBER OPTICS
FIBER OPTIC ASSEMBLIES Integrated fiber optics to simplify your designs G&H offers custom modules of passive and/or active optical components integrated to provide higher functionality in a compact footprint. Our optimized designs use low loss G&H products and advanced assembly techniques such as ribbon splicing and fiber recoating to provide robust solutions that reduce development costs and speed time to market. Our more complex designs have included bulk optics, fiber optics, motion control, and electronics. We optimize fiber assemblies for minimum temperature dependence and maximum reliability by performing finite element stress and strain analysis in 3D solid modeling software. Optical modeling tools are used to design and analyze complex optical trains, including fiber lasers and fiber amplifiers. We can design power, control, and monitoring circuits to optimize component performance and minimize noise. Proprietary techniques are used for mounting fiber optic components and routing fibers in a robust and reliable process while maintaining optimum optical performance. All fiber assemblies are produced using state-of-the-art equipment in clean environments meeting up to Class 10,000 rating, as needed. We have in-house facilities for reliability testing, including thermal cycling chambers, high power lasers, and shock and vibration testing equipment. In addition to custom module designs implemented as build-to-specification or build-to-print, we also offer a range of standard drop-in modules for a wide range of functions. Applications Biomedical instrumentation, fiber laser systems, interferometry, LIDAR, medical diagnostics, optical branching networks, optical coherence tomography (OCT), retinal scanning systems, sensing, spectroscopy, telecommunications.
The products listed in the table below illustrate examples of fiber optic modules. Our product managers and sales engineers routinely work with customers, applying our expertise to customize products or build to customers’ own designs. PRODUCT
DESCRIPTION
Fiber Pigtailed Laser
Lasers pigtailed using single-mode, PM or multi-mode fibers, 405-1550 nm; standard and custom.
Fiber Collimator
A range of non-contact style, single-mode fiber collimators incorporating achromatic lenses; standard and custom.
Custom Modules
Assemblies of low loss G&H passive and/or active optical components designed to provide a specific functionality.
Butterfly Pigtailed Laser
Butterfly lasers pigtailed using single-mode, PM or multi-mode fibers, 630-1550 nm; standard and custom.
Network Expansion Module
Splits optical signals in single-mode optical fiber for optical networking applications; 1x3 to 2x16 standard, custom available.
Motorized Variable Optical Delay Line
Varies optical path length quickly and accurately in a compact housing with single fiber pigtail.
GOOCH & HOUSEGO
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FIBER OPTICS
OCT COMPONENTS AND SUBSYSTEMS Reliable, high-performance solutions for commercial OCT systems Optical Coherence Tomography (OCT) is a technique that utilizes low coherence optical interference to create noninvasive 3D images of biological tissue in real time. G&H enables fiber optic OCT systems with the high-performance fused fiber components, assemblies, and spectrometers needed to achieve highresolution imaging.
Drawing on deep knowledge of optical technology and experience in the design of custom OCT modules, G&H has developed a complementary set of key optical elements for OCT systems. Our OCT optical delay line, used as an interferometer reference arm, offers stable optical performance over time, delay and environmental conditions. OCT interferograms can be analyzed by our compact OCT optical spectrometer, which offers state of the art resolution and image capture rate. In addition to our commercial off-the-shelf products, G&H has the optical design skills and fabrication facilities to produce custom optical beam delivery systems, fiber interferometers, and bespoke optical modules incorporating electronics and motion control for OCT systems in volume. Custom projects have included fiber switching circuits, stepped fiber assemblies, fiber based ASE sources, and full optical head assembly. Applications Clinical diagnostics, medical instrumentation, OCT research.
Compact OCT optical spectrometer 80/20 OCT Coupler Process Capability Study 160 140
Frequency
While traditional retinal scanning systems may use an optical source with a bandwidth of ~30 nm, the latest generation of OCT systems are moving to >100 nm bandwidth to deliver higher resolution images. In response, G&H has developed the Extremely Wideband Optical Coupler (EWOC) with uniform performance over a 140 nm wavelength range, making it ideal for high end and future generations of OCT instruments.
Small form-factor OCT delay line
120 100 80 60 40 20 0 78.9 79.1 79.3 79.5 79.7 79.9 80.1 80.3 80.5 80.7 80.9 81.1
Insertion loss [dB]
EWOC 50/50 OCT Coupler 200 nm Operating Band 60
Coupling ratio [%]
The initial rapid growth of OCT was driven by ophthalmic applications, particularly the unique ability to provide retinal in vivo imaging. It is now being applied to the biometric measurement of the eye’s anterior segment (cornea and lens), significantly improving treatments such as cataract replacement. The technique is also being applied to imaging of the skin, artery walls, the esophagus and other tissues for clinical diagnostics and as an alternative to biopsy. High quality, performance and reliability has made G&H a leading supplier for OCT ophthalmology instrumentation, providing the fused fiber couplers, interferometers, and collimators used in many commercial systems. Exacting control over our manufacturing processes ensures highly repeatable performance and tight performance distributions.
50 40 30 20 10 0 950
1000
1050
1100
1150
Wavelength [nm] Series 1
Series 2
PRODUCT
FUNCTION
WAVELENGTH
FEATURES
OCT Fiber Collimator
Collimator
840, 1060, 1300 nm
2, 3 mm beam diameter options
OCT Coupler, 850 and 1300 nm
Tap coupler
850, 1310 nm
±20 to ±50 nm bandwidth options
OCT Coupler, 1060 nm Wideband
Tap coupler
1060 nm
±20 to ±50 nm bandwidth options
OCT Coupler, Extended Wideband (EWOC)
Tap coupler
840, 1060, 1300 nm
±100 nm bandwidth
OCT Optical Delay Line
Delay line
850, 1060, 1310 nm
Point-and-return; customizable chassis
Small Form-Factor OCT Variable Optical Delay Line
Delay line
850, 1060, 1310 nm
Point-and-return or dual fiber; customizable chassis
Compact OCT Optical Spectrometer
Spectrometer
850, 1060, 1310 nm
<0.1 nm/pixel resolution; flexible platform
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GOOCH & HOUSEGO
FIBER OPTICS
HIGH RELIABILITY FUSED FIBER OPTIC COMPONENTS Proven performance and reliability for undersea and space applications The G&H line of HI REL components are deployed in environments such as undersea and space where the costs of component replacement are prohibitive and reliability is of premier concern. G&H is established as a preferred supplier of these components to most major undersea telecommunications equipment manufacturers. Our HI REL capability is built upon the foundation of an extended history of also manufacturing very reliable components for land-based (or terrestrial) systems in volume. G&H has established full reliability testing facilities to carry out customer specific HI REL qualification programs, which can include accelerated aging and Weibull analysis. Failure rates for undersea telecommunication systems and components are often described using a FIT rate (Failures in Time). The fused fiber couplers from our HI REL coupler range offer a very low 0.1 FIT rate, equivalent to one failure in roughly fifty thousand components in 25 years. The ultra-low loss of G&H fused fiber components helps to promote low noise figure and improved system margin in undersea transmission systems. Components are supplied in regular (bare fiber), semi-ruggedized (0.9 mm sleeving) or custom housings, depending on the installation environment. The newest addition to the range is our pump combiner, which allows erbium-doped fiber amplifier (EDFA) designers to double pump powers. This enables higher power EDFAs and in turn greater data carrying capacity. In space applications, photonics is expected to displace current RF/microwave satellite technology for transport of data between satellites, and between satellites and the Earth. In addition to offering higher data carrying capacity than the present radio wave systems, the reduced size and weight of optical systems will enable smaller, lighter next generation satellites. The G&H HI REL space range of fused fiber components builds on the quality and reliability for which our undersea couplers are known, adding features such as material lot unicity, qualification in high radiation environments and lot validation testing. Services for HI REL customers include custom qualification programs, dedicated workstations, full traceability of materials and processing, advanced fiber management, and customer-specific validation tests. Applications
NEW
Undersea telecommunications, harsh environment, satellite laser communications, satellite on-board optical processing.
PRODUCT
FUNCTION
WAVELENGTH
High Reliability Fused Coupler, 980 nm band
Tap coupler
980 nm
High Reliability C or L band Fused Coupler
Tap coupler
C, L-band
High Reliability Pump Signal WDM
WDM
980 nm, C-band
High Reliability Pump Signal WDM
WDM
1480 nm, C-band
High Reliability Pump Combiner
Combiner
980 nm
GOOCH & HOUSEGO
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FIBER OPTICS
HIGH RELIABILITY BOOSTER ERBIUM-DOPED FIBER AMPLIFIERS Modules for space flight and harsh environments Fiber amplifiers are used widely to boost signals in terrestrial telecommunications, and can be designed to enable transmission distances of more than 70 million kilometers for use in the next generation of deep space probes. G&H’s high-reliability erbium-doped fiber amplifier (EDFA) and erbium/ytterbium co-doped (EYDFA) fiber amplifier modules are designed to operate in demanding thermal, vibration, and radiation environments. When offered as OEM modules, they can be controlled and monitored through an electrical interface – ideal for system integration into laser transmitters, including satellite laser communication terminals. The G&H optical amplifier product family includes pre-amplifiers, mid-booster amplifiers, and high power amplifiers. Versatility is allowed for with different levels of laser modem and terminal system integration: • • •
Gain blocks offer direct access to optoelectronic components allowing for external control EDFA modules include circuitry to monitor and control the optical fiber amplifier operation Digital or analog interfaces can be provided with tailored functions and control levels
Applications Optical inter-satellite links, satellite to ground laser communications, space probes.
Customized optical performance, enclosures, port configurations, and amplifier arrays in a single housing can be developed to meet end-user and mission requirements for optical and electronic functionality, as well as mechanical housing customization. Our units integrate high reliability passive and active components fabricated and tested in-house, maintaining full visibility and control over the supply chain.
PRODUCT
WAVELENGTH
OUTPUT POWER
STATIC GAIN FLATNESS
FIBER
HYDRA Series
1530-1565 nm
+16 to +21 dBm
<0.5 dB
PM/SM
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GOOCH & HOUSEGO
PO PRECISION OPTICS Gooch & Housego began manufacturing precision optics in 1948. Today our precision optics manufacturing encompasses five operations, located in the UK and the US, each focused on its own unique capabilities. From components to modules, the deep vertical integration of our supply chain allows us to maintain control over design, materials, and processes, while ensuring quality and security of supply.
Capabilities
56
Products Precision Prisms
63
Corner Cubes
64
Precision Lenses
65
SWIR Lens Assemblies
66
Precision Mirrors
68
Synchrotron Mirrors
69
Plate and Cube Beamsplitters
70
Windows and Optical Flats
71
Waveplates 72 Superpolished SROC
74
Ring Laser Gyroscope Components
75
Infrared Optics
76
Optical Domes
77
Electro-Optic Sighting Systems 78
GOOCH & HOUSEGO
55
PRECISION OPTICS
TECHNICAL EXPERTISE AND MANUFACTURING CAPABILITIES G&H develops and manufactures world class precision optical components and assemblies for applications in aerospace & defense, industry, medical systems and scientific research. Our expertise ranges from nonlinear optical crystal growth, to crystal quartz waveplate production. Our capabilities include: • • • • • • • • •
Optical crystal growth Single-point diamond turning Magnetorheological finishing (MRF) Superpolishing Coatings Hy-Per Bond™ – adhesive and organic-free bonding Opto-mechanical assemblies Electro-optical assembly and systems Metrology
We have advanced capabilities in anti-reflection, high reflection, and high laser damage threshold coatings, as well as adhesive-free bonding. As part of a process of continuous improvement, each of our five operations strives to expand, develop, and improve its competencies. G&H products for laser cavity and beam conditioning include active and passive components as well as nonlinear crystals. Many customers employ our custom lenses and housed subassemblies in transmission and imaging applications. Much of our business involves creating high quality, custom optics for volume OEM applications and unique optics for research. G&H superpolished ring laser gyro mirrors are used in most major aerospace manufacturing programs around the world. We have provided 0.4x0.4 m KDP waveplates to the National Ignition Facility (NIF).
56
OPTICAL CRYSTAL GROWTH Beginning with the raw chemicals we grow, orient, fabricate, finish, coat, and mount: ß-barium borate (BBO), cadmium sulfide (CdS), cadmium selenide (CdSe), potassium dihydrogen phosphate (KDP), potassium dideuterium phosphate (KD*P), lithium niobate (LiNbO3 or LN), and tellurium dioxide (TeO2).
MATERIALS Our expertise in optical materials begins with the selection of the correct material to meet the requirements of customers. We grow much of our own crystalline material and employ rigorous sourcing procedures for those crystals externally procured. We routinely work with a wide variety of optical glass types. The level of vertical integration of our manufacturing processes allows us to provide dependable design advice, and improves the quality of our finished products through unified standards and reduced component handling between manufacturing steps.
GOOCH & HOUSEGO
PRECISION OPTICS
MATERIAL
APPLICATIONS
ß-barium oxide (BBO)
• Pockels cells
Cadmium selenide (CdSe)
• Infrared waveplates
Cadmium sulfide (CdS)
• Infrared waveplates
Calcite (CaCO3)
• Polarizers
Calcium fluoride (CaF2)
• Lenses, windows, mirrors
Chalcogenides: GASIR®, AMTIR
• Wide bandwidth windows and lenses
CVD SILICON CARBIDE™ (silicon carbide)
• Mirrors
Deuterated dihydrogen potassium phosphate (KD*P)
• Ultra high energy research lasers
Dihydrogen potassium phosphate (KDP)
• Pockels cells
Filter glasses
• Optical filters
Fused silica
• Acousto-optic devices, high power laser optics, low expansion substrates
Gallium arsenide (GaAs)
• Infrared windows and lenses
Germanium (Ge)
• Infrared windows and lenses, acousto-optic devices
Glasses: flint, crown, fused silica
• Prisms, lenses, and flats
Lithium niobate (LiNbO3)
• Acousto-optic devices, waveplates/retardation plates and depolarizers
Lithium triborate (LiB3O5)
• Frequency doubling
Low CTE glass: ZERODUR®, CLEARCERAM®-Z
• Mirrors for metrology, ring laser gyro blocks, stable optical mounts, metrology reference blocks
Magnesium fluoride (MgF2)
• Achromatic waveplates, polarizers, waveplates
Multi-Spectral Zinc Sulphide: CLEARTRAN™
• Infrared lenses
Phosphate glasses (P2O5)
• Laser rods
Quartz: synthetic SiO2
• Acousto-optic devices, waveplates, rotators
Sapphire: α-Al2O3
• Very hard windows and waveplates
Silicon (Si): polycrystalline, mono-crystalline, standard optical grade, floatzone
• Infrared windows and lenses
Silicon carbide (SiC)
• Optical flats
Spinel: MgAl204, Co:MgAl204
• Passive Q-switches
Tellurium dioxide (TeO2)
• Acousto-optic devices
YAG: Y3Al5O12
• Laser rods
Zinc selenide (ZnSe)
• Infrared lenses
Zinc sulfide (ZnS)
• Infrared lenses
GASIR® is a registered trademark of Umicore CVD SILICON CARBIDETM is a registered trademark of the Dow Chemical Corporation ZERODUR® is a registered trademark of Schott AG CLEARCERAM®-Z is a registered trademark of Ohara Corporation CLEARTRAN™ is a registered trademark of the Dow Chemical Corporation
GOOCH & HOUSEGO
57
PRECISION OPTICS
SINGLE-POINT DIAMOND TURNING We use single-point diamond turning (SPDT) to produce ultra-precision infrared optical components such as infrared aspheric, diffractive and spherical optics and gratings. The process of mechanical machining infrared optical components using lathes equipped with diamond tipped tools enables us to manufacture crystal based optical products with a greater degree of precision than otherwise possible with standard machining techniques.
CHARACTERISTICS Configurations
• High performance rotationally symmetrical with raster correction for high precision optics such as IR spherical lenses, aspheres, binary diffractive lenses (plano, spherical, aspherical diffractive), Fresnel lenses, hybrid lenses, mirrors.
Material
• Calcium fluoride (CaF2), chalcogenide glass (gallium arsenide), germanium, silicon, zinc selenide, zinc sulphide, multi-spectral zinc sulphide (CLEARTRAN™) and other materials on request. Refer to materials table for further details.
Sizes
• Diameter range from 8.0-250.0 mm
Surface form error
• ≤0.25 µm P-V (depending on material and configuration)
MAGNETORHEOLOGICAL FINISHING (MRF) MRF is a patented, deterministic lens surface finishing process which G&H uses to improve form finish of precision optical components. This technique enables us to control optical polishing with a greater degree of precision than conventional lap polishing. These complement existing polishing capabilities for surface correction when enhanced precision is required.
CHARACTERISTICS MRF polishing service
• Flats, spherical lenses and aspheres.
Materials
• Common glasses (CDGM, Hoya, Ohara, Schott, Sumita, etc.), fused silica, glass ceramics, calcium fluoride, silicon, germanium. Refer to materials table for further details.
Size
• Up to 200 mm in diameter
Form figure
• Up to λ/50 P-V
Metrology
• Sub-aperture stitching interferometer (SSI®) to measure high numerical aperture, large clear aperture parts, transmitted wavefront testing.
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GOOCH & HOUSEGO
PRECISION OPTICS
SUPERPOLISHING For ring laser gyroscope (RLG) mirrors, R&D applications, short wavelength and ultrafast lasers, superpolishing offers significantly superior performance compared to products from other optics manufacturers. G&H’s process delivers ScratchDig of 5-2, less than 0.5 Å of surface roughness, and zero defects at 300x magnification. Most superpolished optics are supplied with polished or acid-etched outside diameters and bevels. These extra refinements add to the level of cleanliness and durability of the components. Superpolished materials include N-BK7, calcium fluoride, crystal quartz, fused silica, sapphire, silicon carbide, YAG and Nd:YAG, and ZERODUR®.
Roughness comparison showing superpolishing vs. regular high quality optical polishes
Sapphire Polishing Sapphire is a unique material well suited for many ultraprecision optical applications. It is transparent from the lower UV (142 nm) through the mid IR (6.5 µm). Its high tensile strength makes it well suited to many high g-force environments. In addition, sapphire is very tolerant of high radiation environments, such as space-based applications. Due to its high mechanical strength, sapphire is a very difficult material to polish. Our unique superpolishing processes allow us to polish sapphire components to better than 1 Å surface roughness. Silicon Carbide Silicon carbide (SiC) is often used in the optics industry to replace components previously manufactured from beryllium. The material offers a viable alternative with low weight, high specific stiffness, high thermal conductivity and excellent dimensional stability. We have developed expertise in polishing silicon carbide mirrors, and can polish CVD SILICON CARBIDE™ and lightweighted versions of this material. G&H also offers customer-supplied substrate polishing services. Additionally, we offer SiC cladding with IBS coatings to ensure the finest possible final surface finish. Lastly, we also supply optical coatings on the finished mirror.
COATINGS G&H operates four facilities with thin film optical coating capabilities: two in the US and two in the UK; each with multiple chambers. We offer customers temperature stable optical coatings to meet high laser damage thresholds at short pulse lengths across the bandwidth of commercial laser wavelengths from deep UV through to far IR. Our expertise in coating has been supported by investment in custom built, ultra-clean, high repeatability chambers to meet customers’ evolving needs for environmentally-stable optical coatings. Our engineers are continuously researching the performance characteristics of new coating materials and integrating the results into our modelling software to optimize the designs for customers’ applications. We have a comprehensive range of coating techniques: • • • • •
Thermal evaporation Electron-beam (e-beam) Ion assisted deposition (IAD) Ion beam sputtering (IBS) and Chemical vapor for diamond-like coatings (DLC)
GOOCH & HOUSEGO
1
DEPOSITION TECHNOLOGY
COATING TYPES OFFERED
Chemical vapor
• Diamond-like coating (DLC)1
Thermal evaporation
• Metallic
Electron beam gun evaporation (e-beam)
• • • •
High-reflection (HR) Anti-reflection (AR) V-coats, double-V coats Broadband AR
Ion assisted e-beam deposition (IAD)
• • • • •
High-reflection (HR) Anti-reflection (AR) V-coats, double-V coats Broadband AR Bandpass filters (high and low)
Ion beam sputtering (IBS)
• Dielectric mirrors • High-reflection (HR)
Currently outsourced
A chamber that incorporates thermal, e-beam, and an ion source provides increased coating flexibility. This enables us to tune and allow selective bombardment of the various coating materials during deposition to match challenging substrate types and meet exacting performance requirements.
59
PRECISION OPTICS
We use thermal evaporation for deposition of metals and dielectrics which are less compatible with e-beam coating. For the many materials that are compatible however, the e-beam technique provides coating with lower stress where surface flatness is a priority, higher laser induced damage threshold (LIDT), and improved control of impurities in the deposited material. E-beam is especially useful for coating components for operation at deep ultraviolet and infrared wavelengths. Ion assisted electron beam (IAD) coating deposits robust coatings with very high laser induced damage threshold (LIDT) and very low thermal shift. IAD coatings are widely utilized for optical systems designed for the defense industry where multiple laser wavelength devices are required to work together in rugged environments.
Ion beam sputtering (IBS) generates very dense, hard coatings ideal for very high reflection and low loss requirements. IBS is thus well-suited to finishing super-polished mirrors – whether for cutting edge research or for Ring Laser Gyros (RLG). IBS coatings have a lower LIDT than IAD coatings. As part of the quality control process, we test our coated optics using the following processes: • •
Temperature cycling, adhesion, abrasion and humidity testing to ISO and MIL standards. Transmission measurements made using spectrophotometers with wavelengths from 300 nm to 28 μm. IBS Coated Laser Mirror 100.000 99.995
Reflectance [%R]
99.990 99.985 99.980 99.975 99.970 99.965 99.960 99.955 99.950 570
590
610
630
650
670
690
710
Wavelength [nm]
Ion beam sputtering (IBS) coated laser mirror Reflectance confirmed with cavity ring-down spectroscopy (CRDS)
HY-PER BOND™ – ADHESIVE AND ORGANIC-FREE BONDING Hy-Per Bond™, our adhesive-free bonding process, overcomes issues such as beam distortion and performance degradation resulting from the outgassing of optical cement. Hy-Per Bond™ is more tolerant of temperature differentials than optical contacting when used in high energy, humid, or cryogenic applications. By activating precision optical surfaces prior to joining them, permanent bonds are formed between the components, improving environmental stability. When bonding low expansion ceramics, thermal distortion is negligible. Key features include: • • • • • • • • • 60
Space qualified No outgassing In shear strength trials the bulk material fails, rather than the bond Negligible thermal distortion Resistant to moisture and vibration Maintains strength at cryogenic temperatures Stronger than optical cement (>50 MPa) Alignment at submicron accuracy Bond thickness ~100 nm
Hy-Per Bond™ is suitable for a wide range of materials, including fused silica, ZERODUR®, crystal quartz, and optical glasses. Hy-Per Bond™ can also be utilized for large surface areas, up to 170 cm2. Bonds tested achieved a laser induced damage threshold (LIDT) of >15 J/cm2, significantly better than typical epoxy-based bonds.
GOOCH & HOUSEGO
PRECISION OPTICS
OPTO-MECHANICAL ASSEMBLIES Protecting the customers’ investment in precision optical components, we offer a value-added service of design, manufacture, and assembly of the optical components into protective easy-to-handle housings. The cost and time benefits to production when sourcing an opto-mechanical assembly from G&H can be significant: • •
• • •
Pre-alignment of complex optical components enables drop-in final assembly Precision alignment of various and varied optical surfaces reduces production time and internal metrology requirements Ease of handling minimizes internal production time Minimization of damage to precision surfaces reduces yield losses Relaxation of cleanroom requirements lowers facility costs
Optomechanical assembly
Applications Laser cavity designs: Lasers, rangefinding, reconnaissance, surveillance, target identification, targeting and designating.
The opto-mechanical assemblies we produce for customers are wide ranging and include: • • • • •
Prisms potting in aluminum housings Waveplates in ring-mounted housings Periscope prism assemblies 25x magnification lens assemblies Zoom lenses
Imaging designs: Dermatology, endoscopy, hyperspectral imaging, inspection, machine vision, metrology, optometry, projection, thermal imaging.
ASSEMBLY TYPE
RANGE OF CAPABILITIES
Laser cavity and beam conditioning sub-assemblies
• • • •
Mirror and acousto-optic sub-assemblies Zero order waveplates, retarders in a housing Assembled prisms, beamsplitter cubes Frequency doubling crystals in a housing
Transmission and imaging sub-assemblies
• • • •
Doublet, triplet lenses Beam focusing lens sub-assemblies Integrated electro-mechanic components Custom housing and mounts
Optical modules
• Integrated optics and electronics • Build-to-print, or design and manufacture • Optimized optical performance, footprint, power consumption
ELECTRO-OPTICAL ASSEMBLY AND SYSTEMS For some customers, the convergence of electronics, mechanics, and photonics with G&H design and assembly capabilities have enabled them to realize significant performance improvement, operational optimization, and cost savings. Our design-for-manufacture approach enables our customers to gain improved product performance while at the same time reducing costs and managing delivery schedules.
GOOCH & HOUSEGO
In partnership with our customers, we have designed a widevariety of electro-optical assemblies and systems ranging from: • • •
Optical coherence tomography sub-systems Rangefinding laser systems Electro-optical sighting systems (EOSS)
G&H design and manufacturing teams are well-versed in delivering products into military and medical applications.
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PRECISION OPTICS
METROLOGY To deliver high quality components and systems, it is critical to accurately measure and test processed optical components with high precision and accuracy. At G&H, we have invested in world class measurement equipment to ensure the parts our customers receive meet the most exacting of specifications. If we can measure it; we can make it We use a range of interferometric measurement systems during production and at the end of processes as part of our quality assurance procedures. This enables us to provide a broad range of exceptionally high quality precision optical components and assemblies.
METROLOGY INSTRUMENT/SYSTEM
CAPABILITIES
6” GPI™ LC interferometer
• Visual fringe analysis of flat or spherical surfaces • Transmitted wavefront measurement, OD≤4
NewView™ 5000 white light interferometer
• Fast, non-contact, high-precision 3D metrology of surface features
QED SSI stitching interferometer
• Measures aspheric optics up to 1000 λ from best fit sphere • Measures components with NA up to 1 (full hemispheres) • Measures plano, convex, or concave surfaces, OD≤200 mm
Form Talysurf® PGI 1240 and 1250
• Measures dimension, form, and texture on curved surfaces
Nikon 6D Autocollimator
• Prism angle measurement
PrismMaster goniometer®
• Prism angle measurement
Opticentric®
• Centration measurement and alignment
Computer generated holograms (CGH)
• 3D full aperture testing in conjunction with an interferometer • Can create virtually any wavefront shape
Laser centration systems
• Used for aberration-corrected lens assemblies • Enables mechanical re-balancing and pusher cell technology to optimize lens systems
Coordinate measuring machines (CMM)
• Measures microscope objectives and complex lenses in 3D
ZYGO® is a registered trademark of the Zygo Corporation GPI™ and NewView™ are trademarks of the Zygo Corporation Talysurf® is a registered trademark of Taylor Hobson PrismMaster® and Opticentric® are registered trademarks of Trioptics
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PRECISION OPTICS
PRECISION PRISMS Precision in every facet for challenging applications The simplicity of the prism function belies the complexity of its manufacture. Each surface that is polished and coated must also be held in the strictest of angular tolerance to the other surfaces. Prisms bend, fold, invert, reinvert, displace, and deviate light. Though not used as often as lenses and mirrors, prisms are critical components in the systems which utilize their bending or refracting properties. Prisms are challenging to fabricate as each surface and its angular tolerances to the whole are difficult to maintain during polishing and coating. Prism manufacturing requires complex tooling as difficult to manufacture and maintain as the prism itself. In order to collapse or control the optical path, optical engineers may generate designs which require optical contacting of multiple prisms to create complex optical structures. Each angle and surface must be held in the tightest of tolerances to the whole piece. Coatings are similarly difficult, as surfaces may receive different coatings, fixturing is complex, and the final surfaces may need to be completely flat to enable proper contacting, bonding, and alignment to the whole assembly. Prisms types include: Abbe, Amici, Dove, Leman, Penta, Periscope, Porro, Rhomboid, Schmidt, Wollaston and Zeiss. We invest in state-of-the-art metrology to ensure customers receive the highest quality products. G&H has received ISO9001 certification across all of its manufacturing sites and AS9100C certification has been achieved at select facilities. Durability testing can be performed against MIL, DIN, or BSI standards as appropriate. Applications Biomedical, dermatology, fluorescence, laser cavities, laser systems, laser rangefinders, metrology, optical interferometry, optical sights, periscope optics, spectroscopy, targeting.
SPECIFICATIONS
DESCRIPTION
Wavelength ranges
• 240 nm to 5000 nm
Dimensions
• 5-150 mm diameter
Coating options
• • • •
GOOCH & HOUSEGO
Frontside anti-reflection coatings Backside metal coatings Backside protective black coatings for improved handling performance High laser damage threshold coatings
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PRECISION OPTICS
CORNER CUBES Circulators for laser cavities Our high laser damage threshold corner cubes are used in laser range finders to collapse the optical cavity, reduce weight, and improve system performance. Corner cubes comprise three mirrors, or reflective prism faces, which return an incident light beam in the opposite direction. Corner cubes are primarily used in either imaging or laser applications.
IMAGING Corner cubes for imaging applications are used where it is difficult or too timeconsuming to attain precision alignment of the returned beam. The monolithic structure of the component eliminates mounting errors which can arise when using mirrors and is also less sensitive to thermal errors. Such corner cubes are optimized for broadband performance and minimal transmitted wavefront distortion. Corner cubes may be supplied with or without coatings on the reflecting surfaces as they operate on the principles of total internal reflection (TIR). Coatings are recommended in applications where TIR angles are exceeded or the surfaces cannot be kept clean.
Corner cubes
Retro reflector Input / output Beam splitter
LASER CAVITIES Corner cubes from G&H are most often used in laser cavity designs as a circulator. These are often deployed in laser rangefinding applications to keep system size and weight to a minimum. For laser applications, our cubes are optimized for laser damage threshold and minimization of losses (absorption, reflections, transmission, and scattering).
Input / output
Corner cubes improve performance and compress beam paths
G&H has earned ISO9001 and AS9100C certifications. Durability testing can be performed against MIL, DIN, or BSI standards as appropriate. Applications Laser cavities, rangefinding, satellites, spectroscopy, surveying.
SPECIFICATIONS
DESCRIPTION
Wavelength ranges
• 240 nm to 5000 nm
Dimensions
• 5-150 mm diameter
Coating options
• • • •
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Frontside anti-reflection coatings Backside metal coatings Backside protective black coatings for improved handling performance High laser damage threshold coatings
GOOCH & HOUSEGO
PRECISION OPTICS
PRECISION LENSES Unparalleled quality across the spectrum Custom lenses are a key optical component for many transmission and imaging applications in the aerospace, security, defense, machine vision, health care, and life science industries. G&H manufacture custom lenses for imaging, focusing, collimation and illumination, using standard polishing and grinding techniques, as well as single-point diamond turning. We take a design-for-manufacture approach to lens production, facilitating the production of cost-effective, high quality custom lenses. Our lens processing capabilities include CNC generating, grinding, and polishing. We polish spherical, semi-spherical, and aspheric lenses. 5-axis grinding and polishing machines are utilized for the manufacturing high precision aspheric surfaces on optical glass. Single-point diamond turning is used for aspheric and diffractive optical elements.
x
A unique capability for G&H is our ability to manufacture complex shapes on lenses, such as step profiles or off-axis shapes In addition to singlets, we produce a wide variety of doublets, triplets, and more complex lens assemblies. We have made significant investments in metrology equipment to ensure that our customers receive quality, high-performing products. More details on our metrology capabilities can be found at the start of this section and on our website.
z
We offer environmental guarantees for adhesion, abrasion, humidity, temperature. Environmental testing is available on-site, and other tests are available on request. Profile * 4.97 Zones * 0.309
Applications Dental imaging, dermatology, endoscopy, hyperspectral imaging, lasers, machine vision inspection, metrology, optometry, projection, rangefinding, reconnaissance, surveillance, target identification, targeting and designating, thermal imaging.
Examples of single diamond point turned profiles on spherical and aspherical lens surfaces
VISIBLE THROUGH INFRARED – 400 nm-14 μm
VISIBLE ONLY
INFRARED ONLY – 3-14 μm
SPECIFICATIONS1
SPHERICAL
ASPHERICAL
CYLINDRICAL
ASPHERIC/DIFFRACTIVE/ HYBRID
Substrate material
• All optical glasses
• All optical glasses
• All optical glasses
• Ge, Si, ZnS, ZnSe, chalcogenides
Diameter ranges
• Up to 200 mm
• Up to 60 mm
• Up to 200 mm
• Up to 250 mm
Thickness ranges
• Up to 100 mm
• Up to 100 mm
• Up to 100 mm
• Up to 100 mm
Surface quality
• 40-20 to 5-2
• 20-10
• 20-10
• 20-10
Surface accuracy (conventional polishing)
• λ/10
• λ/10
• λ/10
• λ/10
Surface accuracy (MRF)
• λ/40
• λ/20
• λ/20
• λ/20
Dimensional tolerance
• ±0.005 mm
• ±0.005 mm
• ±0.005 mm
• ±0.005 mm
Radius
• 2.0 m to infinity
• 2.0 m to infinity
• 2.0 m to infinity
• 2.0 m to infinity
AR coatings
• High laser damage threshold • High transmission • Broadband or V-coat anti-reflection
• High laser damage threshold • High transmission • Broadband or V-coat anti-reflection
• High laser damage threshold • High transmission • Broadband or V-coat anti-reflection
• High transmission • Broadband or V-coat anti-reflection
1 Actual specifications are dependent upon design, geometry, and material. Please talk to an applications engineer early in your design process to capture the most value from our design-for-manufacture approach.
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PRECISION OPTICS
SWIR LENS ASSEMBLIES Customized solutions for VIS-SWIR imaging applications G&H engineers precision visible – short-wave infrared (SWIR) lens assemblies for demanding custom applications in commercial and military aerospace, defense, industry, life sciences, and scientific research. Our lens modules are specifically designed for operation at visible and/or SWIR wavelengths, leveraging the benefits of the new, larger InGaAs detectors. Considered selection of lens system parameters, materials, and coatings improve resolution, accuracy, and exposure times; criteria which are critical in low light situations.
OPTIMIZED STANDARD LENS DESIGNS G&H has developed a series of high precision lens systems for a wide variety of short-wave infrared (SWIR) imaging applications. The lens design, material selection, and coatings for each lens are optimized for high resolution, high signal to noise, and high performance in low light conditions. Our SWIR/VIS-SWIR lens modules are fully environmentally qualified as athermalized, shock and vibration proof and waterproof. • • •
The Barle lens is optimized for InGaAs camera applications. The large field of view is designed to work with the latest InGaAs detection systems. The Avill high resolution VIS-SWIR lens is optimized for short focal length applications and a wider spectral range than the Barle. The Isle is a lightweight, high performance, compact VIS/SWIR continuous electronic zoom lens. It is athermalized and militarized for integration into fixed wing, rotary, and tracked or wheeled vehicle platforms.
SWIR lenses for InGaAs cameras for machine vision and security applications
Design-for-manufacture approach and extensive metrology tools enable G&H to provide superior value for precision lens assemblies
F/1.4 SWIR lens – ray trace diagram
STANDARD LENS PRODUCTS PRODUCT FAMILY
PRODUCT CODE
WAVELENGTH
FOCAL LENGTH
IRIS RANGE
CLEAR APERTURE
FIELD OF VIEW
FOCUSING RANGE
Barle
RD3348
900-1700 nm
25 mm
F1.4-F16
0.5”, 2/3”,1”
55°
0.7-infinity
Avill
RD3346
550-1700 nm
12.5 mm
F1.8-F16
68°
0.7-infinity
Isle
RD3347
550-1700 nm
40-200 mm
F3.6
3.63-18.38°
0.7-infinity
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CUSTOM LENS ASSEMBLIES FOR VIS TO LWIR APPLICATIONS
• • •
Custom bonded multi-element optical components Mounted optical assemblies Modules with integrated electronics for use at visible through long-wave infrared (LWIR) wavelengths
We provide stringent controls and documentation required for military and defense applications, working between multiple facilities to meet export legislation requirements, and quality requirements (ISO 9001, AS9100C) on multi-decade programs.
0.9
Modulator transfer function
G&H design and develop custom lens assemblies for a wide variety of custom applications. Designs developed by G&H include:
MTF Chart Showing (SWIR) Lens Quality 1
0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0 0
5
10
15
20
25
Spatial frequency/line pairs per mm T&S center of field
Tan 6 mm from center
Sag 6 mm from center
Tan 9 mm from center
Sag 9 mm from center
Applications Hyperspectral imaging, optical coherence tomography, machine vision inspection, rangefinding and designating, reconnaissance, surveillance, SWIR imaging, targeting, thermal imaging, visible imaging.
SPECIFICATIONS
CUSTOM LENS ASSEMBLIES
Lens Complexity
• From singlets in a housing to large diameter zoom lenses
Materials
Material selection optimized for application: • Wavelength range (UV, VIS, NIR, SWIR, LWIR, FIR) • Zoom • Weight
Coatings
• Optimized for the sensor and design criteria • Narrowband or broadband across the UV – VIS – FIR spectrum
Design Origins
• Build-to-print to customer design • G&H In-house design to customer application specifications
Metrology
• Single elements – Transmitted wavefront distortion – Surface quality – Transmission • Assemblies – MTF
Especially optimized for
• Abrasive environments • High long-term stability • Athermalization for operating temperature range
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PRECISION OPTICS
PRECISION MIRRORS High energy performance for laser cavities and applications Custom high-reflectivity mirrors deliver superior performance and value to customers designing and building laser cavities from small, lightweight rangefinding lasers to high laser damage threshold industrial lasers. Discerning customers understand that the smallest defect leads to a system failure. Our goal is to minimize or eliminate system failures due to coating or polishing defects. Dielectric laser cavity and beam routing mirrors demonstrate very high reflectivity and high laser damage threshold. Protected and enhanced metal reflector coatings offer superior abrasion and climatic resistance for lower power applications. To ensure performance in the field, we leverage extensive metrology capabilities to qualify every component at every step in the manufacturing process. Environmental testing of components and coatings is critical for assurance of performance in rugged conditions. G&H environmental testing capabilities include MIL-C-675C, MIL-C-48497A, MIL-E-12397, and MIL-M-13508C for endurance against abrasion, adhesion, humidity, temperature, and environmental conditions. G&H has received IS09001 certification across all of its manufacturing sites and AS9100C certification has been achieved at select facilities. Applications Laser cavities, laser rangefinders, target designators.
MIRROR OPTIONS Typical substrate shapes
• • • • •
Coatings
• High laser damage threshold dielectrics • Protected metal – Aluminum – Gold – Platinum – Silver • Enhanced metal – Aluminum – Gold – Silver
Other coating options
• Front surface • Back surface
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Optical grade flats Spherical Rectangular Square Parabolic
GOOCH & HOUSEGO
PRECISION OPTICS
SYNCHROTRON MIRRORS Research Grade Mirrors and Flats As the original provider of superpolished optical components, G&H has been producing superpolished surfaces for over 40 years. Our proprietary process serves high volume production requirements as well as small volume, specialized applications. Superpolished substrates feature surface roughness lower than 1 Å, scratch-dig <5-2, and inspection criteria of up to 320x magnification. The results are low scattering losses and significantly fewer defects. Substrates demonstrate an impressive λ/20 or better surface accuracy. Most of our synchrotron optics and research grade flats are supplied with polished or acid-etched diameters and bevels. These extra touches add to the level of cleanliness and durability that can be achieved.
High heat load from synchrotron sources require superpolished silicon substrates
To complement our superpolished surfaces, we offer ion beam sputtered (IBS) coatings which provide very low levels of total loss (absorption and scatter) and exceptional environmental stability. Our custom optics have enabled scientists to achieve prize-winning results in LIGO, NASA’s Mars Curiosity Sky Crane, and in synchrotron facilities around the world. State-of-the-art metrology ensures customers receive the highest quality product. G&H has earned ISO9001 and AS9100C certifications.
Applications DUV experiments, high-energy applications, interferometry, laser and X-ray research, reference standards, synchrotron mirrors, ultra-fast laser systems.
SPECIFICATIONS
SYNCHROTRON MIRRORS
RESEARCH GRADE FLATS AND MIRRORS
Substrate material
• Silicon
• Fused silica, silicon carbide, Zerodur®
Coating wavelength ranges
• 355 nm-3.2 μm
• 355 nm-3.2 μm
Sizes
• 2 mm-500 mm
• 1 mm-500 mm
High surface quality
• <5-2 scratch-dig, <1 Å surface roughness
• <5-2 scratch-dig, <1 Å surface roughness
Wavefront distortion
• Up to 1/50th wave at 633 nm
• Up to 1/50th wave at 633 nm
Dimensional tolerance
• Sub-micron
• Sub-micron
Angular tolerances
• <1 Arc second
• <1 Arc second
Clear aperture dimensions
• Up to 500 mm
• Up to 500 mm
Mounted or unmounted
• Optically contacted, bonded, adhesive-free, customer specified
• Optically contacted, bonded, adhesive-free, customer specified
Slope error
• <0.5 μRad
• <0.5 μRad
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PRECISION OPTICS
PLATE AND CUBE BEAMSPLITTERS Accurate solutions for high energy applications Optimized beamsplitter designs from G&H demonstrate superior laser damage performance for each unique wavelength, split, and incident angle combination. Cube beamsplitters can divide the incident beam based on polarization (S or P) or power (ratio of energy into each arm). They are easy to mount and mechanically durable. Cube beamsplitters from G&H may be provided cemented, optically contacted, or even air-spaced. For some applications, higher power handling and lighter weight is required. Plate beamsplitters display intrinsically higher beam power handling capability than cube beamsplitters. Plate varieties are preferred in high laser energy applications, or where cost or weight limits on the assembly come into play. However, the physics of the plate beamsplitter operation generates a beam offset dependent upon the thickness of the substrate. An anti-reflection coating on the exit surface of the substrate can minimize the ghost beam.
Cube beamsplitters are durable and minimize ghost beams
Beamsplitter types and selection factors Selection of the appropriate beamsplitter design is dependent upon several factors: • • • • • • •
Polarizing or non-polarizing Non-polarizing beam ratio (examples may be 50-50, 70-30, 90-10) Wavelength separation Power handling (high power or high incident laser energy) Ghost reflection tolerance Beam displacement tolerance Cube or plate
Beamsplitter coating
Plate beamsplitter
Plate beamsplitters are smaller, lightweight, and intrisically handle higher power
G&H has received IS09001 certification across all of its manufacturing sites and AS9100C certification has been achieved at select facilities. Applications Biomedical, dermatology, fluorescence, laser cavities, laser systems, laser range finders, metrology, optical interferometry, spectroscopy, targeting.
SPECIFICATIONS
PLATE
CUBE
Wavelength ranges
• 240 nm to 5000 nm
• 240 nm to 5000 nm
Dimensions
• 5-150 mm diameter
• 5x5x5 mm to 50x50x50 mm typical
Beamsplitting options
• • • •
• • • •
Coating options
• E-beam dielectric optimized for LIDT • Backside AR coating to minimize ghosting • Low phase shifting coating designs
Assembly options
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Polarizing or non-polarizing Beam ratios from 90-10 to 50-50 Wavelength separation Long pass or short pass
Polarizing or non-polarizing Beam ratios from 90-10 to 50-50 Wavelength separation Long pass or short pass
• E-beam dielectric optimized for LIDT • Cemented • Optically contacted • Air-spaced
GOOCH & HOUSEGO
PRECISION OPTICS
WINDOWS AND OPTICAL FLATS Custom solutions for environmentally challenging conditions Optical windows are a critical component in a variety of applications which require minimal optical impact with maximum mechanical separation between two environments.
WINDOWS FOR INDUSTRIAL APPLICATIONS Optical windows are utilized in lasers, testing chambers, and other systems where the environment on one side may be pressurized, filled with a specific gas, or otherwise need to be chemically separated from the other. The window needs to transmit the photon energy with minimal disruption (highest transmission, lowest absorption and scattering, and minimal polarization or optical path distortion). Highest quality optical windows from G&H demonstrate very high parallelism, supremely low surface roughness, low transmitted and reflected wavefront errors, and are optical transparent at the operational wavelength range. Window material is chosen based on environmental factors such as acidity of atmosphere, strong vacuums, high pressures, or high temperatures and the operational wavelength range.
WINDOWS FOR DEFENSE APPLICATIONS Defense-grade windows from G&H are significantly larger and may be coated with diamond-like coatings to withstand abrasive environments in the desert. Window thickness is determined by environmental factors: pressure differentials, thermal conditions, and mounting mechanics. G&H has received ISO9001 certification across all of its manufacturing sites and AS9100C certification has been achieved at select facilities. Durability testing can be performed against MIL, DIN, or BSI standards as appropriate. Applications Biomedical instrumentation, corrosive chemistry, directed energy experiments, industrial instrumentation, IR imaging, laser cavities, machine vision, multiphoton imaging.
1
SPECIFICATIONS1
INDUSTRIAL
DEFENSE
Coating options
• High laser damage threshold • High transmission • Broadband or V-coat anti-reflection
• Broadband or V-coat anti-reflection • Diamond-like coatings for abrasion resistance
Substrate materials
• Ge, ZnS, ZnSe, common glasses, fused silica, glass ceramics
• Ge, ZnS, ZnSe, common glasses, fused silica, glass ceramics
Sizes
• Typical 3 mm to 300 mm
• Up to 450 mm
Especially optimized for
• High energy • Transmission at high angles • High temperature stability
• Abrasive environments • Transmission in high angles • High long-term stability
Environmental testing
• Humidity, sea salt spray, DIN, MIL upon request
• Humidity, sea salt spray, DIN, MIL upon request
Actual specifications are dependent upon design, geometry, and material choices.
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PRECISION OPTICS
WAVEPLATES Superior polarization control across the spectrum From crystal growth, crystal orientation and cutting, to waveplate fabrication and coating, no other waveplate supplier has as much control over the fabrication stages as G&H. For all wavelength ranges, we orient, cut, and polish the optical crystals for waveplate production. Tight internal controls enable better retardation tolerances within and between production runs. Polishing, coating, assembly, and metrology complete the manufacturing process. Compound zero-order (also known as net-zero order) and achromatic waveplates are often optically contacted to reduce reflection losses at the surfaces. Air-spacing is recommended for high energy applications. Specialty waveplate designs such as offaxis or true-zero order waveplates are produced to custom specifications. G&H has received IS09001 certification across all of its manufacturing facilities. AS9100C certification has been achieved at select facilities.
WAVEPLATES FROM THE UV TO THE NIR From crystal orientation to assembled product, we produce cutting-edge waveplates for a varied range of applications and customers. • • • • • •
Applications Aerospace, astronomy, biomedical, laser power control and attenuation, military, optical isolation, polarimetry, remote sensing, semiconductor metrology, spectroscopy, surveillance.
Crystal Quartz – standard material for UV-NIR waveplate applications LiNbO3 – infrequently used in 1.5 μm applications and optical frequency shifters MgF2 – typically used in combination with crystal quartz for achromatic waveplates Mica – for ophthalmology applications Sapphire – for defense applications in extreme environmental conditions YVO4 – waveplates for the 400 nm to 5 μm ranges
WAVEPLATES FOR THE IR, HIGHER ENERGIES, OR LARGER FORMATS As the world’s only entirely vertically integrated CdS, CdSe, and KDP waveplate producer, we deliver accurate performance for demanding applications. Our control over crystal growth benefits customers who need larger sizes, high laser damage threshold performance, or more accurate retardation tolerances.
1
CRYSTAL GROWTH • CdS, CdSe • KDP and KD*P
CRYSTAL GROWTH
CdS, CdSe KDP and KD*P
1
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CRYSTAL GROWTH CdS, CdSe KDP and KD*P
2
CRYSTAL ORIENTATION • Internal controls deliver accuracy and consistency
2 2
CRYSTAL ORIENTATION
Internal controls deliver accuracy and consistency
CRYSTAL ORIENTATION Internal controls deliver accuracy and consistency
3
4
• UV, VIS, NIR AR • 3-5, 5-8, 8-13 mm • Custom
• Standard and custom housings • Air-spaced or optically contacted
COATING
3 3
COATING
UV, VIS, NIR AR 3-5, 5-8, 8-13 mm Custom
COATING UV, VIS, NIR AR 3-5, 5-8, 8-13 mm Custom
ASSEMBLY
4 4
ASSEMBLY
Standard and custom housings Air-spaced or optically contacted
ASSEMBLY Standard and custom housings Air-spaced or optically contacted
GOOCH & HOUSEGO
PRECISION OPTICS
Two waveplates manipulating the polarization of light
1
VISIBLE AND NIR SPECIFICATIONS
UV, VIS, NIR MULTIPLE ORDER, NET-ZERO, DUAL
UV, VIS, NIR ACHROMATIC
UV, VIS, NIR HIGH ENERGY
Substrate material
• Crystal quartz
Crystal quartz & MgF2
KDP or KD*P
Sizes
• 5-150 mm
• 5-50 mm
• 5-430 mm
High surface quality
• 10-5
• 40-20 typical
• 10-5 for substrates less than 20 mm in diameter • 20-10 for substrates less than 430 mm in diameter
Retardation tolerance
• λ/500 at 23°C at 633 nm
• λ/72 at 23°C
Operating conditions
• 10 J/cm2, 20 ns pulse, 20 Hz
• 10 J/cm2, 10 ns pulse at 1064 nm
Transmission
• 99.9%
• 99%
• 99%
Transmitted wavefront
• λ/10 at 633 nm
• λ/10 at 633 nm
• λ/6 at 633 nm
Parallelism
• <0.5 arc sec
• <0.5 arc sec
• <15 arc sec
INFRARED SPECIFICATIONS1
IR MULTIPLE ORDER SINGLE WAVELENGTH (3 µm-12 µm)
IR NET ZERO ORDER NARROW RANGE (3 µm-12 µm)
ACHROMATIC 3-5 µm, 5-8 µm OR 8-12 µm
Substrate material
• CdS or CdSe
• CdS/CdS or CdSe/CdSe
• CdS/CdSe
Sizes
• 4-29 mm
• 4-29 mm
• 4-29 mm
Retardation tolerance
• ± 5° at design wavelength
• ± 5° at design wavelength
• ± 10°
Transmission
• >97% at design wavelength
• >90% at center wavelength
• >90% at center wavelength
Custom wavelength ranges available
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PRECISION OPTICS
SUPERPOLISHED SROC High quality superpolished short radius of curvature optics Gooch & Housego has been producing superpolished surfaces for over 40 years and is the world’s original provider of superpolished optical components. We have evolved our proprietary process to handle high volume and specialized R&D requirements. Superpolished substrates feature surface roughness lower than 1 Å, scratch-dig <5-2, and inspection upwards of 320x magnification. The result is extremely low scatter, losses and defects – a requirement for any high performance laser application. The substrates offer an impressive λ/20 or better surface accuracy. In keeping with the high standards of our superpolished surfaces, most of our optics are supplied with polished or acid etched diameters or bevels. These extra touches add to the level of cleanliness and durability that can be achieved. To complement our superpolished surfaces we offer ion beam sputtered (IBS) coatings which achieve very low levels of total loss (absorption and scatter), and exceptional environmental stability. G&H has received IS09001 certification across all of its manufacturing sites and AS9100C certification has been achieved at select facilities. Applications Cavity enhanced absorption spectroscopy, ring laser gyroscopic systems, ultrafast laser research, ultraviolet laser systems.
SPECIFICATIONS Substrate materials
• BK7, crystal quartz, fused silica, Zerodur®.
Sizes
• 2-400 mm
Surface quality
• Scratch-dig <5-2, <1 Å
Wave front distortion
• λ/20 @ 633 nm
Dimensional tolerance
• Sub-micron
Angular tolerances
• <1 arc second
Clear aperture dimensions
• Up to 400 mm
Mounted/unmounted
• Optically contacted, bonded, adhesive-free, customer specified
Radius of curvature
• >20 mm
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RING LASER GYROSCOPE COMPONENTS Delivering precision and complexity for navigation-critical components Vertical integration enables G&H to supply the entire ring laser gyroscope (RLG) package: RLG frame and optical components. Our integration of capabilities delivers superior performance and streamlines sourcing. There are many components within the ring laser gyroscope; each performs unique functions and is optimized accordingly. The Zerodur® frame must deliver maximal stability over a large range of operating environments (namely, temperature, humidity, and environmental composition). We have 40 years of experience producing high-quality, consistent, Zerodur® frames. Flat, wedged, and curved mirrors used in RLGs are superpolished with surface roughness better than 1 Å RMS with high-reflectivity low-loss IBS coatings designed to survive extreme environmental conditions.
Mirror Fringe pattern
Anode Gas discharge region
Precision beam splitters, prisms, and wedges complete the assembly. Readout detector
Extensive metrology capabilities are critical to the abilities of G&H to meet and exceed difficult specifications. • • •
Zygo® ZeMapper™ for surface roughness and structure <1 Å OGP® CMM for geometrical tolerances down to sub-micron features 18” Zygo® Interferometer measures flatness up to λ/50
Corner prism
Cathode
Light Beams
G&H facilities are certified to ISO9001 and AS9100: 2009 Rev.C. G&H businesses comply with ITAR legislation and are registered with the US government.
Piezoelectric dither mirror
Anode
Schematic of optical components produced by G&H for RLG assemblies
Applications GPS, hyperspectral imaging, infrared microscopy, laser scanning microscopy, metrology, optical failure analysis for semiconductor processing, rangefinding, reconnaissance, surveillance, target identification, targeting and designating, thermal imaging.
1
SPECIFICATIONS1
ZERODUR® FRAMES
RLG MIRRORS
RLG BEAM COMBINERS
RLG PRISMS & WEDGES
Substrate materials
• Zerodur®
• Zerodur®, fused silica
• Fused silica
• Fused silica
Sizes
• 1-500 mm
• 1-500 mm
• 1-500 mm
• 1-500 mm
Surface Roughness
• <1 Å
• <1 Å
• <1 Å
• <1 Å
Wavefront distortion
• λ/50 @ 633 nm
• λ/50 @ 633 nm
• λ/50 @ 633 nm
• λ/50 @ 633 nm
Dimensional tolerance
• Sub-micron
• Sub-micron
• Sub-micron
• Sub-micron
Angular tolerances
• <1 arcsecond
• <1 arcsecond
• <1 arcsecond
• <1 arcsecond
Clear aperture dimensions
• Up to 500 mm
• Up to 500 mm
• Up to 500 mm
• Up to 500 mm
Actual specifications are dependent upon design, geometry, and choice of material.
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PRECISION OPTICS
INFRARED OPTICS Integrated fabrication capabilities Our combination of technical skills, manufacturing competencies, and metrology capabilities enable G&H to deliver highly integrated, superior performing optical components. G&H brings together a set of capabilities which enable our customers to combine techniques, even on the same part. G&H utilizes several techniques (high precision CNC processing, diamond turning, magnetorheological finishing, and traditional polishing) either separately or in tandem to achieve superior product specifications, such as surface accuracies to better than 100 nm. One of our distinguishing capabilities is our ability to manufacture complex shapes on lenses, such as step profiles or off-axis shapes. Durable antireflection (AR) coatings from G&H are tailored to the application. Typical AR coatings include: Broadband, V-coat, and dual band. Broadband coatings perform well from 400-14000 nm wavelength ranges. Reflectivity as low as 0.25% for the 3-5 μm range is achievable. Extensive metrology capabilities are critical to the abilities of G&H to meet and exceed difficult specifications. •
QED SSI® stitching interferometry measures aspherics, full hemispheres, and OD up to 200 mm Taylor Hobson contact metrology tools measure surface roughness and surface accuracies up to 60 nm NewView™ 5000 white light interferometer is use for surface analysis and micro-roughness down to 2 Å RMS Computer generated holograms (CGH) can be utilized for volume production and high precision surface measurement.
• • •
G&H has received IS09001 certification across all of its manufacturing sites and AS9100C certification has been achieved at select facilities. Applications Hyperspectral imaging, infrared microscopy, laser scanning microscopy, metrology, optical failure analysis for semiconductor processing, rangefinding, reconnaissance, surveillance, target identification, targeting and designating, thermal imaging.
SPECIFICATIONS1
1
Substrate materials
• ZnSe, ZnS, Ge, CaF2, MgF2, AMTIR, chalcogenides, silicon, sapphire
Sizes
• 3-250 mm
Surface roughness (Å, RMS)
• 10
Surface accuracy
• λ/20
Scratch-dig
• 10-5, material dependent
Optimized for
• Abrasive environments • Transmission in high angles • High long-term stability
Environmental testing
• Humidity, sea salt spray, DIN, MIL
Actual specifications are dependent upon design, geometry, and choice of material.
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PRECISION OPTICS
OPTICAL DOMES IR domes for aerospace and defense
NEW
CNC processing, combined with extensive metrology capabilities, deliver precision domes for aerospace and military applications. Optical domes are essentially windows: two parallel surfaces, curved. The dome protects and isolates critical sensors and electronics from the environment with minimal disruption to the optical path. High numerical aperture (NA) optical domes from G&H are produced using precision tooling. This new capability features zinc selenide, zinc sulphide, or germanium materials. To ensure performance in the field, we leverage our extensive metrology capabilities to qualify every component at every step in the manufacturing process. Optical domes are difficult to measure; therefore, we have developed proprietary stitching interferometry processes to minimize errors due to reflections. Environmental testing of components and coatings is critical for assurance of performance in rugged conditions. Environmental testing capabilities include MILC-675C, MIL-C-48497A, MIL-E-12397, and MIL-M-13508C for endurance against abrasion, adhesion, humidity, temperature, and environmental conditions. G&H has received IS09001 certification across all of its manufacturing sites and AS9100C certification has been achieved at select facilities.
Applications FLIR, seeker head optics, submersibles, underwater cameras.
SPECIFICATIONS1
1
Substrate materials
• Ge, ZnS, ZnSe
Sizes
• 75-200 mm
Material thickness
• ≥4 mm
Surface figure
• 2 fringes with power x 0.5 fringes irregularity over 100 mm diameter @ 633 nm
Dimensional tolerance
• 0.1 mm
Parallelism
• 30 arc seconds
Coatings
• AR coatings for VIS, NIR, MWIR, LWIR, broadband
Especially optimized for
• Abrasive environments • Transmission in high angles • High long-term stability
Environmental testing
• Humidity, sea salt spray, DIN, MIL
Actual specifications are dependent upon design, geometry, and choice of material.
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PRECISION OPTICS
ELECTRO-OPTIC SIGHTING SYSTEMS Vision systems for armored fighting vehicles An international supplier of electro-optic sighting solutions (EOSS) and unity vision periscopes, sighting solutions, and related equipment for armored fighting vehicles (AFVs), Kent Periscopes (a Gooch & Housego company) supplies all of the major AFV integrators and major turret sub-systems vendors around the world. Our designs include: • • • • •
Sabre Sighting Systems with long-wave infrared (LWIR) thermal imaging Day/night vision Embedded Image Periscopes (EIPs) combine images and video Passive Driver Periscopes (PDPs) for hatch down, night driving Unity vision periscopes Spares, repairs, and drop-in replacement designs
Our EOSS are offered with a range of optional features, built to a proven build standard, and qualified for performance in the field.
DESIGN, PRODUCTION, SPARES AND REPAIRS We design optimized solutions taking into account a wide range of constraints and variables such as: space envelope, interface definition, fields of view, and user positioning. We can modify existing products as well as develop entirely new, custom designs. New designs can be turned quickly into evaluation units using rapid prototyping techniques. 3D solid models are generated for ‘virtual’ fitting providing: ground intersect calculations, polar maps to check for obscuration, and 3D accommodation of in situ positioning of equipment. Design, manufacturing, and assembly services are available in the UK and the US, meeting all export controls. We offer repair and refurbishment services for a range of in-service optical equipment. Kent Periscopes has received IS09001 certification.
Above from top: Unity vision, Embedded Image and Sabre class periscopes
PRODUCT
PRODUCT CODE
DESCRIPTION
Unity vision periscopes
K2LU20
Constructed with two glass prisms, a separate, desiccated air-gap provides additional ballistic protection. Fits into M27 space, using same mounting brackets.
K6
Simple single ‘mono block’ glass prism, similar to acrylic variants. Fits into same space, using same mounting brackets as M17.
T1 or T2
T1, unity vision driver's periscope. T2, a narrower version, installs alongside the T1 to maximize the horizontal azimuth field of view.
T6
Multiple units, installed adjacent to each other, in driver’s position, provide a virtually uninterrupted, panoramic horizontal field of view.
SABRE NGS
Tall, narrow periscope, with dual field of view, and custom graticule that can be boresighted with azimuth and elevation adjustment.
Biocular EIP
Provides standard unity vision functionality for normal daytime viewing plus the ability to display digital images from range of on-vehicle sensors and cameras.
EIP BVM
Provides the user with a relaxed view of video images obtained from cameras and sensors located on the outside of the vehicle minimizing eye strain.
EIP DMM
Designed for small space envelopes to display digital image feeds.
Sabre Commander/ Gunner Sights
SABRE Ti
Uncooled, ITAR-free, LWIR thermal imaging solution for gunner or commander.
Other products
PDP
Single micro-channel plate image intensifier tube and biocular eyepiece with automatic brightness control.
Vision Blocks
Vision solution with ballistic and laser protection.
Embedded Image Periscopes
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LMI INSTRUMENTATION Gooch & Housego has more than 45 years of experience in photonics system design and manufacturing. We are the supplier of choice for test and measurement instruments in leading R&D laboratories as well as the solid-state and LED lighting, automotive lighting, avionics, and display industries.
Capabilities
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Product Overview
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Test and Measurement
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INSTRUMENTATION
TECHNICAL EXPERTISE AND MANUFACTURING CAPABILITIES G&H’s instrumentation division is recognized worldwide as the leading expert in spectroradiometry for both instrumentation and calibration services (specifically measurements from 200 nm to 30 µm). ENGINEERING AND DESIGN CAPABILITIES
G&H designs, engineers, and manufactures commercial off-the-shelf (COTS) light measurement instrumentation for spectroradiometry, colorimetry, and photometry, as well as hyperspectral imaging systems. Our instruments enable precision light measurement for defense and security, industrial, and life science applications.
• • •
Our instruments and systems provide accurate, repeatable, NIST-traceable, research-grade measurements in the UV-VISNIR-IR wavelength ranges for research, academia, industry, and the military. Our light measurement systems are designed to provide consistent, precise, and repeatable measurements throughout the life of the instrumentation.
• •
Our spectroradiometers are used for testing night vision compatibility, LED, OLED, IRED and display measurements, detector spectral response, internal and external quantum efficiencies, and more. We offer spot and imaging colorimeters for highly accurate luminance and color measurements, and radiometers/photometers for total luminance, illuminance, and broadband radiance and irradiance measurements. Our hyperspectral/multi-spectral imaging systems are used in life science research and stand-off detection.
PRECISION CONTRACT MANUFACTURING G&H offers full product engineering, design, and manufacturing of optomechanical and photonics systems at our ISO 9001:2008 certified instrumentation systems division. Our engineers have extensive experience with demanding commercial product delivery, as well as customer designed and OEM solutions for light measurement applications and requirements.
• •
• • •
CE compliant design Current source precision regulation Custom electro-optical/mechanical design and development Digital signal processing/image processing Extremely low level detection technology (1 fA, 1 nV resolution) Integrating sphere technology ISO 9001 engineering, project management and documentation structure Optical modeling/systems design Precision motion control Windows®, Mac® and embedded software development capabilities
CALIBRATION AND TEST SERVICES Our NIST-traceable calibration, measurement, and test services include spectroradiometric calibration, characterization of detectors and light sources, and supply/ recalibration of calibration standards. We also supply spectroradiometric standards and power supplies, from spectral irradiance/illuminance standards and spectral radiance/luminance standards to detector standards. We are an ISO/IEC 17025 accredited facility.
Specialized facilities include those for diffuse reflectance coating and electro-static discharge (ESD) assembly. From precision optomechanical and electronics assembly to systems level integration and test, our OEM solutions are supported by manufacturing enterprise and supply chain management systems, and validated by NIST-traceable test and calibration services.
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INSTRUMENTATION
PRODUCT OVERVIEW Components and instruments for spectroradiometry We offer products and custom solutions for highly challenging program requirements, drawing on our depth of expertise and vast experience in optics, mechanics, electronics, software, firmware, photonics, and systems integration. Our flexible production facilities can accommodate demanding commercial and quick-turn production, as well as custom designed and OEM solutions.
STANDARDS Our integrating sphere standards are designed for accurate instrument calibration (photometric, radiometric, or spectroradiometric response) with manual and motorized, computer-controlled variable apertures. We provide high-accuracy irradiance standards based on the NIST spectral irradiance scale. Specular and diffuse reflectance standards are available for use in bi-directional reflectance distribution factor (BRDF) applications, and as targets for irradiance to radiance conversion.
OL-458-4F White LED-Based Fixed Luminance Sphere Calibration Standard
DETECTORS G&H manufactures a range of detectors. Available technologies include extended InGaAs, Ge, HgCdTe, InGaAs, InSb, PbS, PbSe, PMT, pyroelectric, Si. NIST-traceable calibration of these detectors can be provided to support spectroradiometry systems configured to spectrally characterize the response of sensors, focal plane arrays (FPA) and cameras, as well as solar cells.
OL 455-6KSA Ultra-High Uniformity Calibration Standard
INTEGRATING SPHERES We provide integrating spheres in a range of sizes, as well as a multitude of baffle and port configurations, to meet any source or input optic requirement. Sphere coatings for applications in the UV through IR wavelength ranges are available.
COLORIMETERS/PHOTOMETERS G&H has developed a line of rugged, compact colorimeter/photometers for use in industrial environments. Our manual tristimulus colorimeter/photometers serve the needs of high-speed production line and QC inspection, as well as product development. The MANTIS Imaging Colorimeter/Photometer delivers ultra-fast high resolution spatially resolved measurements of luminance, chromaticity, and color temperature for full field measurements of automotive and aerospace lighting and displays in high speed production test environments.
GOOCH & HOUSEGO
OL IS-1800H 18-Inch Integrating Sphere (with vertical opening)
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INSTRUMENTATION
SCANNING SPECTRORADIOMETERS PRODUCT CODE
WAVELENGTH
FEATURES
OL750
0.20-30 μm (depending on model)
• Source analysis (irradiance or radiance), transmittance, specular reflectance, diffuse reflectance, and detector response • Entirely computer-controlled
OL756
200-800 nm
• Extremely low stray light levels • Built-in overload feature to protect the highly sensitive photomultiplier (PMT) cathode from saturation • USB interface, auto-ranging PMT signal acquisition system
OL750-NVG
380-930 nm
• Complete turnkey system for spectroradiometric and photometric certification of night vision (NVIS) compatible lighting devices • Exceeds MIL-L-85762A and MIL-STD-3009 requirements
MULTI-CHANNEL SPECTRORADIOMETERS PRODUCT CODE
WAVELENGTH
FEATURES
OL770 LED Series (LED Measurement)
200-800 nm
• Designed for solid state and other lighting sources and fully compliant with CIE 127 • Wavelength accuracy of 0.5 nm • Can measure luminaires up to approximately 1.2 m long when coupled to our spheres ≥2 m, full automated integrating spheres • Software development kit for integration with production and materials handling systems • High-speed USB interface • Ability to create custom Word and Excel report templates
OL770 DMS Series (Display Measurement)
200-800 nm
• • • •
OL770-NVS System (Night Vision Display Test and Measurement)
380-1100 nm
• Fast, multi-channel measurements of spectral radiance, luminance, chromaticity, NVISa and NVISb • Powerful user-friendly software, precise direct viewing imaging optics, and DSP technology • Fast, multi-channel measurements of spectral radiance, luminance, chromaticity, NVISa and NVISb • Pass/fail results per MIL-L-85762A and MIL-STD-3009 requirements
OL770-InGaAs (High-speed, Multi-channel Spectroradiometer)
850–1700 nm
• Modular design for easy integration with 770 series to cover an even wider spectral range with same accessories • Applications include chemometrics, determining atmospheric absorption, solar simulation, and IRED source measurements
OL 756 Portable UV-VIS Spectroradiometer
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Accurate color, luminance and spectral information of displays Picture of measurement area provided and may be stored with data Custom field of views (FOVs) available Capable of diffuse and specular reflectance measurement and sunlight readability following ICDM IDMS1 in both a manual and automated positioning configuration • 770-ADMS version for results in .ies format
OL 770-LED Test and Measurement System
OL 770-DMS Display Measurement System
GOOCH & HOUSEGO
INSTRUMENTATION
TEST AND MEASUREMENT Services Using high accuracy standards and precise optical instrumentation our engineers can perform a full range of NIST-traceable measurement services. From C.I.E 127 to LM-79/LM-80, IEC 62471 to VESA and IDMS, we offer comprehensive test and measurement solutions at our ISO/IEC 17025 accredited facility. Measurement services for source spectral analysis include: • • • • • • • • • • • • • • • •
Average luminous intensity (candelas) – Average radiant intensity (watts/sr) Color purity – Correlated color temperature (CCT) Color rendering indices – Chromaticity coordinates Color rendering indices (CRI) – Relative power External quantum efficiency Half bandwidth – Correlated color temperature (CCT) Maximum intensity – Chromaticity values Night vision compatibility (NVIS) (MIL-STD 3009 and MIL-L-85762A) Peak wavelength – Dominant wavelength Photobiological hazard assessment: UV/thermal (IEC 62471) Peak wavelength – Half-bandwidth Photosynthetic active radiation (PAR) 2 2 Spectral irradiance (W/cm ) – Illuminance (lm/cm ) 2 2 Spectral radiance (W/cm /sr/nm) – Luminance (lm/cm /sr) Total radiant flux (W) – Total luminous flux (lm) – Total spectral flux (W/nm) Tristimulus values – Lab/Luv values
In addition to source spectral analysis, we also have the capability to provide the following services: • • • • • •
Detector spectral response (including FPAs and IR Cameras) Solar cell spectral response and quantum efficiency Diffuse and specular reflectance Linear and divergent/diffuse transmittance Goniometric reflectance and transmittance (intensity vs. angle) Lumen maintenance
GOOCH & HOUSEGO
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CONTACT US
GOOCH & HOUSEGO LOCATIONS GET IN TOUCH We enable leading organizations all over the world by delivering tailored, innovative solutions to meet precise requirements. For specific information or to discuss your next project, please visit goochandhousego.com, e-mail us at [emailprotected] or call the relevant sales contact.
EUROPE
USA
Gooch & Housego (Deutschland)
Gooch & Housego (Boston)
EUROPEAN SALES OFFICE
ACTIVE FIBER OPTIC COMPONENTS, MODULES AND PHOTONICS PACKAGING
Berliner Allee 55, 22850 Norderstedt, Germany T: +49 40 528899 12
Gooch & Housego (France) FRENCH SALES OFFICE
Gooch & Housego (California)
Opening early 2017
PRECISION OPTICAL ASSEMBLIES AND COMPONENTS
Gooch & Housego (Glenrothes)
COMPANY HEADQUARTERS Gooch & Housego PLC Dowlish Ford, Ilminster TA19 0PF, UK T: +44 1460 256440
ASIA Gooch & Housego (Japan) JAPAN SALES OFFICE Level 4, Nikko Shoken Building, 3-2-3 Sakae, Naka-ku, Nagoya, 460-0008, Japan T: +81 90 5615 2610
7 Oak Park Drive, Bedford, MA 01730, USA T: +1 781 275 7501
PRECISION OPTICAL ASSEMBLIES AND COMPONENTS Telford Road, Glenrothes KY7 4NX, UK T: +44 1592 771590
Gooch & Housego (Torquay) PASSIVE FIBER OPTIC COMPONENTS, MODULES AND PHOTONICS PACKAGING
5390 Kazuko Court, Moorpark, CA 93021, USA T: +1 805 529 3324
Gooch & Housego (Madison) ELECTRO-OPTICAL AND LASER SYSTEMS 1832 Wright Street, Madison, WI 53704, USA T: +1 608 240 4885
Broomhill Way, Torquay TQ2 7QL, UK T: +44 1803 611700
Gooch & Housego (Ohio)
Gooch & Housego (UK)
676 Alpha Drive, Highland Heights, OH 44143, USA T: +1 216 486 6100
ACOUSTO-OPTIC COMPONENTS, PRECISION OPTICAL ASSEMBLIES AND COMPONENTS
CRYSTAL AND ELECTRO-OPTIC COMPONENTS AND ASSEMBLIES
Dowlish Ford, Ilminster TA19 0PF, UK T: +44 1460 256440
Gooch & Housego (Palo Alto)
Kent Periscopes Ltd
44247 Nobel Drive, Fremont, CA 94538, USA T: +1 650 856 7916
ELECTRO-OPTIC SIGHTING SYSTEMS 6 Ffordd Richard Davies, St. Asaph Business Park, Denbighshire LL17 0LJ, UK T: +44 1745 584480 www.kentperiscopes.co.uk
ACOUSTO-OPTIC, CRYSTAL OPTIC AND LITHIUM NIOBATE PRODUCTS
Gooch & Housego (Orlando) LIGHT MEASUREMENT INSTRUMENTATION AND CALIBRATION SERVICES 4632 36th Street, Orlando, FL 32811, USA T: +1 407 422 3171 Toll free from the US: 1 800 899 3171 www.ghinstruments.com
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CONTACT US
SALES CONTACTS SYSTEMS AND COMPONENTS – GLOBAL SALES TEAM Senior Vice President, Sales Europe and Asia-Pacific Paul Morris T: +44 7843 349553 E: [emailprotected]
South Asia Account Manager Tak-Sing Lam T: +65 9159 3261 E: [emailprotected]
Servicing: India, Singapore, Malaysia, Thailand and Vietnam
EUROPE
AEROSPACE & DEFENSE
European Sales Director
EUROPE
Ekkehard Overbeck T: +49 8152 396 1702 E: [emailprotected]
Key Account Manager Aerospace & Defense Gary Sinclair T: +44 7917 533559 E: [emailprotected]
Business Development Manager Aerospace & Defense Trevor Cook T: +44 7891 133728 E: [emailprotected]
USA Director of Business Development Aerospace & Defense Iwan Dodd T: +1 440 561 7123 E: [emailprotected]
INDUSTRIAL, LIFE SCIENCE AND SCIENTIFIC RESEARCH
ASIA Asia Pacific Sales Director Masashi Wada T: +81 90 5615 2610 E: [emailprotected]
China, South Korea and Taiwan Sales Director Martin Cheng T: +852 6348 6199 (Hong Kong) T: +86 150 0022 5614 (China) E: [emailprotected] Servicing: China, South Korea and Taiwan
Business Development Manager Precision Optics Pete Williams T: +44 7736 278044 E: [emailprotected]
European Precision Optics Sales Manager Clive Morrison T: +44 7712 677035 E: [emailprotected]
Germany, Austria and Switzerland Account Manager Bernhard Uhlhaas T: +49 221 677 707 99 E: [emailprotected]
UK and Northern Europe Account Manager Dan Barlow T: +44 7843 349 550 E: [emailprotected]
Southern Europe Regional Manager
USA Director of Business Development Life and Health Sciences Mark Stevens T: +1 910 274 8927 E: [emailprotected]
Director of Sales, Americas Tom McGunigal T: +1 540 305 5020 E: [emailprotected]
US East Coast Regional Sales Manager Tom Geyer T: +1 781 491 6941 E: [emailprotected]
US West Coast Regional Sales Manager Merrill Apter T: +1 650 354 0156 E: [emailprotected]
US West Coast Key Accounts Manager Jim Data T: +1 408 887 5510 E: [emailprotected]
INSTRUMENTATION
USA Sales and Marketing Coordinator Maureen Knowles T: +1 407 422 3171 extension 206 E: [emailprotected]
Sébastien Lenoir T: +33 6 08 78 52 56 E: [emailprotected]
Southern Europe Account Manager Martial Destoc T: +33 6 21 78 03 42 E: [emailprotected]
European Sales Assistant Anja Schumacher T: +49 40 5288 9912 E: [emailprotected]
Japan Sales Manager Yosh*taka Yokoyama T: +81 90 1798 7955 E: [emailprotected]
GOOCH & HOUSEGO
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CONTACT US
DISTRIBUTORS COMPONENTS AND PHOTONIC ASSEMBLIES
ASIA CHINA ACOUSTO, ELECTRO, AND FIBER OPTICS
Ante Laser Technology Co. Ltd. (a subsidiary of Sintec Optronics) T: +86 20 2839 5114/5167/5172/5176 E: [emailprotected] www.antelaser.com ACOUSTO-OPTICS
Aunion Tech Co. Ltd. T: +86 21 5108 3793 E: [emailprotected] www.auniontech.com
HanRay Group Ltd. (a subsiduary of Shanghai Unisilver Technology Ltd.) T: +852 3645 8129 E: [emailprotected]
Shanghai UniSilver Technology Ltd. T: +86 (21) 3367 5018 E: [emailprotected] www.uni-silver.com
Wuhan Sintec Optronics Co. Ltd. T: +86 (27) 51858988 E: [emailprotected] www.518168.cn FIBER COUPLED ACOUSTO-OPTICS, FIBER OPTICS
Miracle Photonics Technology Co. Ltd. T: +86 (10) 6378 6090 E: [emailprotected] www.miraclephotonics.com
INDIA, MALAYSIA, PHILIPPINES, SINGAPORE, THAILAND,VIETNAM ACOUSTO, ELECTRO, AND FIBER OPTICS
New Age T: +91-124-4086513 16 E: [emailprotected] www.newagein.com Servicing: India
Distributors represent all G&H products unless specified otherwise. 86
Sintec Optronics Pte Ltd T: +65 6316 7112 E: [emailprotected] www.sintecoptronics.com.sg Servicing: India, Philippines, Singapore
Kumpulan Abex SDN BHD
EUROPE AUSTRIA, GERMANY, SWITZERLAND EQ Photonics GmbH
T: +60(03) 5192 2898 E: [emailprotected] www.kabex.com.my
Contact: Franz Schwarzbauer T: +49-89-319-019-23 E: [emailprotected] www.eqphotonics.de
JAPAN
FRANCE
Servicing: Malaysia, Thailand, Vietnam
Autex, Inc. T: +81 3 3226 632 E: [emailprotected] www.autex-inc.co.jp
New Metals T: +81 3 3231 8600 E: [emailprotected] www.newmetals.co.jp
Opto Science T: +81 3 3356 1064 E: [emailprotected] www.optoscience.com
Nano-Giga S.A.R.L. Contact: Rached Bouazza T: +33 1 71 36 05 63 E: [emailprotected] www.nano-giga.fr
ISRAEL New Technology Contact: Sagie Cohen T: +972-3-6792000 E: [emailprotected] www.newtech.co.il
ITALY
FIBER OPTICS
dB Electronic Instruments SRL
Hakuto Co. Ltd.
T: +39 02 646 9341 E: [emailprotected] www.db-electronic.it
T: +81-3-3225-8910 www.hakuto.co.jp
KOREA L2K (Laser Leader of Korea) T: +82 42 9347744 E: [emailprotected] www.l2k.kr
TAIWAN
POLAND Lambda System Contact: Radoslaw Kreft T: +48 22 622 20 14 M: +48 666 026 793 E: [emailprotected] www.lambdasystem.pl
Veego Technology Corporation
RUSSIAN FEDERATION
T: +886 4 22603233 E: [emailprotected] www.veego.com.tw
Special Systems, LLC.
AUSTRALIA AND NEW ZEALAND
T: +7 812 385 7297 E: [emailprotected] www.sphotonics.ru
NORTH AMERICA
Coherent Scientific Pty Ltd.
USA
T: +61 8 8150 5200 E: [emailprotected] www.coherent.com.au
XSoptix, LLC. Contact: Mike Carr T: +1 203 401 8093 E: [emailprotected] www.xsoptix.com
Servicing: East of the Mississippi
GOOCH & HOUSEGO
CONTACT US
INSTRUMENTATION
ASIA CHINA, HONG KONG, SINGAPORE Light All Contact: Bob Liu T: +86 21 5102 9613 E: [emailprotected] www.light-all.com
INDIA Deepti Marketing Services Contact: M.R. Gopinath T: +91 80 32713974 E: [emailprotected] www.deepms.com
JAPAN KLV Ltd. Contact: Sada Machida T: +81 3 3258 1238 E: [emailprotected] www.klv.co.jp
MALAYSIA MBit Technologies Contact: Andy Low T: +60 3 5612 0009 E: [emailprotected] www.mbittech.com
SOUTH KOREA HK International Corp. Contact: Ji-Soung Park T: +822 2658 4366 E: [emailprotected] www.hkic.co.kr
TAIWAN Forter Technology Contacts: Chester Chen, James Chien T: +886 4 22607729 E: [emailprotected] or [emailprotected] www.forter.com.tw
THAILAND Aditus Technik
AUSTRALIA AND NEW ZEALAND Coherent Scientific Contact: Paul Wardill T: +61 8 81505200 E: [emailprotected] www.coherent.com.au
EUROPE AUSTRIA, CZECH REPUBLIC, GERMANY HUNGARY, SLOVAKIA Opteema Engineering Contact: Ingo Fischbach T: +49 3677 79 05 58 E: [emailprotected] www.opteema.de
BELGIUM, NETHERLANDS, LUXEMBOURG Spectra Partners Contact: Frans van der Meij T: +31 23 544 11 64 E: [emailprotected] www.spectrapartners.nl
DENMARK, FINLAND, NORWAY, SWEDEN AMS Technologies/Azpect Photonics Contact: Joakim Karnbratt T: +46 8 55 44 2480 E: [emailprotected] www.azpect.com
FRANCE Scientec Contact : Jean-Luc Rondeau T: +33 1 64 53 27 00 E: [emailprotected] or [emailprotected] www.scientec.fr
ISRAEL
ITALY Photo Analytical Contact: Ilaria Chiodelli T: +39 02 95379353 E: [emailprotected] www.photoanalytical.com
POLAND MD Scientific Contact: Dr Marek Danielewicz, PhD T: +45 7027 8565 E: [emailprotected] www.md-scientific.dk
RUSSIAN FEDERATION Eniseylab Contact: Dmitriy Zhiltsov T: +7 391 278 3092 E: [emailprotected] www.eniseylab.ru or www.ghinstruments.ru
SPAIN, PORTUGAL Azbil Telstar Technologies Contact: Teresa Esquefa T: +34 93 544 23 20 E: [emailprotected] www.telstar.eu
SWITZERLAND Instrumat AG Contact: Dr. Francois Maystre T: +41 21 634 25 25 E: [emailprotected] www.instrumat.ch
UNITED KINGDOM Precision Photometrics Contact: Chris MacLellan T: +44 131 618 0600 E: [emailprotected] www.precisionphotometrics.com
NORTH AMERICA
SK Advanced
CANADA
Contact: Eyal Shachar T: +972 3 549 3364 E: [emailprotected] www.sk-advanced.com
GL Photonics Contact: Gord Leachman T: +1 647-293-4309 E: [emailprotected]
Contact: Yod Unhavaithaya T: +66 2 691 6477 E: [emailprotected]
GOOCH & HOUSEGO
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INDEX
INDEX COSTA RICA Vimat Contact: Esteban Ardón León T: +506 8997 0208 E: [emailprotected] www.vimat.net
USA Brooks Engineering T: +1 312-867-1840
Servicing: Arkansas, District of Columbia, Illinois, Indiana, Iowa, Kansas, Kentucky, Louisiana, Maryland, Michigan, Minnesota, Missouri, Nebraska, North Dakota, Ohio, Oklahoma, Pennsylvania (zip codes 15000 thru 16800), South Dakota, Texas, Virginia, West Virginia and Wisconsin)
DMS Technologies Contact: David Sandoz T: +1 949-812-1410 E: [emailprotected] www.dmstech.us
Servicing: Arizona, California, Colorado, Idaho, Montana, Nevada, New Mexico, Oregon, Utah, Washington, and Wyoming
Ray Pini Consulting Contact: Ray Pini T: +1 908-720-5491 E: [emailprotected]
Servicing: Alabama, Connecticut, Delaware, Florida, Georgia, Maine, Massachusetts, Mississippi, New Hampshire, New Jersey, New York, North Carolina, Pennsylvania (16801 – 19699), Rhode Island, South Carolina, Tennessee and Vermont
For all other states Contact Gooch & Housego (Orlando) T: +1 407-422-3171 E: [emailprotected]
SOUTH AMERICA ARGENTINA Laseroptics SA Contact: Claudio Petriella T: +54 11 4372 7547 E: [emailprotected] www.laseroptics.com.ar
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AO Beam deflectors PO Coatings PO Corner cubes CO Crystals and nonlinear optics FO DFB lasers and modules PO Electro-optic sighting systems PO Electro-optical assembly and systems FO Fiber optic assemblies and subsystems FO Fiber-coupled pump lasers AO Fiber-Q® fiber-coupled modulators AO Frequency shifters FO Fused fiber optic components FO High reliability erbium-doped fiber amplifiers FO High reliability fused fiber optic components FO High speed detectors PO Hy-Per Bond™ – adhesive and organic-free bonding PO Infrared optics LMI Instrument calibration LMI Integrating spheres FO Laser controllers PO Lenses LMI Light measurement detectors LMI Light measurement services EO Lithium niobate Q-switches CO Lithium niobate wafers PO Magnetorheological finishing (MRF) PO Metrology PO Mirrors AO Mode lockers AO Modulators – free space and fiber-coupled AO Multi-channel modulators LMI Multi-channel spectroradiometers LMI NIST-traceable test and measurement services CO Nonlinear optics FO OCT components and subsystems PO Optical crystal growth PO Optical domes PO Optical flats PO Optical materials PO Opto-mechanical assemblies CO Periodically-poled lithium niobate PO Plate and cube beamsplitters EO Pockels cells EO Pockels cell drivers PO Prisms AO Pulse pickers/cavity dumpers FO Pump combiners AO Q-switches – acousto-optic AO RF drivers PO Ring laser gyroscope components PO Single-point diamond turning PO SROC PO Superpolishing PO SWIR lens assemblies PO Synchrotron mirrors AO Tunable filters – free space and fiber-coupled PO Waveplates PO Windows
15 59 64 32 45 78 61 51 44 20 16 49 54 53 47 60 76 81 81 48 65 81 81, 83 39 31 58 62 68 17 18, 20 22 82 83 32 52 56 77 71 56, 57 61 33 70 37 38 63 23 50 24 27 75 58 74 59 66 69 25, 26 72 71
GOOCH & HOUSEGO
Published by Gooch & Housego PLC – January 2017 Compiled by: Lynore Abbott and Cicely Rathmell Design and artwork: Paul McKenzie Studio Photography: Paul Box, Rod Johnson, Roger Mastroianni and Lucy Wallace Image retouching: Damian Adams Illustrations and renders: Lauren Jones Project management: Deb Kamofsky Every effort has been made to ensure the accuracy of the information contained in this catalog at the time of publication. As part of our policy of continuous product improvement, we reserve the right to change specifications at any time. For the most up-to-date information, please refer to our website. goochandhousego.com
Gooch & Housego PLC Dowlish Ford, Ilminster TA19 0PF, United Kingdom T: +44 (0)1460 256440 E: [emailprotected] goochandhousego.com