De-Specklers

Inside Diameter 15 to 450 µm; Outside Diameter 90 to 673 µm; Coating Polyimide; Temperature Range -190 to +350 °C; Tensile Strength >600 kpsi Fiberguide’s fused silica capillary tubing is used for micro-fluidics applications and in gas chromatography (GC) separation columns. These capillaries are coated with polyimide for mechanical stability and versatile uses. With inert surfaces and high purity, Fiberguide’s capillary tubing solutions provide a very high phase stability, while their peak mechanical stability leads to greater yield and more cost-efficient tubing. Based on the great flexibility combined with high tensile strength (>600 kpsi), these capillary tubing solutions are pressure resistant to 4,500 psi and allow very small radii during coiling with no kinking. They are impervious to chemicals, allowing usage in harsh environments. A wide range of internal and external diameters with tight tolerances allows users to select a capillary tubing solution that best suits their flow rate requirements. All capillaries can be easily cleaved or cut, allowing to adjust exactly the column length needed for interfacing. While the mirror smooth inner surface provides stable laminar flow profiles and good adherence, the capillary tubing solutions’ Polyimide coating is very durable and abrasion resistant. Key Features: Pure Fused Silica Construction Outside Diameters: 90 to 673 µm Inside Diameters: 15 to 450 µm Coating: Polyimide Temperature Range: -190 to +350 °C Tensile Strength: >600 kpsi 100% Proof Tested for Strength Applications: Micro-fluidics Applications; Gas Chromatography (GC) Separation Columns

Delivery System consisting of a laser to fiber coupler, fiber optic patchcord, fiber optic collimator, and fiber optic line generator; Power Transmission ≤1 to ≤ 20 W In flow visualization systems, a visible wavelength laser beam is coupled into an optical fiber, recollimated at the fiber output, and then sent through a lens, generating a line. This line of laser light is then shone through the flowing liquid under inspection. Any particulate matter present, or changes to the flow pattern within the fluid, causes fluctuations in the output beam pattern which are visually observed. OZ Optics offers complete delivery systems for flow visualization, consisting of a laser to fiber coupler, fiber optic patchcord, fiber optic collimator, and fiber optic line generator. The line generator uses a Powell lens. Compared to simple cylindrical lenses, this Powell lens transforms a collimated beam into a line with a uniform output intensity along its entire length. Fiber optic delivery systems are available for a wide range of wavelengths. Other wavelengths are available on request. The maximum power transmission possible depends upon the fiber size chosen 4/125 fiber can handle 1 W to 3 W, 10/125 fiber can handle 3 W to 5 W, 25/125 fiber can handle 5W to 10 W, and 50/125 fiber can handle 10 W to 20 W. For best repeatability and stability, FC connectors are recommended for the fiber couplers and collimators. Pigtail style couplers and collimators are also recommended.By choosing different focal lengths for the collimating and Powell lenses, different line widths and fan angles are possible. Standard line widths for singlemode fibers are 0.8 mm and 1.2 mm. Standard fan angles are 10°, 30° and 45°. Contact us for further information on available line widths and fan angles. Key Features: Uniform Output Intensity over Entire Length Rugged and Compact Design Low Insertion Loss Visible Wavelength Range: 400 to 700 nm Wide Fan Angles Available: 10 to 75 degrees Applications: Flow Cytometry, Particle Measurement, Imaging Systems

Fixed or Variable; Receptacle or Pigtail Style; Fiber Type SM, MM, PM; 400 to 1600 nm; Back Reflection 25 to 60 dB OZ Optics’ FORF series of fiber optic reflectors are used to reflect the light emerging from a fiber back in the reverse direction. They are used to build fiber interferometers, or with fiber fused splitters to measure back reflection within fiber optic components. They can also be used to measure the sensitivity of sources to back reflection from other devices, by providing reference reflection levels. This is very useful for deriving back reflection specifications for transmitters. Fiber optic reflectors consist of a fiber optic collimator and a mirror. The fiber output is first collimated, then it strikes the mirror and is reflected back into the collimator. The angle between the collimator and the mirror is adjusted using OZ Optics' patented tilt adjustment technique, until as much light as possible is reflected back into the fiber. Using this technique, reflectors with typical losses of only 0.6 dB can be constructed. A variable reflector is available that includes a blocking screw, to obtain variable reflection levels. This is achieved by partially blocking the collimated beam between the lens and the mirror. Both connector receptacle style and pigtail style reflectors are available. Connector receptacle style reflectors come with a female connector receptacle to allow the fibers to be easily changed. Pigtail style reflectors come with a fiber of your choice permanently attached to the collimating lens. This type of reflector is recommended for optimum coupling efficiency and stability. The other end of the fiber can be terminated with your choice of connector. OZ Optics also provides fibers with coated ends. Gold coatings are used to provide excellent broadband reflection for infrared wavelengths. Other coating materials are available for other wavelengths. The ends can have total reflecting, or partial reflecting/partial transmitting coatings. Contact AMS Technologies for further information. Reflectors are available for wavelengths from 400 to 1600 nm. Reflectors that operate at both 1300 and 1550 nm are available, with only a slight difference in insertion losses at both wavelengths. Broadband reflectors using achromatic lenses to collimate light at different wavelengths are available. Partially reflecting mirrors are also available, to partly transmit the light. The transmitted light can be coupled into an output fiber as an option, thus forming an in-line reflector. Contact AMS Technologies for further details. Key Features: Wide Range of Available Wavelengths Available in Single Mode (SM), Polarization Maintaining (PM) and Multi Mode Versions Low Insertion Loss Compact Housing Partial Reflectors Available Applications: Interferometric Sensors; Circulators; Return Loss Testing; Reference Beam Power Measurements

980-1650 nm; Total Phase Shift >8π; IL <0.1 dB; RL >65 dB; PDL <0.05 dB; Residual Amplitude Modulation ±0.01 dB General Photonics’ FPS-001 is an all-fiber device that shifts or modulates phase by up to 15π at frequencies from DC to 20 kHz. The advantage of the all-fiber construction is that insertion loss and back reflection are reduced to near zero. Key Features: Low Insertion Loss (IL): < 0.1 dB Low Residual Amplitude Modulation: ±0.01 dB NoTail™ Version Available Operating Wavelength: 1260 to 1650, 980 to 1310 nm Return Loss (RL): >65 dB Total Phase Shift (0 to 20 kHz): >8π Half-wave Voltage (0 to 20 kHz): <20 V Polarization Dependent Loss (PDL): <0.05 dB Maximum Applied Voltage: 150 V Dimensions: 35 x 14 x 14 mm (Pigtail), 74 x 14 x 14 mm (NoTail™) Applications: Precision Phase Tuning or Phase Modulation in Fiber Interferometers, Sensor Systems, Fiber Laser Systems or Fiber Resonators

780-1550 nm; Total Phase Shift >65π; IL <0.5 dB; RL >50, >55, >58 dB; PDL <0.05, <0.1 dB; Residual Amplitude Modulation ±0.01 dB Coherent or interferometric sensor systems, such as distributed acoustic sensors (DAS), often require a low-loss, low-cost phase shifter or modulator to obtain the desired sensing signals. General Photonics’ FPS-002 is an all-fiber device that shifts or modulates phase shifts up to 75π at frequencies from DC to 20 kHz. The FPS-002 phase shifter requires a lower half-wave voltage than the FPS-001 phase shifter module: only 2 V compared to up to 20 V. Like the FPS-001, it is an all-fiber design and offers the benefits of low loss and back reflection. Two different size packages (small frame or large frame) are available to accommodate the bend diameter requirements of different fibers. Key Features: Low Insertion Loss (IL): <0.5 dB (at λc, Excluding Connectors) Low Polarization Dependent Loss (PDL): <0.05 dB (SM), <0.1 dB (PM) Return Loss (RL): >58 dB (Without Connectors), >55 dB (With APC Connectors), >50 dB (With PC Connectors) Low Residual Amplitude Modulation: ±0.01 dB at 1550 nm Total Phase Shift (@500 Hz, Vpp = 150 V): >65π (@ 1550 nm) Low Half-wave Voltage (@ 500 Hz): 2.5 to 4.5 V Typical (Small Frame), 0.7 to 1.5 V Typical (Large Frame) Operating Wavelength: 780, 1060, 1310, 1550 nm Fiber Type: ClearCurve ZBL, HI1060, 780 HP, PM, PM980XP Capacitance of Piezo: 0.18 µF Maximum Applied Voltage: 150 V Compact Size: 35 x 17 x 10 mm (Small Frame), 45 x 27 x 11 mm (Large Frame) Applications: Fiber Interferometers; Fiber Laser Systems; Fiber Sensor Systems

780-1550 nm; Total Phase Shift >55π; IL <0.5 dB; RL >55 dB; PDL <0.05 dB; Residual Amplitude Modulation ±0.01 dB General Photonics’ FPS-003 all-fiber phase shifter/modulator combines a wide modulation bandwidth (up to 60 kHz) with low half-wave voltages to create a long-range device that can be driven by standard function generators. Like General Photonics’ other phase shifters, it employs all fiber construction and has low insertion loss and back reflection. In addition to fiber sensor systems, this compact device is ideal for fiber laser systems, fiber resonators, and fiber interferometers for precision phase tuning or phase modulation. Key Features: Wide Frequency Range - Operating Wavelength: 780, 1060, 1310 or 1550 nm Low Half-wave Voltage Large Phase Shift Range Compact Size: 31 x 31 x 14.5 mm Low Insertion Loss (IL): <0.5 dB (at 1550 nm, Excluding Connectors) Return Loss (RL): >55 dB (Excluding Connectors) Low Residual Amplitude Modulation: ±0.01 dB (@ 1550 nm) Total Phase Shift (@500 Hz, Vpp = 150 V): >55π (@ 1550 nm) Fiber Type: ClearCurve ZBL, 780 HP, PM, Other Half-wave Voltage (Vπ @ 500 Hz): 1 to 3 V Typical Resonance Frequency: 36 to -39 kHz Typical Vπ at Resonance Frequency: <150 mV Typical Polarization Dependent Loss (PDL): <0.05 dB at 1550 nm Capacitance of Piezo: 5 to 12 nF Maximum Applied Voltage: 150 V Applications: Fiber Interferometers; Fiber Laser Systems; Fiber Sensor Systems

1260-1650 nm; Delay Range >3 mm; RL >65 dB; Fiber Type SMF-28, Other; IL <0.2 dB; PDL <0.05 dB General Photonics’ FST-001 is a piezo-driven fiber stretcher with an optical delay range of up to 3 mm. The device, including the piezo driver, is packaged in a metal enclosure. Each of the FST-001 fiber stretcher’s four piezos can be controlled independently, allowing high resolution or large stroke. Piezos can be controlled with an analog signal or a 12-bit TTL signal. Under analog control, the driving circuit acts as a 4-channel voltage amplifier with 30V/V amplification. Alternatively, the output voltage can be controlled by a computer equipped with a digital I/O card, or by a microprocessor. Key Features: Large Optical Path Delay Range: >3 mm (In Air) High Speed Low Insertion Loss (IL): <0.2 dB Analog and Digital Control Analog Input: 4 Channels, 4.7 V Maximum For Each Channel Digital Input: 20-pin Connector, 12-bit TTL Control Signal Operating Wavelength: 1260 to 1620 nm Maximum Optical Power: 1,000 mW Phase Change Sensitivity: 810 π/V Internal Voltage Amplification: 30 V/V Maximum Voltage on Piezo: 140 V Resonance Frequency: 2.2 ±0.3 kHz Return Loss (RL): >65 dB Polarization Dependent Loss (PDL): <0.05 dB Fiber Type: SMF-28, Other on Request Dimensions: 170 x 106 x 39 mm Applications: Sensors; Interferometers; Medical Imaging; Spectrum Analysis; OCT

Circular and Oval Configurations; Inner Ø 279 to 4,400 µm; Outer Ø 762 to 5,400 µm; Thickness 203 to 760 µm; Sealing Temperature +340 to +440 °C OZ Optics’ GSP series of glass solder preforms is designed specifically for hermetic sealing of optical fibers in optoelectronic and all optical packaging. The glass solder preforms bond directly to glass and metal surfaces. This enables hermetic sealing of optical fibers to metal packages without costly metallization, thus reducing the cost and lead time of the whole packaging process. After processing, assemblies sealed with glass solder can easily meet the stringent humidity resistance, hermeticity, and strength demanded for component packaging. Custom configurations can be designed for specific applications, please contact AMS Technologies to select a design to fit your needs. GSP series glass solder preforms are compatible with single mode (SM), multi mode (MM) or polarization maintaining (PM) fibers in single fiber and ribbon constructions. To help use the glass solder preforms, OZ Optics can supply a basic resistive or inductive soldering station to solder preforms onto metal ferrules and fibers. Key Features: Compatible with Single Mode (SM), Multi Mode (MM) or Polarization Maintaining (PM) Fibers Alternative to Costly Gold Plating Methods for Hermetic Sealing Available in Circular or Oval Configurations Fatigue and Corrosion Resistant No Flux Required for Use Low Melting Temperature High Fluidity When Molten Large Volume Manufacturing Capacity Designed to Meet Telcordia Specifications Applications: Fiber to Metal Hermetic Sealing; Laser Diode Packaging; Integrated Optics Packaging; Vacuum Feed-through Assemblies

High Power; Insertion Loss <0.5 dB; Power Handling ≤50 W; Shutter Response Speed <5 ms; Shutter Electrical Interface 5 V TTL In response to increasing demand for high power handling fiber optic components, OZ Optics has developed the HPCR / AA-250 / SH-200 series of fiber optic shutters and connectors that incorporate smart sensors for safety interlocks. These shutter systems can be incorporated in high power handling components, including freespace-to-fiber and fiber-to-fiber coupling situations. For extreme power handing capabilities, the shutters can also incorporate additional beam dumps and/or heat sinks to safely absorb the blocked laser power. The key components that allow realization of smart shutters and safety interlocks are a series of proximity sensors and temperature sensors installed at suitable locations in the body of fiber optic assemblies. These provide the necessary electrical signals to alert the end user to take appropriate action. Key Features: Multiple Watt CW Power Handling Shutter Speeds of <5 ms Controlled via 5 V TTL Signal Available with Temperature and Connector Proximity Sensors for Safety Interlocks Compatible with SMA 905 and FC Connectors Available in Laser-to-fiber and Fiber-to-fiber Versions Fiber Connectors and Receptacles with Safety Sensor/interlocks Available Applications: All Situations Involving Laser Beams, Including High Power Laser Beams Coupled into SM or MM Fibers; Laser Facilities Requiring Compliance to Laser Safety Standards; High Power Industrial and Medical Laser Applications - Laser Marking, Cutting, Welding, Laser Scalpel, Eye Surgery, Tattoo Removal; High Power Laser Physics; High Power Spectroscopy; OEM Laser Systems

980-1080 nm; Input Fiber 6/125 µm; Output Fiber 10/125-25/250 µm; Numerical Aperture Output Fiber Core 0.06-0.1; Max. Transmitted Power >50 W; Max. Insertion Loss <0.5 dB A mode field adapter is an essential device to efficiently transfer light for a standard single mode (SM) fiber to the LP01 mode of large mode area (LMA) and low order mode multi mode (MM) fibers. The performance is greatly superior to using a regular splice, as an ordinary splice will produce a degraded quality output beam with a poor M2 factor. Mode field adapters also generate lower losses than ordinary splices, thus ensuring higher power transmission compared to regular splicing. Key Features: High Power Handling Capability Spanning a Wide Optical Spectral Range Adapts and Conserves Modal Content Custom Design Flexibility Wavelength: 980 nm to 1080 nm Input Fiber (Core/Clad): 6/125 µm Output Fiber (Core/Clad): 10/125 µm, 20/125 µm, 25/125 µm, 25/250 µm Numerical Aperture (NA) Core (Output Fiber): 0.06 to 0.1 Max. Transmitted Power: >50 W Max. Insertion Loss (IL): <0.5 dB Dimensions: 76 x 19 x 10 mm Applications: High-power Fiber Lasers; High-power Pigtailed Isolators; High-power Fiber Optic Component Manufacturing; Research and Design

320 to 2100 nm; Tap Ratio 0.5 to 4%; Insertion Loss <0.05 to 0.3 dB; Return Loss >70 dB; Fiber Type SM, MM, PM, PC, Other; Power Handling 250 to 2000 mW With the OPM series, OZ Optics offers inline optical power monitors and tap couplers based on a revolutionary, patented technology. These taps and monitors provide a way to easily measure the signal intensity through an optical fiber in a simple, miniature package and are ideal for real time monitoring and feedback for optical amplifiers or WDM systems as well as for fiber optic sensors. Traditional monitoring systems typically use fused couplers to tap a fixed amount of light into another fiber that guides the optical power to a photodiode. This method is bulky and must be done using discrete components. In contrast, OZ Optics' OPM series of optical taps direct a controlled amount of light from the fiber core to the cladding surface where it can be directly monitored with high efficiency and very low loss. This inline tapping is accomplished without bending, shaping, or otherwise distorting the fiber. As a result, the tap can be directly incorporated into optical assemblies, without affecting the original functionality. While taps are directional in nature (ideal for monitoring traffic independently of signals travelling back through a network link), bi-directional versions are also available and can be provided on request. OPM taps can be fabricated into standard single mode (SM), polarization maintaining (PM), multi mode (MM), photonic crystal (PC) and other specialty fibers, for any design wavelength and with different tap ratios available upon request. OPM optical power monitors combine the optical tap design with a photodiode in an integrated package and are available in different configurations with Si and InGaAs detectors for different wavelength ranges. The devices produce a current proportional to the optical power within the fiber, and the small size and simple interface makes it very easy to design into optical hardware. Multiple channel power monitors for WDM applications are available upon request. Key Features: Miniaturized Package Inline Integration Without Interruption to the Optical Path Telcordia GR-468 Qualified Available for Any Wavelength from 400 to 2100 nm Low Insertion Loss, Return Loss and Polarization Dependent Loss High Directivity and Large Dynamic Range Broadband Response High Power Handling High Extinction Ratios for PM Versions Remotely and Locally Controllable, USB and RS232 Communication Options Available for Standard Telecom Fibers, PM, MM, Photonics Crystal and Other Speciality Fibers Available with or without Integrated Photodiode Applications: Power Monitoring; Optical Power Control Devices; Channel Balancing for Wavelength Division Multiplexing (WDM) Systems; Dynamic Optical Amplifier Gain Monitoring; FTTH Network Monitoring; Real-time Inline Test and Measurement; Fiber Optic Sensors; OCT Systems

High Speed; Fiber Type SM, PM, RC; 780-1625 nm; Fiber Length 5-17 m; Fiber Stretch 0.035-0.21 µm/V; Fiber Leads 1 m, 0.9 mm OD Jacket; Connector Type Bare Fiber, FC/PC, FC/APC The PZ1 series are the high-speed members of Optiphase’s family of fiber stretchers. At the core of the PZ1 high-speed fiber stretchers is a fiber wound piezoelectric element for use in a wide range of optical interferometric measurement and sensing system applications. Optiphase’s expertise in the design, manufacture and use of all-fiber interferometers has produced a unique multi-layer winding approach resulting in an enhanced modulation function while maintaining a high operational frequency. PZ1 high-speed fiber stretchers are available with single mode (SM), commercial polarization maintaining (PM, Panda or Bowtie) or SM reduced cladding (RC) fiber types PZ1 high-speed fiber stretchers deliver a high performance to cost ratio, exceeding all other known competitive devices. The compact and low-profile form factor makes the PZ1 series easily configurable into small spaces. In addition, Optiphase fiber stretchers are unique in that they do not require proprietary drivers. For most low-voltage applications (<±15 V), Optiphase stretchers can be driven by standard electronics such as signal generators, op-amps or other laboratory equipment without modification. For more information on how to drive PZ1 high-speed fiber stretchers see the downloadable application note. Key Features: High Speed Compact Package Fiber Type: Single Mode (SM), Polarization Maintaining (PM )or Reduced Cladding SM (RC) Fiber Multiple Termination Choices Unique Multi-layer Winding Can Be Driven With General Purpose Electronics Operational Wavelength: 780 to 1625 nm Fiber Stretch: 0.035 to 0.21 µm/V Optical Path Displacement (n = 1): 0.05, 0.2, 0.3 µm/V Time Delay: 0.00017 to 0.001 ps/V Fiber Length: 5, 12.3, 17 m Inclusive Fiber Wind: 4 Layer (1 Layer PM Version Available) Optical Loss: ≤0.5 dB Maximum Voltage Range: ±500 V (Off Resonance, 1,000 V Peak-to-Peak) Fiber Leads: 1 m, 900 μm Loose Tube Connector Type: Bare Fiber, FC/PC, FC/APC Dimensions: 50.8 x 50.8 x 21.6 mm Applications: Open Loop Demodulation; Sensor Simulation; Variable Optical Delay; General Purpose Fiber Interferometry; Large-angle Modulation of Interferometric Phase