SPAD Single-Photon InGaAs/InP Avalanche Photodiodes APD

Fiber Type Single Mode, Multi Mode, Polarization Maintaining (PM/PZ); Number of Fibers ≤128 (V-Grooves), ≤4096 (2D Arrays); Fiber Cladding Outer Ø 125 µm (V-Grooves), 125 to 220 µm (2D Arrays); Connector Options SMA, FC, ST, SC, LC, MTP, etc.Fiberguide produces extremely tight tolerance one-dimensional (V-Grooves) and two-dimensional arrays using the supplier’s patented manufacturing techniques. These arrays range from a few fibers to thousands of fibers depending on the application. Optical Arrays are used in optical switching and in sensing applications where spatial optical data is necessary, such as DNA sequencing, astronomy and nuclear research. For high temperature applications, some fiber types can be aluminium or gold coated on request. Additionally, all fiber types can be equipped on demand with Fiberguide’s patented RARe Motheye anti-reflective technology that enhances fiber transmission performance and significantly increases the damage threshold for your application over a large wavelength range. Key Features: Fiber Type: Single Mode, Multi Mode Array End: Precision Machined Housings, Silica V-Grooves or Custom Silicon Wafers Connector Options: SMA, FC, ST, SC, LC, MTP, etc. Packaging: Design and Production of Custom Array Housings and Sheathing Arrangements Available to Protect the Fiber Depending on the Application Standard Temperature Range: -40 to + 100 °C Applications: Fiber Optic Switch; Signal Processing; Astronomical Analysis; Military Mapping; DNA Micro-array Technology; Optical Tomography

3 Stage Scramblers or 4 Stage Controllers Available; 1250 to 1650 nm (Others on Request); Insertion Loss <0.4 dB; Polarization Dependent Loss <0.06 dB; Fiber Type SM OZ Optics' EPC series of electrically driven polarization controllers provides a simple, efficient means to manipulate the state of polarization within a single mode (SM) fiber. Employing a novel mechanical fiber squeezing technique, the device is controlled by either three or four (depending on the model) input voltages that the user can vary over a ±5 V range to provide endless polarization control in a robust, easy to operate package. The EPC controllers’ rapid response speed easily handles changes in polarization caused by the external environment and is highly suitable for polarization scrambling for either averaging PDL effects or for making PMD or PDL measurements. Because the fiber within the device is continuous, all insertion losses, return losses, and PDL effects are limited only by the fiber itself. This makes it ideal for precise test and measurement applications. EPC polarization controllers are available in either a three or four channel configuration. The EPC-300 three-channel system is ideal for polarization scrambling applications such as for polarization averaging or PDL measurements. The added redundancy of the EPC-400 four-channel version opens the way to continuous polarization control, without having to occasionally reset the device when a controller reaches its limit. The unique design of the OZ Optics EPC series of polarization controllers means that they do not require any dedicated driver circuitry. There are no internal voltage multipliers or high voltage signals to worry about. Thus operation is safe and simple. Key Features: Negligible Insertion Losses Negligible Return Losses Negligible Polarization Dependent Losses (PDL) >100 Hz Response Speed Continuous Polarization Control Capability Low Voltage Applications: Polarization Scrambling; Polarization Stabilization; Polarization Mode Dispersion (PMD) Mitigation; Polarization Dependent Loss (PDL) Mitigation; PDL and PMD Measurement Systems; Interferometers and Sensors; OCT Systems

Manual Angled Cleaver; Fiber Type SM, PM; Fiber Diameter 125 µm; Buffer Diameter 250-900 µm; Cleave Angle 8° (±2°); Min. Cleave Length 8 mm Oxford Fiber’s Ox-SAC-08 is the world’s simplest angled cleaver. The single mode (SM) or polarization maintaining (PM) fiber is clamped under rubber rings at two points and bent down onto a sharp diamond blade. The optical fiber is cleaved so that its single mode or polarization maintaining core is at an angle of 8° from perpendicular. This way, the back-reflection from the cleaved end facet is is reduced to <-60dB, avoiding optical noise in telecom systems or eliminating reflections in fiber sensor arrays. If you require a cleaver for any other fiber type or a custom cleaver tailored to your specifications, please get in touch with the AMS Technologies fiber cleaving experts. Key Features: Staple Action for Easy Use Rugged Construction for Field Use 10 Position Diamond Bladed for Extended Life Blade Life: >10,000 Fibers Cleaved (Estimated) Benchtop and Handheld Operation Easy Fiber Loading Using Detachable Fiber Holder Compatible with Angled Mechanical Splice Offcut Bin, Tool Catch & Case Fiber Diameter: 125 μm SM or PM Buffer Diameter: 250 µm to 900 μm Cleave Angle: 8° (±2°) Dimensions (max): 67 mm x 40 mm x 79 mm Weight: 170 g Minimum Cleave Length: 8 mm – Set by Fiber Holder Applications: Mechanical Field-installed Connectors; Pigtailing Fiber to Semiconductor Emitters and Detectors; Removing End-reflections in Fiber-optic Sensing Applications

Wavelength 600-2300 nm; Bandwidth 0.05-1.2 nm; Reflectivity 5-99%; SLSR >8 dB; Fiber Type SM, PM, Double Clad, LMA, Custom; Fiber Pigtail Length ≥0.5, CustomGreitlex Photonics’ GTL-FBG-TB-890 tunable fiber Bragg gratings (FBGs) are a good solution for many applications – including those requiring a corrected central Bragg wavelength. An FBG’s central wavelength strongly depends on applied stress, with the mechanically induced strain linearly shifting the FBG’s central wavelength.The tunable fiber Bragg grating wavelength’s relative strain sensitivity is 0.78 * 10-6 µstrain-1. GTL-FBG-TB-890 tunable fiber Bragg gratings are boxed and operated manually. Athermal performance with an adjustment range of 2 nm is also possible. The gratings are available as bare fibers or with a variety of optical connectors. These FBGs replace similar products from the former FORC Photonics. The following configurations can be changed at the customer's request, please contact AMS Technologies to discuss a customized tunable fiber Bragg grating solution tailored to your project’s requirements.Key Features:Wavelength Range: 600 nm to 2300 nmWavelengths to Quick Order [nm]: 633, 780, 794, 797, 799, 801, 809, 830, 852, 895, 940, 976, 1030, 1057, 1060, 1064, 1080, 1125, 1150, 1178, 1240, 1270, 1310, 1484,1510 - 1580, 1650, 1900, 1908, 1952, 2300Fiber Type: Single Mode (SM), Polarization Maintaining (PM), Double Clad, LMA, CustomThermal Wavelength Stability (0°C to +60°C): <0.18 nmReflectivity: 5% to 99%Bandwidth (WFHM): 0.05 nm to 1.2 nmFBG Length: 1 mm to 20 mmAdjustment Range: 2 nmSLSR: >8 dBFBG Pigtail Length: ≥0.5 mFBG Recoating: On Customer Request Tensile Strength: >100 kpsiOptical Connector: Bare Fiber, FC/APC, LC/APC, CustomPackage Dimensions: 66 x 18 x 16 mmApplications: Where Corrected Central Bragg Wavelength is Necessary

760-1083 nm; Typ. Linewidth 0.6 MHz; Output Power 6-150 mW CW; Threshold Current ≤70 mA; Slope Efficiency 0.7 W/A; Side Mode Suppression Ratio ≥30 dBToptica eagleyard’s DFB series of distributed feedback (DFB) laser diodes features a built-in wavelength-selective grating stabilizing the wavelength. The DFB series’ entire resonator consists of a periodic structure. Thus, the devices operate on a single resonator mode emitting quasi-monochromatic radiation with a very small line width and low phase noise. The lasers can have very low-intensity noise because of the lack of mode partition noise. Due to the Gaussian mode the output is diffraction-limited.The choice of a distributed feedback design instead of a similar distributed Bragg grating (DBR) structure enables even a broader smooth tuning range around the operational point without the risk of experiencing spectral issues known as mode-hops, as these are given by design of a DBR diode, making the latter less suitable for the needs of atom spectroscopy.Special variants are available – two versions are intended to be used as seed lasers for pulsed fiber lasers, while other variants aim at oxygen detection as the emission wavelength of these laser diodes match with the strong absorption lines of oxygen at 760 nm and 764 nm while wavelength tuning around one of these absorption lines is possible.Further variants are especially suitable for spectroscopy with mode‐hop free operation and small linewidth guaranteed at the specified target wavelength for spectroscopic applications – these laser diodes are reaching the target wavelength by temperature tuning and allow wavelength tuning around this target wavelength.External backreflections may disturb the spectrum of these laser diodes, so the use of butterfly (BFW01) or TOC03 packages and effective optical isolation is recommended for spectroscopic applications requiring absolutely mode‐hop‐free tuning. Finally, special tunable variants with integrated optical isolators are available, enabling a wide mode‐hop free tuning range given by the specified operating temperature range and the specified power range.Key Features:Single Frequency ModeHigh Side Mode Suppression > 50 dBNarrow Linewidth <1 MHzPulse Width 1 to 50 nsPeak Power up to 500 mWRepetition Rate up to 1 MHzSMSR >35 dBProductWavelengthOutput PowerSpecificsDFB-0760-00012-1500-BFY12-0005760 nm12 mWoxygen detection, spectroscopy, metrologyDFB-0760-00040-1500-BFW01-0005760 nm40 mWoxygen detection with collimatorDFB-0760-00040-1500-TOV01-0005760 nm40 mWoxygen detection VCSEL replacementDFB-0760-00040-1500-TOC03-0005760 nm40 mWoxygen detectionDFB-0780-00020-1500-BFY12-0005780 nm20 mWoxygen detection,spectroscopy: Rb D2DFB-0780-00040-1500-BFY02-0000780 nm40 mWbasic variant with PM fiberDFB-0780-00040-1500-BFY02-0002780 nm40 mWtunable with PM fiberDFB-0780-00040-1500-BFW11-0005780 nm40 mWspectroscopy: Rb D2 with isolator and collimatorDFB-0780-00080-1500-TOV01-0005780 nm80 mWspectroscopy: Rb D2DFB-0780-00080-1500-BFW01-0002780 nm80 mWtunable with collimatorDFB-0780-00080-1500-BFW01-0005780 nm80 mWspectroscopy: Rb D2 with collimatorDFB-0780-00080-1500-TOC03-0000780 nm80 mWbasic variantDFB-0780-00080-1500-TOC03-0002780 nm80 mWtunableDFB-0780-00080-1500-TOC03-0005780 nm80 mWspectroscopy: Rb D2DFB-0785-00040-1500-BFY02-0000785 nm40 mWbasic variant with PM fiberDFB-0785-00040-1500-BFY02-0002785 nm40 mWtunable with PM fiberDFB-0785-00100-1500-TOV01-0000785 nm100 mWbasic variantDFB-0795-00015-1500-BFY12-0005795 nm15 mWspectroscopy: Rb D1 lineDFB-0795-00040-1500-BFW11-0005795 nm40 mWspectroscopy: Rb D1 with isolator and collimatorDFB-0795-00080-1500-BFW01-0005795 nm80 mWspectroscopy: Rb D1 with collimatorDFB-0852-00015-1500-BFY12-0005852 nm15 mWspectroscopy: Cs D2 DFB-0852-00050-1500-BFY02-0000852 nm50 mWbasic variant with PM fiberDFB-0852-00050-1500-BFY02-0002852 nm50 mWtunable with PM fiberDFB-0852-00100-1500-BFW01-0002852 nm100 mWtunable with collimatorDFB-0852-00100-1500-BFW01-0005852 nm100 mWspectroscopy: CS D2 with collimatorDFB-0852-00150-1500-TOC03-0000852 nm150 mWbasic variantDFB-0852-00150-1500-TOC03-0002852 nm150 mWtunableDFB-0852-00150-1500-TOC03-0005852 nm150 mWspectroscopy: Cs D2DFB-0895-00050-1500-TOV01-0005895 nm50 mWspectroscopy: Cs D1DFB-0935-00080-1500-TOC03-0004935 nm80 mWspectroscopy: YbDFB-1030-00500-1500-BFY02-00101030 nm500 mWseed laser (pulsed mode) with PM fiberDFB-1064-00025-1500-BFY12-00021064 nm25 mWtunable with isolator and PM fiberDFB-1064-00040-1500-BFY02-00001064 nm40 mWbasic variant with PM fiberDFB-1064-00040-1500-BFY02-00021064 nm40 mWtunable with PM fiberDFB-1064-00080-1500-TOC03-00001064 nm80 mWbasic variantDFB-1064-00080-1500-TOC03-00021064 nm80 mWtunableDFB-1064-00500-1500-BFY02-00101064 nm500 mWseed laser (pulsed mode) with PM fiberDFB-1083-00025-1500-BFY12-00021083 nm25 mWtunable with isolator and PM fiberDFB-1083-00080-1500-TOC03-00021083 nm80 mW Applications: Interferometry, Laser Doppler Velocimetry and Vibrometry; Cold Atoms; Optically Pumped Atom Clocks; Quantum Optics; THz Generation, Raman Spectroscopy; Cs- ,Rb- , K- Spectroscopy; Seed Laser for LIDAR SystemsPlease note that TOPTICA eagleyard products are not availble from us in Denmark, Finland, Iceland, Norway, and Sweden. 

Polarization Insensitive, Single/Dual Stage; 1528 to 1565 nm (C-Band); Isolation ≥30, ≥48 dB; Power Handling ≤500 mW; Fiber Type SMF-28e & Hi1060 Fiber WDM/Isolator hybrid is made by special packaging technology, which combines FWDM and isolator into a compact package. It has WDM and isolator function at the same time. It is widely used in EDFA and other fields. Key Features: Compact size Low insertion loss High channel isolation Low cost Applications: EDFA; WDM system; CATV

1250-1650 nm; Responsivity 25 A/W; Breakdown Voltage 40-70 V; Dark Current 1 nA; Package 3-pin TO 46 Wooriro’s APD module for OTDR applications is based on an InGaAs/InP avalanche photodiode (APD) in TO-46 package. This module’s APD is pigtailed, and the module can be ordered either without connector or with a SC, LC or FC type optical connector in UPC or APC version. Designed for an optical wavelength range of 1250 nm to 1650 nm, the APD module for OTDR features a very low dark current of 1 nA typical at 98% breakdown voltage. Typical responsivity is 25 A/W at 1550 nm wavelength and 10 nW optical input power. Key Features: InGaAs/InP Avalanche Photodiode APD Low Dark Current: 1 nA (Typical, @0.98 x Breakdown Voltage) High Reliability Optical Wavelength Range: 1250 nm to 1650 nm Responsivity: 25 A/W Typ. (VAPD = 0.98 VBR, λ = 1550 nm, Pin = 10 nW) Breakdown Voltage VBR: 40 V to 70 V (Id = 10 µA) Temperature Coefficient of VBR: 90 mV/°C (-40 °C to +85 °C) Dimensions: Ø 6 mm x Length 20.2 mm Applications: OTDR; Optical Sensor; Optical Test Instruments