General Photonics
BPD-002 Balanced Photodetector
InGaAs Photodetector; 1060, 1310, 1550 nm; Aluminium Enclosure; Responsivity 0.7 mA/mW; RF Bandwidth 0-200 MHz; Transimpedance Gain 3×104 V/A OCT and sensor systems require high-performance balanced photodetectors to increase system signal-to-noise ratio (SNR). General Photonics’ BPD-002 balanced photodetector module is specially designed for use in research and development, with ease of use and high performance as the primary design goals. The BPD-002 device is fully enclosed in a compact, sturdy aluminium box with two optical input ports, a balanced RF output port, two 1 MHz monitor ports and a power supply port. With a bandwidth up to 200 MHz, a transimpedance gain larger than 30K and a saturation power larger than 130 µW, the BPD-002 balanced photodetector is ideal for integration into laboratory or commercial OCT, fiber sensor, and high-performance optical measurement systems. Key Features: Low Noise and High Common Mode Rejection Ratio (CMRR) High Conversion Gain Wide RF Output Bandwidth (3dB): DC to 200, 100, 50, 10 or 5 MHz Wavelength Range: 1060, 1310 or 1550 nm ±50 nm Compact Size: 97 x 61 x 19 mm Photodetector Type: InGaAs Photodetector Responsivity: 0.7 mA/mW @1310 nm Transimpedance Gain: 3×104 V/A CW Balanced Saturation Power: >130 μW @ 1310 nm PD Input Power (linear range): 0 to 1 mW @ 1310 nm PD Power Damage Threshold: 20 mW Common Mode Rejection Ratio: >25 dB RF Output Voltage Range (at 50 Ω): ±1.8 V Applications: Optical Coherence Tomography; Fiber Sensing Interrogator; Instrumentation; Research and Development
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BPD-003 OEM Balanced Photodetector
InGaAs Photodetector; 1060, 1310, 1550 nm; Aluminium Enclosure; Responsivity >0.5->0.8 mA/mW; RF Bandwidth 0-200 MHz; Transimpedance Gain 100×103 V/A OCT and sensor systems require high performance balanced photodetectors to boost system signal-to-noise ratio (SNR). General Photonics’ BPD-003 OEM balanced photodetector module is specially designed for OEM applications in such fields, engineered for low cost and small size as well as high performance. The BPD-003 device consists of an optical head and a post-amplification board with an SMA or SMB RF output connector. The optical head has two input fibers aligned with a pair of matched photodetectors, selected for high CMRR and sensitivity, followed by an integrated low-noise transimpedance amplifier (TIA) placed immediately after the photodetectors to amplify received signals with low noise and enhanced CMRR. The integrated post-amplification circuit further conditions and amplifies the output of the detectors to a range of ± 3.5 V maximum. With a bandwidth of up to 200 MHz and a high conversion gain, the BPD-003 is ideal for integration into OCT, fiber sensor and high-performance optical measurement systems. Key Features: Very Low Noise Excellent Common Mode Rejection Ratio (CMRR): >15 (40 to 200 MHz), >35 dB (DC to 40 MHz) Photodetector Type: InGaAs Photodetector Responsivity: >0.5 to >0.8 mA/mW High Conversion Gain: >50 to >80 x 10³ mV/mW Wide RF Output Bandwidth: DC to 200 MHz Wavelength Range: 1060, 1310 or 1550 nm ±50 nm Polarization Dependent Loss (PDL): <0.2 dB Return Loss (RL): >45 dB Maximum Input Power: 10 mW Transimpedance Gain: 100 x 10³ V/A Fiber Type: SMF-28, HI1060 Compact Size: 49.5 x 21.6 x 16.5 mm Applications: Sensor Systems; Optical Coherence Tomography (OCT) Systems; Optical Measurement Systems; Fiber Sensing Interrogator; Instrumentation; Research and Development
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DEP Depolarizer
1310, 1550 nm; IL 1.0 dB; DOP <5%; ER <0.5 dB; RL 55 dB General Photonics’ DEP depolarizer module is a passive device (requiring no external power) that depolarizes laser output. The standard configuration can be used for coherence lengths less than 10 m. Custom units can be specified for coherence lengths of multiple kilometers. The DEP polarizer is ideal for minimizing the polarization sensitivity of fiber optic sensor systems such as systems for quasi-distributed temperature and strain sensing based on fiber Bragg gratings (FBG), systems for distributed temperature and strain sensing based on Brillouin or Raman scattering and systems for distributed acoustic sensing based on Rayleigh scattering. It can also help to eliminate the effects of PDL or polarization sensitivity of optical components and instruments. Equally important, it can be used for depolarizing pump lasers to eliminate the polarization sensitivity of Raman amplifiers. The DEP polarizer is packaged in a small (85 × 60 × 10 mm), rugged aluminium box, providing high performance and superb environmental stability. The internal structure and package size may be different depending on the coherence length or spectral width of the light signal to be depolarized. Contact AMS Technologies for an optimized configuration for your intended applications. Key Features: Customizable for Light Sources With Different Coherence Lengths Low Output Degree of Polarization (DOP): <5% Center Operating Wavelength: 1310, 1550 nm Wide Operating Wavelength Range: ±50 nm Low Insertion Loss: 1.0 dB Typical, 1.4 dB Maximum Compact Size: 85 × 60 × 10, 85 x 85 x 15 mm, Larger Package for Coherence Length >200 m No Power Source Required Coherence Length of Light Source: 10 m Standard, Others Specify Residual Extinction Ratio (ER): <0.5 dB Return Loss: 55 dB Optical Power Handling: ≥300 mW Fiber Type Input: PM Panda Fiber Fiber Type Output: SMF-28 Applications: Minimize Polarization Sensitivity of Fiber Sensors; Depolarize Pump Lasers; Remove Polarization Sensitivity of Raman Amplifiers; Eliminate Polarization Sensitivity of Optical Instruments; Eliminate the Effects of PDL; Can Be Integrated Into Remote Monitors
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DGD-1000 PMD Source
DGD Range 0-200, 0-44 ps; DGD Resolution 0.2 ps; Single Band C, L, O, Dual Band CL; Max. IL 3.5 dB; Max. PDL 0.3 dB; RL >50 dB Polarization mode dispersion (PMD) can seriously degrade the quality of high-speed fiber-optic data transmission. High-speed transceivers must meet stringent standards for PMD tolerance. General Photonics’ DGD-1000 PMD Source/Emulator accurately and repeatably generates both high and low values of differential group delay (DGD) or first-order PMD. Both the DGD and PDL are very stable over time and wavelength within the performance band. The DGD-1000 PMD source/emulator is available in different versions to accommodate the need for different wavelengths and DGD ranges. Key Features: Generates Differential Group Delay DGD up to 400 ps DGD Range: 0 to 200 ps, 0 to 400 ps DGD Resolution: 0.2 ps DGD Change Rate: Up to 64 ps/s Wavelength Range Single Band: C Band, L Band or O Band Wavelength Range Dual Band: CL Bands Insertion Loss (IL): ≤3.5 dB Very Low Insertion Loss (IL) Variation Over DGD Range: 0.1 dB typ. Very Low Polarization Dependent Loss (PDL) Over DGD Generation Range: 0.3 dB max., 0.1 dB typ. Return Loss: >50 dB Slow SOP Variation: <1 rad/min Small DGD Variation Over Time: <0.1 ps Over 8 Hours Extended Version Can Cover up to 600 ps as Special Order Applications: System PMD Tolerance Testing; 1st Order PMD Performance Simulation
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DOP-201 Degree of Polarization Meter
1260-1620 nm; DOP Accuracy 0.2%, 0.5%; DOP Range 0-100%; DOP Resolution 0.01%; Operating Power Range -40-6dBmThe DOP-201 system from Luna measures and displays the degree of polarization (DOP) of a light source in real time on the front panel display. The instrument incorporates a patented maximum & minimum search technique that accurately measures both low and high DOP with a wide dynamic range. This technique is superior to polarimeter-based methods that are inaccurate at low values of DOP as well as scrambler-based methods which are less accurate at high values of DOP.The instrument's wide wavelength range includes the S, C and L bands, without calibration. Simultaneous measurement of DOP and optical power level of the light source under test can be used to obtain DOP power dependence and to ensure low insertion loss during depolarizer manufacturing.The DOP-201 degree of polarization meter is ideal for characterizing the performance of depolarizers and depolarized light sources, such as ASE and SLED sources and the pumps for Raman amplifiers. It can also be used to monitor the OSNR (optical signal-to-noise ratio) and PMD (polarization mode dispersion) of optical signals, and to measure the noise figure of optical amplifiers.The DOP-201 features fast measurement, high accuracy and resolution, a wide operating power range, a bright OLED display and an analog output port for easy integration in automated depolarizer manufacturing stations.Key Features:Rapid Measurement Speed: 30 msDegree of Polarization (DOP) Wavelength IndependenceHigh DOP Accuracy: ±0.5% for Single Sample, ±0.2% for 10 Sample AverageWide Operating Wavelength Range: 1260 to 1620 nmDOP Range: 0 to 100%DOP Resolution: 0.01%Operating Power Range: -40 to 6 dBmFront Panel Real-time DisplayAnalog OutputDimensions: 356 x 216 x 89 mmApplications: Characterizing Depolarizers and Depolarized Light Sources, Such as ASE and SLED Sources and the Pumps for Raman Amplifiers; Monitoring OSNR and PMD of Optical Signals; Measuring the Noise Figure of Optical Amplifiers; Depolarizer Manufacturing and QC; Fiber Gyro Coil Characterization; ROADM Manufacturing
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ERM-202 Extinction Ratio Meter
600-1620 nm; No. of Channels 1, 2; PER Resolution 0.1 dB; PER Dynamic Range >40, >50 dB; Angular Resolution 0.06 dB; Input Optical Power Range -30-10 dBm; Power Resolution 0.02, 0.2 dB; Measurement Speed 0.1-10 sLuna’s ERM-202 is a single or dual channel polarization extinction ratio (PER) meter. When used with a broadband source, it directly measures PER. Single and dual channel models are available. The single channel instrument can be upgraded to a dual-channel version at a later date.The dual channel version is specifically designed to simultaneously measure the PER and power ratio of a device with two polarization maintaining (PM) outputs, such as a Y-branch fiber gyro IOC, PM coupler (PMC), or polarization beam splitter (PBS), as well as evaluate the performance (output DOP) of depolarizers.By combining low-noise circuitry with a high-resolution stepper, the ERM series achieves a PER dynamic range of 50 dB and an angular resolution of 0.06°, outperforming all competitors in its class. These instruments feature OLED displays with a high contrast bright readout that allows the data to be observed from several feet away. The instruments can be operated from the front panel or via remote control.The operator can choose from four measurement speeds ranging from 0.1 to 1 s/cycle to optimize speed or accuracy and can observe multiple parameters on the front panel screen including PER, axis angle, power ratios, and optical power. The measurement data can be stored and recalled for comparison purposes from the front panel as well. Full digital or remote control is included for unattended or system applications.Key Features:One or Two Measurement ChannelsFree-space InputFront Panel or Remote ControlSimultaneous Polarization Extinction Ratio (PER) and Power Ratio TestingPER Resolution: 0.1 dBPER Dynamic Range: >40, >50 dB High Angular Resolution: 0.06 dBOperating Wavelength Range: 1260 to 1620 nm, 960 to 1160 nm, 600 to 850 nmInput Optical Power Range -30 to 10 dBmPower Resolution: 0.02, 0.2 dBMeasurement Speed: 0.1 to 10 sBright OLED DisplayStore and Recall FunctionsDimensions: 356 x 216 x 89 mmApplications: Verification of PM Connectorization and Splices; Testing PM Fiber Coils; Simultaneous Measurement of PER and Power Ratio; Testing Y-branch Fiber Gyro IOCs; Testing PM Couplers (PMC) or Polarization Beam Splitters (PBS); Evaluating the Performance of Depolarizers; Laser Diode PM Fiber Pigtailing; PM Fiber Patchcord Production; PM Fiber Fusion Splicing QA; PM Fiber Coil and Fiber Gyro QA
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FDE-002 Fixed Differential Group Delay
1550 nm; DGD 0-45 ps; RL 55 dB; IL 0.8 dB; Fiber Type SMF-28; PDL <0.2 dBLuna’s FDE-002 fixed differential group delay (DGD) artifacts eliminate the need for precise measurement of polarization maintaining (PM) fiber lengths to add defined amounts of first order PMD to a system.DGD values of up to 45 ps are available in the FDE-002 fixed differential group delay standard size package. Larger DGD values are also available by special request.Key Features:Large 1st Order PMD: up to 45 psLow Insertion Loss (IL): <1 dB (0.8 dB Typical)Operating Wavelength: 1550 ± 50nmDGD Value: 0 to 45 ps Standard, Larger Values on RequestDGD Calibration Accuracy: ±(1 fs + DGD x 0.5%)Insertion Loss (intrinsic): < 1 dB (0.8 dB typical)Polarization Dependent Loss (PDL): <0.2 dBReturn Loss (RL): 55 dBPower Handling: >300 mWFiber Type: SMF-28Dimensions: 108 × 7.9 x 7.9 mmApplications: PMD Emulation; PMD Compensation; TDM Bit Alignment
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FPS-001 Phase Shifter
980-1650 nm; Total Phase Shift >8π; IL <0.1 dB; RL >65 dB; PDL <0.05 dB; Residual Amplitude Modulation ±0.01 dBLunas’ 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 dBLow Residual Amplitude Modulation: ±0.01 dBNoTail™ Version AvailableOperating Wavelength: 1260 to 1650, 980 to 1310 nmReturn Loss (RL): >65 dBTotal Phase Shift (0 to 20 kHz): >8πHalf-wave Voltage (0 to 20 kHz): <20 VPolarization Dependent Loss (PDL): <0.05 dBMaximum Applied Voltage: 150 VDimensions: 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
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FPS-002 Phase Shifter
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 dBCoherent 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. Lunas 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 nmTotal 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 nmFiber Type: ClearCurve ZBL, HI1060, 780 HP, PM, PM980XPCapacitance of Piezo: 0.18 µFMaximum Applied Voltage: 150 VCompact 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
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FPS-003 Phase Shifter
780-1550 nm; Total Phase Shift >55π; IL <0.5 dB; RL >55 dB; PDL <0.05 dB; Residual Amplitude Modulation ±0.01 dBLunas 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 Lunas 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 nmLow Half-wave VoltageLarge Phase Shift RangeCompact Size: 31 x 31 x 14.5 mmLow 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, OtherHalf-wave Voltage (Vπ @ 500 Hz): 1 to 3 V TypicalResonance Frequency: 36 to -39 kHz TypicalVπ at Resonance Frequency: <150 mV TypicalPolarization Dependent Loss (PDL): <0.05 dB at 1550 nmCapacitance of Piezo: 5 to 12 nFMaximum Applied Voltage: 150 VApplications: Fiber Interferometers; Fiber Laser Systems; Fiber Sensor Systems
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MDL-002 Fiber Optic Delay Lines
840-1650 nm; Delay Range 0-1,120 ps; RL 50 dB; Fiber Type SMF-28, HI1060, HI780, PM Panda, PM 980 Panda; IL 1.0, 1.5 dB; PDL 0.1, 0.2 dBLunas MDL-002 family of motorized variable fiber optic optical delay lines allow optical path length adjustment of up to 560 ps in a single pass. Driven by a DC motor with an integrated encoder, the MDL-002 has a delay resolution of less than 0.3µm (1 fs).In addition, its advanced motion design guarantees longevity for long-term continuous operation. Low insertion loss and high reliability make this device ideal for integration in optical coherence tomography (OCT) systems, network equipment and test instruments for precision optical path length control or timing alignment.Three configurations of the MDL-002 fiber optic delay line series are available:Integrated unit for use as a bench-top instrument for laboratory applicationsTwo-piece unit with the optical head and control unit separated for installation into customer equipmentOEM version with a miniature controller boardAll three versions can be remote controlled by a PC or a micro-processor through an RS-232 interface. The delay line is available with either single mode (SM) or polarization maintaining (PM) fiber pigtails.Key Features:High Optical Delay Resolution: 0.3 µm / 1 fs, 0.6 µm / 2 fs Per Encoder CountLow BacklashLow Insertion Loss (IL): 1.0, 1.5 dB TypicalInsertion Loss Variation: ±0.3, ±0.5, ±0.7 dB Over EntireHigh Delay-to-Length RatioOptical Delay Range: 0 to 330, 0 to 560, 0 to 1,120 psOperating Wavelength: 840 to 1650 nmPosition Accuracy: ±3, ±6 µmPosition Repeatability: ±3, ±6 µmPolarization Dependent Loss (PDL): 0.1, 0.2 dB MaximumReturn Loss (RL): 50 dBExtinction Ratio: >18 dB (For PM Model)Optical Power Damage Threshold: 300 mWControl Mode: Panel Keypad and RS-232 InterfaceFiber Type: SMF-28, HI1060, HI780, PM Panda, PM 980 PandaDimensions: 178 x 102 x 41, 229 x 112 x 41 mm (Integrated Unit), 65 x 65 x 21.5 mm (Mini Controller Board), 132/157 x 37 x 18 mm (Optical Head)Applications: Optical Coherence Tomography (OCT) Systems; Scientific Instrument Control; Network Optical Path Length Control or Timing Alignment; Optical Fourier Spectrum Analysis; Optical Interferometry; Delay Generation and Measurement; Optical Time Division Multiplexing (OTDM); Fiber Sensors
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MDL-003 Fiber Optic Delay Line
840-1650 nm; Delay Range 0-100, 0-200 ps; RL 55 dB; Fiber Type SMF-28, HI780, HI1060, PM Panda; IL 1 dB; PDL 0.15 dBLunas motorized variable optical delay line is the smallest delay line in the MDL series of products, with a total volume of less than 2 cubic inches. The MDL-003 provides low-cost, precision optical path length adjustment and delay scanning functionality. This addition to the MDL product line is specifically designed for OEM applications that require continuous scanning capability and a small footprint.The standard MDL-003 motorized variable optical delay line has a delay range of 100 ps; however an internal mirror can be installed to double pass the light, thereby doubling the delay range. The device uses a stepper motor and dual position sensors for precise control. A small controller board is available as an option.Key Features:High ResolutionLow BacklashLow Insertion Loss (IL): 1 dBInsertion Loss Variation: ±0.3 dB Over Entire RangeHigh Delay-to-Length RatioOperating Wavelengths: 840, 1060, 1310, 1550 or 1260 to 1650 nmOptical Delay Range: 0 to 100 ps, Single-passOptical Delay Resolution: 30 μm, Single-pass at Maximum SpeedOptical Delay Accuracy: ±40 μm, Single-pass at Maximum SpeedOptical Delay Repeatability: ±40 μm, Single-pass at Maximum SpeedPolarization Dependent Loss (PDL): 0.15 dB (SM Fiber)Return Loss (RL): 55 dBExtinction Ratio: >18 dB (PM Model)Actuation Speed: 50 ps/s (Single-pass) MaximumOptical Damage Power Threshold: 100 mWFiber Type: SMF-28, HI780, HI1060, PM PandaDimensions: 51 x 36 x 14 mmApplications: Optical Coherence Tomography (OCT) Systems; Scientific Instrument Control; Network Optical Path Length Control or Timing Alignment
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MPC Polarization Controller
1260-1650 nm; IL 0.05 dB; PMD 0.05 ps; AL <0.01, <0.05 dB; RL >65 dB; Max. Rise & Fall Time 30 µsLunas MPC all fiber polarization controller module is packaged in a low-profile, 16 mm high enclosure, suitable for system integration and mounting on a PCB. The module’s low height is especially advantageous for integration in test equipment, fiber sensors, fiber lasers and optical network modules.Available with three (-3x) and four channels (-4x), the MPC polarization controller module features an all-fiber design with inherently low loss, minimal activation loss and minimal back reflection. A special athermal design leads to stable operation over a wide range of temperatures (-25 to +80 °C).Combined with Lunas miniature piezo driver card, it can be controlled either by a digital or analog signal to obtain any desired polarization output from an arbitrary input polarization state.Key Features:OEM PackagingAll-fiber DesignLow Intrinsic Insertion Loss: 0.05 dBLow Back Reflection – Return Loss: >65 dBFast Response – Maximum Rise and Fall Time: 30 µsOperating Wavelength Range: 1260 to 1650 nm Maximum Activation Loss (AL): 0.01, 0.05 dBPolarization Mode Dispersion (PMD): 0.05 psCompact Size – Dimensions: 65.5/83 x 20.3 x 16 mmApplications: Polarization Stabilization; Compensate PMD in Fiber Sensing Systems; Polarization Demultiplexing; Fiber Sensor; Fiber Laser; Testing Equipment
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MPC-201 Polarization Controller
980-1620 nm; Multiple Polarization Control Modes; IL <0.6 dB; PDL <0.1 dB; PMD <0.2 ps; AL <0.1 dB; RL >50 dBControlling the state of polarization (SOP) of an optical signal has never been easier – Lunas MPC-201 multifunction polarization controller has four operational modes for complete polarization control: variable rate polarization scrambling, manual polarization adjustment, polarization modulation, and externally triggered random SOP generation.Four different polarization scrambling methods enable the SOP to a) trace out a spiral pattern about a static or rotating axis with a nearly uniform SOP variation rate for system stress tests (Tornado scrambling); b) generate a continuous trace with a Rayleigh distribution of SOP variation rate, for emulation of the SOP variation in a fiber link (Rayleigh scrambling); c) generate a continuous trace with uniform sphere coverage for PDL measurement (Triangle scrambling); or d) evenly cover the Poincaré sphere with discrete, random points at a uniform rate (Discrete scrambling).In the SOP modulation mode, each polarization control axis can be selectively controlled with a sine, square, or triangle wave of user defined frequency and amplitude. Each polarization control axis can also be controlled manually, by setting the input voltage either from the front panel controls or through a remote control interface. In externally triggered scrambling mode, discrete, random SOPs are generated in response to a trigger input, a feature desirable for recirculating loop applications or other applications requiring synchronization with other devices.Finally, the MPC-201 can emulate the Agilent 11896A polarization scrambler function, allowing it to act as a plug-in replacement for this popular but discontinued device, while offering many more advanced features. The MPC-201 polarization controller puts the user in control.Key Features:Multiple Polarization Control ModesTornado Scrambling (Quasi-uniform Rate Distribution): 0.00 to 2,000 Revolutions/sReal Fiber SOP (State of Polarization) Variation Emulation (Rayleigh Rate Distribution): 0.00 to 2,000 rad/sDiscrete Random States SOP Scrambling: 0.00 to 20,000 Points/sTriangle Polarization Scrambling: 0.00 to 2,000 x 2π rad/sAgilent 11896A Scrambling Emulation: Speed Settings 1 to 8, Matched to 11896A SettingsSOP ModulationOperating Wavelength Range: 1260 to 1620 nm, 980 to 1310 nmManual Polarization Control: 4 Channels, 0 to 4π Each ChannelLow Insertion Loss (IL): <0.5 dB With ConnectorsLow Polarization Dependent Loss (PDL): <0.05 dB With ConnectorsLow Polarization Mode Dispersion (PMD): <0.1 ps With ConnectorsLow Activation Loss (AL): <0.05 dB With ConnectorsReturn Loss: >50 dB With ConnectorsOptical Power Handling: 1,000 mWBright OLED DisplayApplications: Recirculating Loop Studies; Automated Testing; Real Fiber Emulation; SOP Variation Emulation; PMD Emulation; Polarization Scrambling; System Polarization Studies; PDL/DOP Measurement
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MPC-202 Polarization Controller
980-1620 nm; SOP Change Rate >360 krad/s; IL <0.6 dB; PDL <0.1 dB; PMD <0.2 ps; AL <0.1 dB; RL >50 dBLunas MPC-202 advanced multifunction polarization controller is specially designed to meet the requirements of coherent receiver performance tests.MPC-202 combines Luna award winning PolaRite™ II/III polarization controller with proprietary polarization control algorithms to achieve a wide range of polarization control functionalities, including high-speed quasi-uniform rate polarization scrambling, random-rate polarization scrambling with Rayleigh rate distribution, discrete-state polarization scrambling with high slew rate, sine, square, and triangle-wave SOP (state of polarization) modulation, and manual polarization control functions.In particular, the “Tornado” quasi-uniform rate polarization scrambling function can achieve a high SOP scrambling rate of up to 60,000 revolutions/s (more than 360 krad/s) with a narrow rate distribution clustered around the highest rate.In short, the MPC-202 is an ideal tool for production or laboratory testing of polarization related functions and parameters, including passive/active component characterization, performance tests of fiber optic interferometers, sensor systems, RF photonics systems, etc. The quasi-uniform rate high-speed scrambling function is particularly useful for SOP tracking speed testing of coherent receivers, and the square wave SOP modulation function is ideal for SOP recovery time tests.Key Features:Quasi-uniform Rate SOP (State of Polarization) ScramblingSOP Change Rate: >360 krad/sScrambling With Rayleigh Rate DistributionDiscrete SOP ScramblingSOP ModulationOperating Wavelength Range: 1260 to 1620 nm, 980 to 1310 nmTornado Polarization Scrambling: 0.00 to 60,000 Revolutions/sMean Rayleigh Rate Distribution Polarization Scrambling: 0.00 to 2,000 rad/sTriangle Polarization Scrambling: 0.00 to 2,000 x 2π rad/sDiscrete Random States Polarization Scrambling: 0.00 to 20,000 points/sManual Polarization Control: 4 Channels, 0 to 4π Each ChannelLow Insertion Loss (IL): <0.6 dB With ConnectorsLow Polarization Dependent Loss (PDL): <0.1 dB With ConnectorsLow Polarization Mode Dispersion (PMD): <0.2 ps With ConnectorsLow Activation Loss (AL): <0.1 dB With ConnectorsReturn Loss: >50 dB With ConnectorsOptical Power Handling: 1,000 mWBright OLED DisplayApplications: Laboratory Testing of Polarization-related Parameters; Performance Tests of Fiber Optic Interferometers and Systems; SOP Tracking Speed Testing of Coherent Receivers
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MPC-203 Polarization Controller
980-1620 nm; SOP Change Rate ≤11 Mrad/s; IL <0.6 dB; PDL <0.1 dB; PMD <0.2 ps; AL <0.1 dB; RL >50 dBLunas MPC-203 high-speed multifunction polarization controller is specially designed to meet the high SOP (state of polarization) scrambling requirements needed for stress testing a coherent receiver’s polarization tracking performance.MPC-203 combines Lunas award winning PolaRite™ II/III polarization controller with proprietary polarization control algorithms to achieve a wide range of polarization control functionalities, including high-speed polarization scrambling with a maximum SOP change rate of up to 11 Mrad/s.Unlike other high-speed polarization scramblers found in the market, this all-fiber, pass-through design ensures low insertion loss (IL), polarization dependent loss (PDL), polarization mode dispersion (PMD) and activation loss (AL).Key Features:High-speed SOP (state of polarization) ScramblingSOP Change Rate up to 11 Mrad/sScrambling With Rayleigh Rate DistributionDiscrete SOP ScramblingSOP ModulationOperating Wavelength Range: 1260 to 1620 nm, 980 to 1310 nmTornado Polarization Scrambling: 0 to 11 Mrad/sMean Rayleigh Rate Distribution Polarization Scrambling: 0.00 to 2,000 rad/sTriangle Polarization Scrambling: 0.00 to 2,000 x 2π rad/sDiscrete Random States Polarization Scrambling: 0.00 to 20,000 points/sManual Polarization Control: 4 Channels, 0 to 4π Each ChannelLow Insertion Loss (IL): <0.6 dB With ConnectorsLow Polarization Dependent Loss (PDL): <0.1 dB With ConnectorsLow Polarization Mode Dispersion (PMD): <0.2 ps With ConnectorsLow Activation Loss (AL): <0.1 dB With ConnectorsReturn Loss: >50 dB With ConnectorsOptical Power Handling: 1,000 mWBright OLED DisplayApplications: SOP Response Test of Coherent Receivers; SOP Tracking Speed Test; PMD and PDL Related Tests; SOP Variation Emulation; Polarization Scrambling
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MZI-001 Mach-Zehnder Interferometer
1060, 1310, 1550 nm; Wavelength Range ±70 nm; FSR 10-100 GHz; Detector Responsivity >0.8 A/W; Connector Type FC/APC, FC/PC, SpecifyLunas’ MZI-001 is a fiber pigtailed Mach-Zehnder free space interferometer that detects changes in optical frequency. The device comes with two high-speed photodetectors for the balanced detection of the two complementary outputs of the interferometer.The free spectral range (FSR) or zero-cross spacing of the device is defined to within 1. The FSR is user-defined between 10 GHz and 100 GHz. The MZI-001 interferometer’s free-space optical design eliminates polarization sensitivity.Key Features:Accurate Free Spectral Range (FSR): 10 to 100 GHz, User SelectableFSR Tolerance: 2%Center Wavelength: 1060, 1310, 1550 nmWavelength Range: ±70 nmDetector Responsivity: >0.8 A/WDetector Rise/Fall Time: 0.3 ns With 50 Ω LoadDetector Capacitance: 0.7 pFTemperature StablePolarization InsensitiveFine Optical Frequency SpacingBalanced PhotodetectorsReturn Loss (RL): 55 dBPolarization Dependent Loss (DPL): <0.5 dBInput Fiber: SMF-28 or HI1060 Fiber With 900 µm BufferOptical Connectors: FC/APC, FC/PC, SpecifyCompact Size: 53.6 x 28 x 9.4 mmApplications: Determining Instantaneous Wavelength of Swept Source; Clocking Optical Coherence Tomography (OCT) Platforms; Detecting Drift in Fiber Sensor Systems; Detecting Drift of Lasers in Coherent Detection Systems; Spectrum Analysis
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OCA-1000 Optical Component Analyzer
1260-1620 nm; 8-40 Channels; PDL Measurement Range 0-20 dB; PDL Resolution 0.01 dB; IL Measurement Range 0-60 dB; IL Resolution 0.002 dB; Optical Power Range -60-8 dBm; Optical Power Accuracy ±0.5 dB Lunas’ OCA-1000 is a multi-channel optical component analyzer that simultaneously measures insertion loss (IL), polarization dependent loss (PDL), and optical power (P) on multiple optical paths. The measurement is based on the Mueller Matrix method, which offers fast characterization of wavelength dependent optical parameters that are critical in today’s optical communication systems.The OCA-1000 base model can have up to eight channels. Custom 8- or 16-channel expansion units can be added to increase the system capacity to up to 40 channels. The instrument comes with a control program with built-in functions to display measured power, IL, and PDL vs. wavelength or to monitor the time variation of power/IL for all channels simultaneously to determine their stability. For AWG characterization, the data analysis software also calculates passband center wavelength, bandwidth, and flatness as well as inter-channel crosstalk (from adjacent and nonadjacent channels).The OCA-1000 optical component analyzer is an ideal solution for easy, accurate characterization of components and modules with multiple outputs, including DWDMs, ROADMs, AWGs and PLCs. It can be used with various tunable lasers , such as those from Keysight or Santec. This flexibility makes full use of existing laser resources and reduces the cost of making such measurements. Its rapid measurement reduces the time required to characterize devices with large numbers of ports, enabling higher production throughput.Key Features:Wide Wavelength Range: 1260 to 1360 nm (O-Band), 1480 to 1620 nm (C- & L-Bands)Number of Channels: 8 to 40PDL Measurement Range: 0 to 20 dBHigh Polarization Dependent Loss (PDL) Accuracy: ±(0.02 + 2% of PDL) dB @PDL<10dB, ±(0.02 + 5% of PDL) dB @10<PDL<20dBPDL Resolution: 0.01 dBInsertion Loss (IL) Measurement Range: 0 to 55 dB, 0 to 60 dBIL Resolution: 0.002 dBOptical Power Range: -60 to 8 dBmOptical Power Accuracy: ±0.5 dBHigh Channel-to-channel UniformityUser-friendly Control SoftwareIntegration Time of Power Meter: 0.5 to 1,000 msDimensions: 19”-Rack-Mountable Enclosure, 1 U, 305 mm DepthApplications: PDL or IL vs. Wavelength Measurement; IL or Power vs. Time Measurement; DWDM Component Passband Characterization: Center Frequency, BW, Ripple, Noise Floor; Fiber Optic Component Characterization; Network Component Characterization (e.g. DWDM, ROADM); Planar Lightwave Circuits (PLC); Photonic Integrated Circuits (PIC)
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OCDR-1000 Optical Coherence Domain Reflectometer
1310, 1550 nm; Dynamic Range >80 dB; Scan Range 600 mm; Spatial Resolution 10-25 µm; RL Range 10-90 dB; Sweep Speed 20 mm/sLunas’ OCDR-1000 is an optical coherence domain reflectometer designed to obtain space-resolved reflection information inside a fiber optical component, such as a photonic integrated circuit (PIC), for diagnosing quality or design issues. It is based on a polarization optimized white light interferometer proprietary to General Photonics.The OCDR-1000 optical coherence domain reflectometer performs the functions of the discontinued Agilent 8504B Reflectometer – and more – but with better polarization management, spatial resolution and accuracy; larger scan range and dynamic range; and smaller size and weight.The OCR-1000 is a low-cost alternative to OFDR technology, with a much higher dynamic range that avoids the masking of small reflection peaks by the large reflections typical of the input surface of an optical device.The OCDR-1000 optical coherence domain reflectometer can measure devices with a length of up to 600 mm. A set of length-matching delay modules is available to match the pigtail lengths of the devices to be measured and place the measurement span in the region of interest. With a reflection dynamic range of over 80 dB and a spatial resolution down to 10 µm, this instrument helps engineers and researchers see the inside of an optical device to precisely identify defects and their locations.Key Features:Dynamic Range: >80 dBScan Range: 600 mm (400 mm in Fiber)Spatial Resolution: 10 to 25 μmOperating Wavelengths: 1310, 1550 nm, Others on RequestReturn Loss (RL) Range: 10 to 90 dBSweep Speed: 20 mm/sCompact & LightweightBuilt-in Light SourceAverage Light Source Power: >-3 dBmPerforms Functions of Discontinued Agilent 8504B Reflectometer - and MoreDimensions: 89 x 356 x 356 mmApplications: Optical Characterization of Photonic Integrated Circuits, Fiber Optic Components; Accurate Measurement of Return Loss, Distributed Reflectivity
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PBPD-001 Polarization Diverse Balanced Photodetector
Polarization Diverse Photodetector; 1310, 1550 nm; Aluminium Enclosure; Signal Conversion Gain >30 V/mW; RF Bandwidth 0-210 MHz; Transimpedance Gain 3x104 V/AOCT and sensor systems require high-performance balanced photodetectors to increase system signal-to-noise ratio (SNR). Polarization-sensitive OCT and similar applications require separate analysis of the two polarization components of a signal.Lunas’ PBPD-001 polarization diverse balanced photodetector module is specially designed for use in such systems and adds polarization sensitivity to the balanced photodetector circuitry of the BPD-002 or BPD-003 balanced photodetector modules.The PBPD-001 polarization diverse balanced photodetector is fully enclosed in a compact, sturdy aluminium box with two optical input ports, a balanced RF output port and two monitor ports for each polarization component and a 12 VDC power supply port.With a bandwidth up to 200 MHz, a transimpedance gain larger than 30K and a saturation power larger than 130 μW, the PBPD-001 polarization diverse balanced photodetector is ideal for integration into laboratory or commercial OCT, fiber sensor, and high performance optical measurement systems with polarization dependent detection requirements.Key Features:Low NoiseHigh Common Mode Rejection Ratio (CMRR): >25 dBHigh Signal Conversion Gain: >30 V/mW (Interference Signal)Wide RF Output Bandwidth (3dB): DC to 210 MHzWavelength Range: 1310 or 1550 nm ±50 nmCompact Size: 100 x 80 27 mmPolarization Crosstalk: <25 dBTransimpedance Gain: 3×104 V/ACW Balanced Saturation Power (At Input): >150 μWCommon Mode Rejection Ratio: >25 dBRF Output Voltage Range (at 50 Ω): ±1.75 VApplications: Polarization Sensitive OCT Systems; Polarization Resolved Sensing; Fiber Optic Distributed Sensing; Instrumentation; Research and Development
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PCD-005 Polarization Scrambler
980-1660 nm; IL <0.05, <0.6 dB; PDL <0.05 dB; PMD <0.05 ps; Residual Amplitude Modulation <±0.01 dB; Residual Phase Modulation <0.1π; RL >65 dBLunas’ PCD-005 polarization scrambler is an all-fiber design module that randomizes polarization states. This module is designed to be easily plugged into sensor equipment or measurement instruments with minimal development effort.The digital control circuitry delivers uniform SOP distribution over a wide operation temperature range, making it a good choice for sensor field applications. The PCD-005 polarization scrambler module can be remote controlled via RS-232 to set the operation wavelength or enable/disable the scrambling operation.The PCD-005 delivers superior performance with extremely low insertion loss, back reflection, and residual phase and amplitude modulation.Key Features:Minimal Insertion Loss (IL): <0.05 dB Without Connectors, <0.6 dB With ConnectorsMinimal Back Reflection: Low Residual Phase Modulation: <0.1πLow Residual Amplitude Modulation: <±0.01 dBRS-232 Control OptionRemote Operation Wavelength ControlCenter Operating Wavelengths: 980 to 1660 nmOperating Wavelength Range: >100 nmOutput Degree of Polarization (DOP): <5%Average Polarization Mode Dispersion (PMD): <0.05 psIntrinsic Polarization Dependent Loss (PDL): <0.05 dB Return Loss: >65 dB Without ConnectorsOptical Power Handling: >1,000 mWBoard Dimensions: 220 x 100 x 30 mmApplications: Eliminate Polarization Sensitivity; Add Optional Capability to Sensor Systems
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PCD-104 Polarization Scrambler
980-1600 nm; Residual Phase Modulation <0.1 π; Residual Amplitude Modulation <±0.01 dB; PMD <0.05 ps; PDL <0.05 dB; IL <0.05, <0.6 dB; RL >65 dBLunas’ PCD-104 polarization scrambler uses a breakthrough patented all-fiber technology to effectively randomize polarization states. Specifications include low insertion loss and low back reflection as well as minimal phase and amplitude modulation. The instrument can be used in automatic test systems under remote control through digital interface options.Depolarizing by polarization scrambling has many important applications. Scrambling the input polarization can eliminate measurement uncertainties caused by the polarization sensitivity of the testing device. Performance degradation due to polarization dependent gain (PDG) induced in optical amplifiers can also be suppressed by polarization scrambling. In addition, polarization scrambling can be used in systems to facilitate and simplify PMD monitoring.The PCD-104 polarization scrambler delivers superior performance, including extremely low insertion loss, back reflection, and residual phase and amplitude modulation.Key Features:Minimal Insertion Loss (IL): <0.05 dB Without Connectors, <0.6 dB With ConnectorsMinimal Back ReflectionOptical Return Loss (RL): >65 dB Without ConnectorsLow Residual Phase Modulation: <0.1 πLow Residual Amplitude Modulation: <±0.01 dBRemote Operation Wavelength ControlBuilt-in RS-232, GPIB and Ethernet PortsCenter Operating Wavelength: λ Range 1 1310, 1480, 1550, 1600 nm, λ Range 2 980, 1060, 1310 nmOperating Wavelength Range: >100 nmOutput Degree of Polarization: <5%Average Polarization Mode Dispersion (PMD): <0.05 psIntrinsic Polarization Dependent Loss (PDL): <0.05 dBOptical Power Handling: >1,000 mWApplications: PDG Mitigation; Elimination of Polarization Sensitivity; Facilitating PMD Emulation; Facilitating PMD Compensation; Enables PDL Measurement
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PCD-M02 Polarization Controller
980-1650 nm; 3, 4 Channels; Polarization Control Range 0-4π Each Channel; IL <0.05, <0.6 dB; PDL <0.05 dB; PMD <0.05 ps; AL <0.01, <0.05 dB; RL >65 dBLunas’ PCD-M02 polarization controller module integrates an all-fiber dynamic polarization controller with a miniature piezo driver card, so that the SOP of the signal can be directly controlled either by a 0 to 5 V analog control signal or a 12-bit TTL digital control signal.The 3- or 4-channel polarization controller module features an on-board high voltage DC/DC converter, so no external high voltage power supply is required. The card can be configured to accept either a ±12 VDC power supply or an optional external 160 V power supply.As a polarization controller, the PCD-M02 can convert any input polarization state to any desired output polarization state. As a scrambler, it can randomize the output polarization state. This module offers the low insertion loss, low back reflection, and low activation loss needed for test and measurement applications, combined with the compact size needed for system integration or handheld devices.Key Features:Minimal Insertion Loss (IL): <0.05 dB Without Connectors, <0.6 dB With ConnectorsMinimal Activation Loss (AL): 0.01 dB, 0.05 dB Fast ResponseDigital and Analog ControlCompact SizeOperating Wavelength Range: 1260 to 1650 nm, 980 to 1310 nmPolarization Control Range: 3 or 4 Channels, 0 to 4π Each ChannelLow Polarization Dependent Loss (PDL): <0.05 dB Low Polarization Mode Dispersion (PMD): <0.05 ps Return Loss: >65 dBOptical Power Handling: 1,000 mWBoard Dimensions: 100 x 100 x 17.5 mmApplications: Polarization Control; Polarization Scrambling; PDL Measurement; PMD Compensation/Emulation; Fiber Sensor
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PDL-201 PDL/IL Multimeter
1260-1620 nm; Measurement Speed 30 ms; PDL Accuracy ±(0.01 + 5% of PDL) dB; PDL Dynamic Range 0-45 dB; IL Accuracy ±(0.01 + 5% of IL) dB; IL Dynamic Range 0-45 dB; Optical Power Range -40-+6 dBmUsing a patented maximum and minimum search method compliant with TIA/EIA-455-198, Lunas’ PDL/IL multimeter simultaneously measures the polarization dependent loss (PDL), insertion loss (IL) and optical power of devices in just 30 ms.Unlike PDL meters that use the polarization scrambling method with large measurement uncertainty, the PDL-201's max-min technique is useful for both low and high values of PDL. And unlike instruments that use a Mueller Matrix technique, the PDL-201 has a wide wavelength range from 1260 to 1620 nm without calibration.The PDL-201 PDL/IL multimeter comes with USB, Ethernet, GPIB and RS-232 interfaces for PC control and is ideal for fast, accurate characterization of the wavelength dependence of passive devices, especially DWDM and fiber sensor components, in manufacturing environments as well as in laboratories.The PDL-201 features fast measurement, large measurement dynamic range, a bright OLED display and an analog output port. The measurement speed of the instrument combined with the remote control interfaces allow it to work in conjunction with tunable lasers in automatic or semi-automatic test stations. Software to facilitate the integration is also available from AMS Technologies tech support.Key Features:Measurement Speed: 30 msWide Wavelength Range: 1260 to 1620 nmHigh Polarization Dependent Loss (PDL) Accuracy: ±(0.01 + 5% of PDL) dBPDL Dynamic Range: 0 to 45 dBInsertion Loss (IL) Accuracy: ±(0.01 + 5% of IL) dBIL Dynamic Range: 0 to 45 dBOptical Power Range: -40 to +6 dBmPower Meter FunctionOLED Display and Analog OutputDimensions: 356 x 216 x 89 mmApplications: PDL vs Wavelength Measurements; Characterization of DWDM Devices; Characterization of Fiber Sensor Component
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