R-QPD Four Quadrant PIN Optical Detection Module 400 - 1700nm Fast Response

Specifications

Diode Type: Indium Gallium Arsenide (InGaAs)
Wavelength Of Operation (Typical): 900 nm
Spectral Range: 400 – 1100 nm
Peak Responsivity (Rmax): 0.64 A/W
Peak Quantum Efficiency: Not Specified
Max Frequency Response: Other / Not specified
Active Area: 50 mm^2
Dark Current: Not Specified
Package Type: Custom Package
Built-In Amplifier: Not Specified
Product Type: Four quadrant PIN optical detection module
Models: R-QPD-B-20K, R-QPD-B-20M, R-QPD-A-20K, R-QPD-A-20M
Detector Type (R-QPD-B Series): Si PIN
Detector Type (R-QPD-A Series): InGaAs PIN
Light Input: Free space
Wavelength Range (R-QPD-B Series): 400–1100 nm
Wavelength Range (R-QPD-A Series): 800–1700 nm
Responsivity (R-QPD-B Series): 0.64 A/W @ 900 nm
Responsivity (R-QPD-A Series): 0.9 A/W @ 1550 nm
Photosensitive Surface Diameter (R-QPD-B Series): 7.98 mm
Photosensitive Surface Diameter (R-QPD-A Series): 3 mm
Unit Gap (R-QPD-B-20K): 42 µm
Unit Gap (R-QPD-B-20M / R-QPD-A-20K / R-QPD-A-20M): 45 µm
Bandwidth 3 DB (R-QPD-B-20K): >20 kHz
Bandwidth 3 DB (R-QPD-B-20M): >20 MHz
Bandwidth 3 DB (R-QPD-A-20K): >20 kHz
Bandwidth 3 DB (R-QPD-A-20M): >20 MHz
Conversion Gain (R-QPD-B-20K): 100 kV/W @ 900 nm
Conversion Gain (R-QPD-B-20M): 2.5 kV/W @ 900 nm
Conversion Gain (R-QPD-A-20K): 10 kV/W @ 1060 nm
Conversion Gain (R-QPD-A-20M): 10 kV/W @ 1060 nm
Rise Time (R-QPD-B-20K): 17 µs
Rise Time (R-QPD-B-20M): 35 ns
Rise Time (R-QPD-A-20K): 17 µs
Rise Time (R-QPD-A-20M): 18 ns
Saturated Optical Power (R-QPD-B-20K): 50 µW
Saturated Optical Power (R-QPD-B-20M): 2 mW
Saturated Optical Power (R-QPD-A-20K): 0.5 mW
Saturated Optical Power (R-QPD-A-20M): 0.5 mW
Coupling Method (R-QPD-B-20K / R-QPD-B-20M): DC coupling
Coupling Method (R-QPD-A-20K / R-QPD-A-20M): DC/AC coupling
Output Impedance: 50 Ω
Total Output Noise Voltage (R-QPD-B-20K): <1 mVpp
Total Output Noise Voltage (R-QPD-B-20M): <5 mVpp
Total Output Noise Voltage (R-QPD-A-20K): <2 mVpp
Total Output Noise Voltage (R-QPD-A-20M): <30 mVpp
Maximum Output Voltage: 5 V
Operating Voltage: DC 12 V @ <150 mA
Signal Output Port: J30J DB15 connector, adapter board to SMA
Module Size: 58 × 42 × 20 mm
Signal Module – Number Of Channels: 4
Signal Module – Maximum Input Signal Bandwidth: 10 kHz
Signal Module – Sampling Rate: max 4 kSPS
Signal Module – Data Update Frequency: typ. 10 Hz, max 4 kHz
Signal Module – Input Voltage Range: ±5 V
Signal Module – ADC Resolution: 16 bit
Signal Module – ADC Conversion Nonlinearity: ±0.2 LSB
Signal Module – Data Interface: USB 2.0 (default), optional RS232
Signal Module – Power Supply Voltage: +5 V (mini USB)
Signal Module – Power Consumption: <1 W
Signal Module – Operating Temperature: -10 ℃ to +50 ℃
Signal Module – Storage Temperature: -20 ℃ to +80 ℃

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Features

  • Wide Spectral Response (400–1700 nm) – Single module family covers both Si PIN (400–1100 nm) and InGaAs PIN (800–1700 nm), ideal for VIS, NIR, and telecom-band (850 nm, 1064 nm, 1310 nm, 1550 nm) laser applications.
  • Four-Quadrant PIN Detector for Precise Beam Positioning – Imported high-uniformity 4‑quadrant photodiodes enable accurate beam centering, pointing error detection, and real‑time position tracking in free-space optical paths.
  • High Responsivity for Low-Power Signals – Typical responsivity of 0.64 A/W @ 900 nm (Si) and 0.9 A/W @ 1550 nm (InGaAs) ensures efficient conversion of weak optical signals into measurable electrical outputs.
  • Fast Response & Wide Bandwidth Options – Models up to >20 MHz (3 dB) bandwidth with rise times down to ~18–35 ns, supporting high‑speed beam tracking, modulation analysis, and beat‑frequency detection for precision angle measurement.
  • Large and Small Active Area Options – Choose from 7.98 mm or 3 mm diameter photosensitive areas with small unit gaps (≈42–45 µm) to balance spot size tolerance, alignment ease, and position resolution.
  • Integrated Low‑Noise Transimpedance Amplifiers – Built‑in, matched 4‑channel low‑noise amplification reduces design complexity and external electronics, providing stable and repeatable performance across all quadrants.
  • High Conversion Gain – Typical conversion gains up to 10 kV/W @ 1060 nm (model‑dependent) allow detection of very low optical powers without needing additional high‑gain external stages.
  • Low Noise Output – Total output noise as low as <1 mVpp (low‑bandwidth models) and optimized noise performance on high‑speed versions enhances SNR for precision beam-centroid calculations and angle measurements.
  • DC and AC Coupling Options – Support for DC coupling (all models) and DC/AC coupling (selected A‑series) lets users optimize for static beam position measurements or high‑frequency signal extraction, including beat‑frequency and modulation detection.
  • Single 12 V Supply Operation – Simplified power requirement of DC 12 V @ <150 mA eliminates the need for multi‑rail supplies, streamlining integration into laboratory setups and OEM systems.
  • Four Independent Electrical Outputs – Each quadrant has an independent analog output for flexible processing (sum, difference, normalization) to compute XY position, pointing error, and tracking signals.
  • Standardized 50 Ω Output Impedance – 50 Ω matched outputs facilitate direct connection to oscilloscopes, spectrum analyzers, data‑acquisition cards, and RF front‑ends with minimal reflection and signal distortion.
  • Compact, Robust Mechanical Design – Small footprint of approximately 58 × 42 × 20 mm supports easy integration into optical benches, breadboards, alignment tools, and embedded photonic systems.
  • J30J DB15 Connector with SMA Adapter Board – Combined power and multi‑channel signal via DB15, plus included adapter to SMA, provides both clean lab connectivity and convenient integration into existing RF/DAQ infrastructures.
  • Optimized for Laser Collimation and Alignment – Designed for real‑time monitoring of beam centering and tilt, improving collimation setups, optical rail alignment, and long‑distance free‑space propagation systems.
  • Ideal for Laser Guidance & Target Tracking – High‑speed models (20 MHz) with four‑quadrant architecture enable dynamic tracking, target acquisition, and closed‑loop guidance control in defense, aerospace, and robotics.
  • Suited for Free‑Space Optical Communication – Free‑space input and wide wavelength coverage make the module a strong fit for FSO links, beam‑steering feedback, and alignment monitoring in optical communication terminals.
  • High‑Precision Angle Measurement Capability – Supports detection of beat‑frequency signals and sub‑microradian angle changes when used with appropriate optics and processing, making it suitable for interferometric and autocollimation systems.

Applications

Applications of the R-QPD Four Quadrant PIN Optical Detection Module

  • Laser beam collimation and alignment – Real‑time monitoring and optimization of laser beam parallelism and pointing; closed‑loop feedback for aligning free‑space optical paths in R&D labs, production lines, and optical test benches.
  • Beam position and centroid measurement – High‑accuracy X–Y position detection of laser spots for characterizing beam pointing stability, jitter, wander, and drift in precision optical systems.
  • Active beam steering and tracking systems – Feedback sensor for fast steering mirrors, galvanometers, and piezo stages where quadrant signals are used to stabilize or dynamically steer laser beams.
  • Free‑space laser communication (FSO) – Fine pointing, acquisition, and tracking (PAT) of communication beams, enabling stable alignment between ground–ground, ground–airborne, and inter‑satellite optical links over 400–1700 nm.
  • Laser guidance and homing – Position‑sensitive detection of guidance laser spots for missile seekers, UAV/UGV guidance heads, semi‑active laser homing, and terminal guidance systems.
  • High‑precision angle measurement – Use of differential quadrant signals and beat‑frequency detection (R‑QPD‑A‑20M) in autocollimators, angle encoders, and interferometric systems for micro‑rad and sub‑micro‑rad angle resolution.
  • Optical tracking and target acquisition – Target capture and tracking in laser tracking telescopes, optical trackers, lidar receivers, and surveillance systems that require fast quadrant‑based position feedback.
  • Laser pointing stabilization – Compensation of platform vibration and thermal drift in airborne, naval, and spaceborne optical payloads by feeding quadrant error signals into stabilization controllers.
  • Space optical communication terminals – Fine alignment in satellite and deep‑space optical terminals, star trackers, and inter‑satellite links where compact, low‑noise, high‑speed quadrant detection is essential.
  • Adaptive optics and wavefront control – Reference beam position sensing in adaptive optics benches for astronomy and high‑power laser systems, supporting wavefront correctors and deformable mirrors.
  • Laser scanning and imaging systems – Position feedback in scanning microscopes, confocal systems, OCT setups, and 2D/3D laser scanners to ensure accurate beam placement on samples or detectors.
  • Vibration, jitter, and beam wander analysis – Quantitative measurement of mechanical vibration and atmospheric‑induced beam wander by analyzing high‑speed quadrant signals up to 20 MHz bandwidth.
  • Optical laboratory automation and alignment tools – Integrated into auto‑alignment modules, motorized stages, and precision mounts for automated optimization of mirrors, lenses, and fiber couplers.
  • Laser cavity and resonator alignment – Monitoring intracavity beam position and symmetry for stable resonator alignment in solid‑state, fiber, and diode‑pumped laser systems.
  • Gaussian beam profiling and mode quality evaluation – Determination of beam centroid, symmetry, and temporal stability as part of laser M² and spatial mode quality characterization workflows.
  • Fiber coupling and alignment monitoring – Alignment of free‑space beams into single‑mode or multi‑mode fibers, with quadrant error signals used to maximize coupled power and maintain long‑term stability.
  • Lidar and range‑finding receivers – Spot position detection in lidar telescopes and range‑finders to improve pointing accuracy, boresighting, and overlap alignment between transmit and receive channels.
  • Optical metrology and precision positioning – Use in interferometers, displacement sensors, and coordinate measuring setups where beam position indicates mechanical movement at nanometer to micrometer scales.
  • Industrial laser processing and micromachining – Real‑time beam position feedback in cutting, drilling, marking, and welding systems to maintain alignment with workpieces and process features.
  • Beam overlap and coaxiality measurement – Verification and active control of coaxial alignment between multiple beams (e.g., pump/probe, visible/IR alignment lasers, or multi‑wavelength systems).
  • Scientific experiments in physics and photonics – General‑purpose quadrant detection in laboratories for experiments involving optical trapping, atomic/ion physics, cavity QED, and precision spectroscopy.