Quadrant-cell photoreceivers are ideal when you need to measure deviations in the position or pointing of your laser beam, such as that required in beam-stabilization systems.
Ideal for beam-stabilization applications
Analog output
Convenient adjustable gain settings and switchable output normalization
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quadrant-cell-photoreceivers - Drawings
Additional drawings are not available for this product.
Specifications
Sensor Size
2901: 3 x 3 mm 2903: Ø3 mm
Transimpedance Gain
2x102 to 2x106 V/A
Optical Input
Free Space
Analog Output
X, Y, SUM
Analog Output Voltage Range
X & Y: ±2.5 V SUM: 0 to +2.5 V
Connector, Analog Output
Male BNC
Analog Output Impediance
1 kΩ
Power Requirements
±15 V, 50 mA power supply or 9V Battery
Bandwidth (-3 dB)
100 kHz (30 Hz for SUM)
Detector Material
2901: Silicon 2903: InGaAs
Rise Time
4 µs
Features
Silicon or InGaAs Sensors
Model 2901 offers silicon sensors which are responsive in the 190-1050 nm wavelength range. Model 2903 uses InGaAs sensors for 900-1700 nm responsivity.
Highly Sensitive Beam Position Measurement
Quadrant-cell photoreceivers consist of four individual yet identical photocells positioned very close to each other (100-µm gaps). To increase the sensitivity of these photoreceivers, each of the cells’ photocurrents is sent to its own individual amplifier before being processed with the other photocell signals to generate top-minus-bottom difference (vertical error) and right-minus-left difference (horizontal error) signals. A sum-of-all-quadrants signal is also provided for normalization purposes.
Battery Operated or External DC Supply
The 2901 and 2903 quadrant-cell photo-receivers can run off batteries or your own DC power supply. To ensure low noise operation, we strongly recommend our Model 0901
Bandpass and neutral-density filters for filtering out unwanted light or attenuating the beam can be attached to the front of these photoreceivers with the aid of Newport's 1280
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