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InGaAs Free-Space Amplified Photodetectors

  • Wavelength Ranges Between 800 - 2600 nm
  • Maximum Bandwidths up to 1.5 GHz 
  • Sensitivities Down to Femtowatt Powers
  • Fixed and Switchable Gain Versions


Switchable Gain
13 MHz Max Bandwidth


Application Idea

PDA Series Detector with Ø1" Lens Tube Attached to a 30 mm Cage System


Fixed Gain
380 MHz Max Bandwidth


Switchable Gain
1.5 GHz Max Bandwidth

Related Items

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Item # Wavelength
Bandwidth NEP
Fixed Gain
PDA015C(/M) 800 - 1700 nm DC - 380 MHz 20 pW/Hz1/2
PDA05CF2 800 - 1700 nm DC - 150 MHz 12.6 pW/Hz1/2
PDF10C(/M) 800 - 1700 nm DC - 25 Hz 7.5 x 10-3 pW/Hz1/2
PDA20C(/M) 800 - 1700 nm DC - 5 MHz 22 pW/Hz1/2
PDA10D2 900 - 2600 nm DC - 25 MHz 10.1 pW/Hz1/2
FPD510-FS-NIR 950 - 1650 nm DC - 250 MHz 3.2 pW/Hz1/2
FPD610-FS-NIR 950 - 1650 nm  DC - 600 MHz 6.6 pW/Hz1/2 
Switchable Gain
PDA20CS2a 800 - 1700 nm DC - 11 MHz 1.95 - 61 pW/Hz1/2
PDA10CS2a 900 - 1700 nm DC - 13 MHz 1.91 - 46 pW/Hz1/2
FPD310-FS-NIRb 950 - 1650 nm 1 - 1500 MHz 14.1 pW/Hz1/2
  • Switchable with 8 x 10 dB steps.
  • Switchable with 2 steps, 0 and 20 dB.


  • Wavelength Ranges within 800 to 2600 nm
  • Low-Noise Amplification with Fixed or Switchable Gain
  • Load Impedances 50 Ω and Higher for ≥3 kHz Bandwidth Versions
  • Free-Space Optical Coupling

We offer a selection of Indium Gallium Arsenide (InGaAs) Free-Space Amplified Photodetectors that are sensitive to light in the NIR wavelength range. Thorlabs' amplified photodetectors feature a built-in, low-noise transimpedance amplifier (TIA) which, for select detectors, is followed by a voltage amplifier. Menlo Systems' FPD series amplified photodetectors have a built-in radio frequency (RF) or transimpedance amplifier. We offer fixed-gain versions that possess a fixed maximum bandwidth and total transimpedance gain, as well as switchable-gain versions with two or eight gain settings.

Thorlabs' photodetectors are designed to meet a range of requirements, with offerings that include the 380 MHz PDA015C with an impulse response of 1 ns, the high-sensitivity PDF10C with a noise equivalent power (NEP) of 7.5 fW/Hz1/2, and the switchable-gain PDA20CS2 with eight switchable maximum gain (bandwidth) combinations from 1.51 kV/A (11 MHz) to 4.75 MV/A (3 kHz). The PDF10C with femtowatt sensitivity is a low-frequency device that should only be terminated into high impedance (Hi-Z) loads, while all other of our InGaAs PDA amplified photodetectors are capable of driving loads from 50 Ω to Hi- Z.

photo detector power supply
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The PDA05CF2 with the Included ±12 V Power Supply. Replacement power supplies are sold below.

Every PDA and PDF detector has internal SM05 (0.535"-40) threading and external SM1 (1.035"-40) threading. Except for some select detectors, each unit's housing features 8-32 tapped holes (M4 for -EC and /M models). The PDA05CF2, PDA10D2, PDA10CS2, and PDA20CS2 feature a new housing with universal mounting holes that accept both 8-32 and M4 threads. For more information about the location of these mounting points and mounting these units, please see the Housing Features and Mounting Options tabs.

Menlo Systems' FPD series photodetectors are easy-to-use InGaAs-PIN photodiode packages with an integrated high-gain, low-noise RF (FPD310-FS-NIR) or transimpedance (FPD510-FS-NIR and FPD610-FS-NIR) amplifier. The FPD310-FS-NIR is recommended, in particular, for applications like pulse shape and low-noise radio frequency extraction. This photodetector is optimized for high gain, high bandwidths, extremely short rise times, and high signal-to-noise ratio. It has a 0.5 ns rise time and a switchable gain between two settings, allowing for an optimal performance for the user's application. The FPD510-FS-NIR and FPD610-FS-NIR have a fixed gain and are optimized for highest signal-to-noise-ratio for detection of low level optical beat signals at frequencies up to 250 MHz and 600 MHz, respectively. The FPD510-FS-NIR has a rise time of 2 ns, while the FPD610-FS-NIR has a 1 ns rise time. The 3 dB bandwidth of these DC-coupled devices is 200 MHz for the FPD510-FS-NIR and 500 MHz for the FPD610-FS-NIR. The compact design of the FPD detectors allows for easy OEM integration. The housing of each Menlo detector features one M4 tapped hole for post mounting.

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Menlo Systems’ Detectors Include a Location-Specific ±12 V Power Supply

Power Supply
A ±12 V linear power supply is included with each amplified photodetector. A power supply that supports input voltages of 100, 120, and 230 VAC and is compatible with these detectors is also available separately below. Before connecting the power supply to the mains, ensure that the line voltage switch on the power supply module is set to the proper voltage range (either 115 or 230 VAC for all detectors except the PDA05CF2, PDA10D2, PDA10CS2, and PDA20CS2). The power supply included with the PDA05CF2, PDA10D2, PDA10CS2, and PDA20CS2 features a three-way switch and can be plugged into any 50 to 60 Hz, 100 V / 120 V / 230 V power outlet. The power supplies should always be powered up using the power switch on the power supply itself. Hot plugging the unit is not recommended.

Menlo's FPD510-FS-NIR, FPD610-FS-NIR and FPD310-FS-NIR include a low-noise power supply.

For detectors with a fiber coupled input, see InGaAs Fiber-Coupled Amplified Photodetectors.

Performance Specifications

Item # Wavelength Bandwidth Rise Time Peak Responsivity Noise Equivalent Power
Active Area Operating
Fixed Gain
PDA015C 800 - 1700 nm DC - 380 MHz 1.0 ns 0.95 A/W @ 1550 nm 20 pW/Hz1/2 0.018 mm(Ø150 µm) 10 to 40 °C
PDA05CF2b 800 - 1700 nm DC - 150 MHz 2.3 ns 1.04 A/W @ 1590 nm 12.6 pW/Hz1/2 0.2 mm2 (Ø0.5 mm) 10 to 50 °C
PDF10C 800 - 1700 nm DC - 25 Hz 19 ms 1.0 A/W @ 1550 nm 7.5 x 10-3 pW/Hz1/2 0.2 mm(Ø0.5 mm) 18 to 28 °C
PDA20C 800 - 1700 nm DC - 5 MHz 70 ns 1 A/W @ 1550 nm 22 pW/Hz1/2 3.14 mm(Ø2.0 mm) 10 to 50 °C
PDA10D2b 900 - 2600 nm DC - 25 MHz 15 ns 1.35 A/W @ 2300 nm 10.1 pW/Hz1/2 0.8 mm(Ø1.0 mm) 10 to 50 °C
FPD510-FS-NIR 950 - 1650 nm DC - 250 MHz 2 ns - 3.2 pW/Hz1/2 0.07 mm2 (Ø0.3 mm) 10 to 40 °C
FPD610-FS-NIR 950 - 1650 nm DC - 600 MHz 1 ns - 6.6 pW/Hz1/2 5 x 10-3 mm2 (Ø0.08 mm) 10 to 40 °C
Switchable Gain
PDA20CS2b 800 - 1700 nm DC - 11 MHzc N/Ad 1.04 A/W @ 1590 nm 1.95 - 61 pW/Hz1/2 3.14 mm(Ø2.0 mm) 10 to 40 °C
PDA10CS2b 900 - 1700 nm DC - 13 MHzc N/Ad 1.05 A/W @ 1550 nm 1.91 - 46 pW/Hz1/2 0.8 mm(Ø1.0 mm) 10 to 40 °C
FPD310-FS-NIR 950 - 1650 nm 1 - 1500 MHz 0.5 ns - 14.1 pW/Hz1/2 5 x 10-3 mm2 (Ø0.08 mm) 10 to 40 °C
  • NEP is specified at the peak responsivity wavelength. As NEP changes with the gain setting for the switchable-gain versions, an NEP range is given for these.
  • This detector has a 50 Ω terminator resistor that is in series with the amplifier output. This forms a voltage divider with any load impedance (e.g. 50 Ω load divides signal in half).
  • This is the maximum possible bandwidth for these amplified photodetectors. Bandwidth varies as a function of gain. For more information see the Switchable Gain table below.
  • Rise times depend on the chosen gain level and wavelength. As one increases the gain of a given optical amplifier, the bandwidth is reduced, and hence, the rise time increases. Please refer to the photodiode tutorial for information on calculating the rise time. Bandwidth specifications for each adjustable photodetector may be found in the table below.

Gain Specifications

Fixed Gain

Item # Gain w/ Hi-Z Load Gain w/ 50 Ω Load Offset (±) Output Voltage
w/ Hi-Z Load
Output Voltage
w/ 50 Ω Load
PDA015C 50 kV/A 25 kV/A 20 mV 0 to 10 Va 0 to 5 Va
PDA05CF2 10 kV/A 5 kV/A 20 mV 0 to 10 V 0 to 5 V
PDA20C 500 kV/A 175 kV/A 25 mV 0 to 10 V 0 to 3.5 V
PDF10Cb 1x108 kV/A - <150 mV 0 to 10 V -
PDA10D2 10 kV/A 5 kV/A 75 mV (375 mV Max) 0 to 10 V 0 to 5 V
FPD510-FS-NIR - 1.5 x 105 V/W - - 0 to 1 V
FPD610-FS-NIR - 2 x 106 V/W - - 0 to 1 V
  • Linear operating range is restricted due to slew rate limitations at maximum bandwidth. See the manual for more details.
  • Due to its 25 Hz cutoff frequency, operating the PDF10C(/M) with less than high impedance loading is not recommended.

Switchable Gain

Item # Gain Step Gain
w/ Hi-Z Loada
w/ 50 Ω Loada
Bandwidth Noise
NEPb Offset (±) Output Voltage
w/ Hi-Z Load
Output Voltage
w/ 50 Ω Load
PDA20CS2 0 1.51 kV/A 0.75 kV/A 11 MHz 286 µV 61 pW/Hz1/2 5 mV (10 mV Max) 0 to 10 V 0 to 5 V
10 4.75 kV/A 2.38 kV/A 1.5 MHz 201 µV 5.7 pW/Hz1/2 6 mV (10 mV Max)
20 15 kV/A 7.5 kV/A 1 MHz 236 µV 2.93 pW/Hz1/2 6 mV (10 mV Max)
30 47.5 kV/A 23.8 kV/A 260 kHz 234 µV 2.19 pW/Hz1/2 6 mV (10 mV Max)
40 151 kV/A 75 kV/A 90 kHz 240 µV 1.95 pW/Hz1/2 6 mV (10 mV Max)
50 475 kV/A 238 kV/A 28 kHz 260 µV 2.24 pW/Hz1/2 6 mV (10 mV Max)
60 1.5 MV/A 0.75 MV/A 9 kHz 300 µV 2.25 pW/Hz1/2 6 mV (10 mV Max)
70 4.75 MV/A 2.38 MV/A 3 kHz 396 µV 2.28 pW/Hz1/2 8 mV (12 mV Max)
PDA10CS2 0 1.51 kV/A 0.75 kV/A 13 MHz 264 µV 46 pW/Hz1/2 5 mV (10 mV Max) 0 to 10 V 0 to 5 V
10 4.75 kV/A 2.38 kV/A 1.7 MHz 190 µV 3.7 pW/Hz1/2 6 mV (10 mV Max)
20 15 kV/A 7.5 kV/A 1.1 MHz 208 µV 2.15 pW/Hz1/2 6 mV (10 mV Max)
30 47.5 kV/A 23.8 kV/A 300 kHz 212 µV 1.95 pW/Hz1/2 6 mV (10 mV Max)
40 151 kV/A 75 kV/A 90 kHz 220 µV 1.91 pW/Hz1/2 6 mV (10 mV Max)
50 475 kV/A 238 kV/A 28 kHz 235 µV 2.17 pW/Hz1/2 6 mV (10 mV Max)
60 1.5 MV/A 0.75 MV/A 9 kHz 270 µV 2.3 pW/Hz1/2 6 mV (10 mV Max)
70 4.75 MV/A 2.38 MV/A 3 kHz 361 µV 2.24 pW/Hz1/2 8 mV (12 mV Max)
FPD310-FS-NIR 0 - 2 x 104 Vpp/W 1 - 1500 MHz -c,d 14.1 pW/Hz1/2 N/A (AC Coupling) - 200 to 800 mV
20 - 2 x 103 Vpp/W - 20 to 80 mV
  • Gain figures can also be expressed in units of Ω.
  • The Noise Equivalent Power is specified at the peak wavelength.
  • The Dark State Noise Level is -100 dBm (up to 5 MHz).
  • The Dark State Noise Level is -130 dBm (5 to 1500 MHz).
PDA015 Top Connectors
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Top of the housing on our PDA and PDF detector housings. The Power In connector, Output BNC connector, and power indicator LED are located at the top of the housing. The PDA015C detector is shown.
Removable Internal SM1 Adapter
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The housings of Thorlabs' detectors feature internal SM05 and external SM1 threads. An SM1T1 SM1 Adapter with internal threads is included with each amplified photodetector, and an SM1RR Retaining Ring is included with the PDA015C, PDA10D2, PDA05CF2, PDA10CS2, and PDA20CS2.

Housing Features of the Amplified InGaAs Photodetectors

PDA and PDF Detectors
Thorlabs' Amplified Photodiode series feature a slim design and many common elements. Each housing features internal SM05 (0.535"-40) threading and external SM1 (1.035"-40) threading. All detectors include an SM1T1 internally SM1-threaded adapter. Most SM1-threaded fiber adapters are compatible with these detectors. The PDA015C, PDA10D2, PDA05CF2, PDA10CS2, and PDA20CS2 also each include an SM1RR retaining ring. A TRE(TRE/M) electrically isolated Ø1/2" post adapter is included with the PDF10A.

Threaded holes on the housings of the detectors allow the units to be mounted in a horizontal or vertical orientation, which gives the user the option to route the power and BNC cables from above or alongside the beam path. The PDA015C has two 8-32 threaded holes, while its metric counterpart has two M4 threaded holes. The PDA20C and PDF10C have three 8-32 threaded holes, while their metric counterparts have three M4 threaded holes. The PDA05CF2, PDA10D2, PDA10CS2, and PDA20CS2 have a new housing design that features the active area flush with the front of the housing, simplifying alignments within optomechanical systems. These detectors also have two universal threaded holes compatible with both 8-32 and M4 threads (please refer to the table below). As a convenience, the back panels of the PDA05CF2, PDA10D2, PDA015C, PDA10CS10, and PDA20CS2 are engraved with the responsivity curve of the InGaAs photodiodes. For more information on mounting these units, please see the Mounting Options tab.

FPD Detectors
The housing of each of Menlo Systems' FPD detectors feature one M4 tapped hole on the bottom for post mounting. The power supply connector and output SMA connector are located on the side of the housing.

Detectors Housing Drawing
(Click Icon for Details)
Mounting Taps SM Thread Compatibility Dimensions Output
PDA/PDF Fixed Gain
PDA05CF2, PDA10D2 Two Universal Taps for
8-32 and M4
Internal SM05 (0.535"-40)
External SM1 (1.035"-40)
1.96" x 0.89" x 2.79"
(49.8 mm x 22.5 mm x 70.9 mm)
PDA015C Two 8-32 Taps
(M4 for Metric Version)
1.89" x 0.83" x 2.76"
(48.0 mm x 21.1 mm x 70.2 mm)
PDF10C, PDA20C Three 8-32 Taps
(M4 for Metric Version)
1.70" x 0.83" x 2.57"
(43.2 mm x 21.1 mm x 65.3 mm)
FPD Fixed Gain
One M4 Tap N/A 2.36" x 0.79" x 1.97"
(60.0 mm x 20.0 mm x 50.0 mm)
PDA Switchable Gain 
PDA10CS2, PDA20CS2 Two Universal Taps for
8-32 and M4
Internal SM05 (0.535"-40)
External SM1 (1.035"-40)
2.07" x 0.89" x 2.79"
(52.5 mm x 22.5 mm x 70.9 mm)
FPD Switchable Gain
FPD310-FS-NIR One M4 Tap N/A 2.36" x 0.79" x 1.97"
(60.0 mm x 20.0 mm x 50.0 mm)

PDA and PDF Series Mounting Options

The PDA series of amplified photodetectors are compatible with our entire line of lens tubes, TR series posts, and cage mounting systems. Because of the wide range of mounting options, the best method for mounting the housing in a given optical setup is not always obvious. The pictures and text in this tab will discuss some of the common mounting solutions. As always, our technical support staff is available for individual consultation.

 amplified photodetector  amplified photodetector disassembled  amplified photodetector close up
Picture of a PDA series photodetector as it will look when unpackaged. Picture of a PDA series photodetector with the included SM1T1 and its retaining ring removed from the front of the housing. Thorlabs' DET series photodetectors feature the same mounting options. A close up picture of the front of the PDA05CF2 photodetector. The internal SM1 threading on the SM1T1 adapter and internal SM05 threading on the photodetector housing can be seen in this image.

TR Series Post (Ø1/2" Posts) System

The PDA housing can be mounted vertically or horizontally on a TR Series Post using the threaded holes for 8-32 (M4 on metric versions). Select PDA housings feature universally threaded holes for both 8-32 and M4 threads.

 mounted amplified photodetector vertical  mounted amplified photodetector horizontal
PDA series photodetector mounted vertically on a TR series post. In this configuration, the output and power cables (PDA series) are oriented vertically and away from the optic table, facilitating a neater optical setup. PDA series photodetector mounted horizontally on a TR series post. In this configuration, the on/off switch is conveniently oriented on the top of the detector.

Lens Tube System

Each PDA housing includes a detachable Ø1" Optic Mount (SM1T1) that allows for Ø1" (Ø25.4 mm) optical components, such as optical filters and lenses, to be mounted along the axis perpendicular to the center of the photosensitive region. The maximum thickness of an optic that can be mounted in the SM1T1 is 0.1" (2.8 mm). For thicker Ø1" (Ø25.4 mm) optics or for any thickness of Ø0.5" (Ø12.7 mm) optics, remove the SM1T1 from the front of the detector and place (must be purchased separately) an SM1 or SM05 series lens tube, respectively, on the front of the detector.

The SM1 and SM05 threadings on the PDA photodetector housing make it compatible with our SM lens tube system and accessories. Two particularly useful accessories include the SM-threaded irises and the SM-compatible IR and visible alignment tools. Also available are fiber optic adapters for use with connectorized fibers.

 Lens tube mounted amplified photodetector
PDA series photodetector mounted onto a Ø1" Slotted Lens Tube, which is housing a focusing optic. The lens tube is attached to a 30 mm cage system via a CP02 SM1-Threaded 30 mm Cage Plate. This arrangement allows easy access for optic adjustment and signal alignment.

Cage System

The simplest method for attaching the PDA photodetector housing to a cage plate is to remove the SM1T1 that is attached to the front of the PDA and use the external SM1 threads. A cage plate, such as the CP02 30 mm cage plate, can be directly attached to the SM1 threads. Then the retaining ring, included with the SM1T1, can be threaded using a spanner wrench into the CP02 to ensure the cage plate is tightened to the desired location and square with the photodetector housing. 

This method for attaching the PDA photodetector housing to a cage plate does not allow much freedom in determining the orientation of the photodetector; however, it has the benefit of not needing an adapter piece, and it allows the diode to be as close as possible to the cage plate, which can be important in setups where the light is divergent. As a side note, Thorlabs sells the SM05PD and SM1PD series of photodiodes that can be threaded into a cage plate so that the diode is flush with the front surface of the cage plate; however, the photodiode is unbiased.

For more freedom in choosing the orientation of the PDA photodetector housing when attaching it, an SM1T2 lens tube coupler can be purchased. In this configuration the SM1T1 is left on the detector and the SM1T2 is threaded into it. The exposed external SM1 threading is now deep enough to secure the detector to a CP02 cage plate in any orientation and lock it into place using one of the two locking rings on the ST1T2.

 photodetector with cage plate

photodetector with cage plate

photodetector with cage plate and spacer

This picture shows a PDA series photodetector attached to a CP02 cage plate after removing the SM1T1. The retaining ring from the SM1T1 was used to make the orientation of the detector square with the cage plate. These two pictures show a PDA series photodetector in a horizontal configuration. The top picture shows the detector directely coupled to a CP02 cage plate.
The bottom picture shows a PDA series photodetector attached to a CP02 cage plate using an SM1T2 adapter in addition to the SM1T1 that comes with the PDA series detector.

Although not pictured here, the PDA photodetector housing can be connected to a 16 mm cage system by purchasing an SM05T2. It can be used to connect the PDA photodetector housing to an SP02 cage plate.


The image below shows a Michelson Interferometer built entirely from parts available from Thorlabs. This application demonstrates the ease with which an optical system can be constructed using our lens tube, TR series post, and cage systems. 

 Michelson interferometer

The table below contains a part list for the Michelson Interferometer for use in the visible range. Follow the links to the pages for more information about the individual parts. 

Item # Quantity Description Item # Quantity Description
KC1 1 Mirror Mount CT1 1 1/2" Travel Translator
BB1-E02 2 Broadband Dielectric Laser Mirrors SM1D12 1 SM1 Threaded Lens Tube Iris
ER4 8 4" Cage Rods SM1L30C 1 SM1 3" Slotted Lens Tube
ER6 4 6" Cage Rods SM1V05 1 Ø1" Adjustable Length Lens Tube
CCM1-BS013 1 Cube-Mounted Beamsplitter CP08FP 1 30 mm Cage Plate for FiberPorts
BA2 1 Post Base (not shown in picture) PAF2-5A 1 FiberPort
TR2 1 Ø1/2" Post, 2" in Length P1-460B-FC-2 1 Single Mode Fiber Patch Cable
PH2 1 Ø1/2" Post Holder DET36A / PDA36A2 1 Biased / Amplified Photodiode Detector

PDA and PDF Series Detectors

BNC Female 0 - 10 V Output (Photodetector)

BNC Female

0 - 10 V Output

Male (Power Cables)

Pinout for PDA Power Cable

Female Power IN (Photodetector)

Pinout for PDA Power Connector

FPD Series Detectors

Signal Out- SMA Female (Photodetector)

BNC Female

For connection to a suitable monitoring device, e.g. oscilloscope or RF-spectrum-analyzer, with 50 Ω impedance.

Female (Power Cables)

Pinout for FPD Power Cable

Male Power IN (Photodetector)

Pinout for FPDPower Connector

Photodiode Tutorial

Theory of Operation

A junction photodiode is an intrinsic device that behaves similarly to an ordinary signal diode, but it generates a photocurrent when light is absorbed in the depleted region of the junction semiconductor. A photodiode is a fast, highly linear device that exhibits high quantum efficiency based upon the application and may be used in a variety of different applications.

It is necessary to be able to correctly determine the level of the output current to expect and the responsivity based upon the incident light. Depicted in Figure 1 is a junction photodiode model with basic discrete components to help visualize the main characteristics and gain a better understanding of the operation of Thorlabs' photodiodes.

Equation 1
Photodiode Circuit Diagram
Figure 1: Photodiode Model

Photodiode Terminology

The responsivity of a photodiode can be defined as a ratio of generated photocurrent (IPD) to the incident light power (P) at a given wavelength:

Equation 2

Modes of Operation (Photoconductive vs. Photovoltaic)
A photodiode can be operated in one of two modes: photoconductive (reverse bias) or photovoltaic (zero-bias). Mode selection depends upon the application's speed requirements and the amount of tolerable dark current (leakage current).

In photoconductive mode, an external reverse bias is applied, which is the basis for our DET series detectors. The current measured through the circuit indicates illumination of the device; the measured output current is linearly proportional to the input optical power. Applying a reverse bias increases the width of the depletion junction producing an increased responsivity with a decrease in junction capacitance and produces a very linear response. Operating under these conditions does tend to produce a larger dark current, but this can be limited based upon the photodiode material. (Note: Our DET detectors are reverse biased and cannot be operated under a forward bias.)

In photovoltaic mode the photodiode is zero biased. The flow of current out of the device is restricted and a voltage builds up. This mode of operation exploits the photovoltaic effect, which is the basis for solar cells. The amount of dark current is kept at a minimum when operating in photovoltaic mode.

Dark Current
Dark current is leakage current that flows when a bias voltage is applied to a photodiode. When operating in a photoconductive mode, there tends to be a higher dark current that varies directly with temperature. Dark current approximately doubles for every 10 °C increase in temperature, and shunt resistance tends to double for every 6 °C rise. Of course, applying a higher bias will decrease the junction capacitance but will increase the amount of dark current present.

The dark current present is also affected by the photodiode material and the size of the active area. Silicon devices generally produce low dark current compared to germanium devices which have high dark currents. The table below lists several photodiode materials and their relative dark currents, speeds, sensitivity, and costs.

MaterialDark CurrentSpeedSpectral RangeCost
Silicon (Si) Low High Speed Visible to NIR Low
Germanium (Ge) High Low Speed NIR Low
Gallium Phosphide (GaP) Low High Speed UV to Visible Moderate
Indium Gallium Arsenide (InGaAs) Low High Speed NIR Moderate
Indium Arsenide Antimonide (InAsSb) High Low Speed NIR to MIR High
Extended Range Indium Gallium Arsenide (InGaAs) High High Speed NIR High
Mercury Cadmium Telluride (MCT, HgCdTe) High Low Speed NIR to MIR High

Junction Capacitance
Junction capacitance (Cj) is an important property of a photodiode as this can have a profound impact on the photodiode's bandwidth and response. It should be noted that larger diode areas encompass a greater junction volume with increased charge capacity. In a reverse bias application, the depletion width of the junction is increased, thus effectively reducing the junction capacitance and increasing the response speed.

Bandwidth and Response
A load resistor will react with the photodetector junction capacitance to limit the bandwidth. For best frequency response, a 50 Ω terminator should be used in conjunction with a 50 Ω coaxial cable. The bandwidth (fBW) and the rise time response (tr) can be approximated using the junction capacitance (Cj) and the load resistance (RLOAD):

Equation 3

Noise Equivalent Power
The noise equivalent power (NEP) is the generated RMS signal voltage generated when the signal to noise ratio is equal to one. This is useful, as the NEP determines the ability of the detector to detect low level light. In general, the NEP increases with the active area of the detector and is given by the following equation:

Photoconductor NEP

Here, S/N is the Signal to Noise Ratio, Δf is the Noise Bandwidth, and Incident Energy has units of W/cm2. For more information on NEP, please see Thorlabs' Noise Equivalent Power White Paper.

Terminating Resistance
A load resistance is used to convert the generated photocurrent into a voltage (VOUT) for viewing on an oscilloscope:

Equation 4

Depending on the type of the photodiode, load resistance can affect the response speed. For maximum bandwidth, we recommend using a 50 Ω coaxial cable with a 50 Ω terminating resistor at the opposite end of the cable. This will minimize ringing by matching the cable with its characteristic impedance. If bandwidth is not important, you may increase the amount of voltage for a given light level by increasing RLOAD. In an unmatched termination, the length of the coaxial cable can have a profound impact on the response, so it is recommended to keep the cable as short as possible.

Shunt Resistance
Shunt resistance represents the resistance of the zero-biased photodiode junction. An ideal photodiode will have an infinite shunt resistance, but actual values may range from the order of ten Ω to thousands of MΩ and is dependent on the photodiode material. For example, and InGaAs detector has a shunt resistance on the order of 10 MΩ while a Ge detector is in the kΩ range. This can significantly impact the noise current on the photodiode. For most applications, however, the high resistance produces little effect and can be ignored.

Series Resistance
Series resistance is the resistance of the semiconductor material, and this low resistance can generally be ignored. The series resistance arises from the contacts and the wire bonds of the photodiode and is used to mainly determine the linearity of the photodiode under zero bias conditions.

Common Operating Circuits

Reverse Biased DET Circuit
Figure 2: Reverse-Biased Circuit (DET Series Detectors)

The DET series detectors are modeled with the circuit depicted above. The detector is reverse biased to produce a linear response to the applied input light. The amount of photocurrent generated is based upon the incident light and wavelength and can be viewed on an oscilloscope by attaching a load resistance on the output. The function of the RC filter is to filter any high-frequency noise from the input supply that may contribute to a noisy output.

Reverse Biased DET Circuit
Figure 3: Amplified Detector Circuit

One can also use a photodetector with an amplifier for the purpose of achieving high gain. The user can choose whether to operate in Photovoltaic of Photoconductive modes. There are a few benefits of choosing this active circuit:

  • Photovoltaic mode: The circuit is held at zero volts across the photodiode, since point A is held at the same potential as point B by the operational amplifier. This eliminates the possibility of dark current.
  • Photoconductive mode: The photodiode is reversed biased, thus improving the bandwidth while lowering the junction capacitance. The gain of the detector is dependent on the feedback element (Rf). The bandwidth of the detector can be calculated using the following:

Equation 5

where GBP is the amplifier gain bandwidth product and CD is the sum of the junction capacitance and amplifier capacitance.

Effects of Chopping Frequency

The photoconductor signal will remain constant up to the time constant response limit. Many detectors, including PbS, PbSe, HgCdTe (MCT), and InAsSb, have a typical 1/f noise spectrum (i.e., the noise decreases as chopping frequency increases), which has a profound impact on the time constant at lower frequencies.

The detector will exhibit lower responsivity at lower chopping frequencies. Frequency response and detectivity are maximized for

Photoconductor Chopper Equation

Posted Comments:
user  (posted 2018-07-01 21:53:00.79)
I hope the maximum optical input power that can be fed to the photodetector, e.g. PDA015C/M is the same as the damage threshold
YLohia  (posted 2018-07-03 10:05:05.0)
Please see the comment on the saturation/damage threshold spec for the PDA015C/M below.
user  (posted 2018-06-15 07:43:08.627)
What is the damage threshold of PDA015C/M photodetectors as it's saturation power is 350 microwatt
YLohia  (posted 2018-06-22 09:48:51.0)
A conservative value would be ~100 W/cm^2 average power density (but it can often be closer to 100 kW/cm^2) or about 100 mW total average power. We don't typically spec a damage threshold for photodiodes for two main reasons: the output voltage will saturate several orders of magnitude before damaging the surface, and only CW (average power) damage is a concern for most situations. For pulsed sources, the active area is less prone to pulsed damage mechanisms (e.g. dielectric breakdown/avalanche ionization). The primary damage mechanism is thermal burning at the PN junction. Both CW and pulsed damage will strongly depend on usage conditions so you should use these numbers as guideline only and not as an official spec.
michael.vandegraaaff  (posted 2018-03-13 11:55:30.23)
We have some older PDA10CS detectors in our lab. On the detector it is labeled 700-1800 nm. However the PDA10CS part currently available for purchase is only spec'd from 900-1700 nm. We have been using these for measuring 767nm light so this is relevant for us; do you have data down to 700nm or data for the older product. Can you explain the reason for the discrepancy?-Thank you
YLohia  (posted 2018-03-16 09:27:04.0)
Hello Michael, thank you for contacting Thorlabs. We tightened the specs of our PDA and DET detector lines in June 2015. The actual photodiode, as well as the circuitry of the detector, is still the same. Having the lower range as 900nm in the latest revision of the spec sheet does not necessarily mean that the unit will not be able to detect 767nm light. You may just have a low output signal from the unit, depending on the input optical power at this wavelength. I have reached out to you directly to discuss this further.
sergio.vilches  (posted 2017-08-08 15:39:48.433)
NEP value of PDA10D is shown as 0.35 pW/sqrtHz in one of the tables. Probably it is 35 pW/sqrtHz ?
tfrisch  (posted 2017-08-16 04:48:23.0)
Hello, thank you for bringing this to our attention. The NEP is 3.5x10^(-11)W/sqrt(Hz) as listed in the manual. This corresponds to 35pW/sqrt(Hz). I will reach out to you directly to clarify this as well.
user  (posted 2017-04-04 05:50:02.717)
What's the damage threshold for PDA10CS? Is it related to maximum current in the electric unit or determined by the maximum optical power density on the active area?
tfrisch  (posted 2017-04-26 01:49:55.0)
Hello, thank you for contacting Thorlabs. We do not list a damage threshold for these detectors as they will saturate before they are damaged. They are only intended for use in the region with linear response. Whether it is the gain electronics or photodiode which saturates first will depend on the gain setting. Please reach out to to discuss further with one of our Applications Engineers.
melanie  (posted 2017-01-26 07:37:36.047)
Please can you tell me the max operating temperature of this photodiode, and also the 10CS, thank you
tcampbell  (posted 2017-01-26 09:06:13.0)
Response from Tim at Thorlabs: thank you for your question. The maximum operating temperature of the PDA20CS(-EC) is 70 °C, and the maximum operating temperature of the PDA10CS(-EC) is 40 °C. These values are given in chapter 6 of the manuals. We will add this information to the web to make it easier to find.
grafen  (posted 2016-05-04 14:01:19.97)
Hello, we use this photodiode for two-photon absorption. Can you tell me of which material the front window is?
besembeson  (posted 2016-05-05 10:21:11.0)
Response from Bweh at Thorlabs USA: The window material for the PDA10D is borosilicate.
bernhard.reitinger  (posted 2015-06-02 17:40:49.587)
Dear ladies and gentleman. I think the PDF10CF is really a great product and the price compared to the biased version is what it makes even more great. Unfortunately in our application (interferometry) we would need an AC-coupled version. Would it be possible to add such a version in your portfolio? Best Regards Bernhard Reitinger
jlow  (posted 2015-06-05 09:39:33.0)
Response from Jeremy at Thorlabs: Thank you very much for the feedback. We will look into offering the AC-coupled version or offer it as a special. We will contact you directly about this.
Karthekab  (posted 2015-04-10 11:21:38.703)
The Adapter doesn't show the green light and I guess the current is not passing through it. Can you please help me with this issue
jlow  (posted 2015-04-14 09:57:47.0)
Response from Jeremy at Thorlabs: Please make sure the voltage selection switch is set to the correct setting. It could also be that the fuse is blown. I will contact you directly to troubleshoot more about this.
user  (posted 2015-02-02 16:36:14.25)
Are the bandwidths quoted single-sided or double-sided ? Thank you
jlow  (posted 2015-02-03 03:58:43.0)
Response from Jeremy at Thorlabs: These are measured from DC so it should be single-sided.
Paul.Wallace  (posted 2014-05-09 13:04:28.943)
We are using multiple numbers of this product (40) in an AWG. A power supply to power multiple units would be a great help. Controling mains leads to 40 power supplys is horid
jlow  (posted 2014-06-11 10:32:30.0)
Response from Jeremy at Thorlabs: Thank you for contacting Thorlabs. We will look into the possibility of providing this custom power supply for you and contact you directly.
marcelogodin  (posted 2012-09-06 09:45:57.0)
Hello I recently bought a PDA36A with the intention of measuring current due to light radioluminescence. I connected a photodiode PDA36A to an electrometer and I measured a noise about 150 nA. Is this normal? PDA36A noise is higher than DET36A?
jlow  (posted 2012-08-09 10:28:00.0)
Response from Jeremy at Thorlabs: Using the SolidWorks, the typical FOV for the different PDA is listed below. PDA100A: 53.13°, PDA36A: 70.19°, PDA10A: 122.92°, PDF10A: 127.81°, PDF8A: 150.64°.
ben.aernouts  (posted 2012-07-31 17:34:45.0)
Dear, Is it possible to provide me with the Field of View (FOV) of following Thorlabs Amplified Si detectors: PDA10A PDA8A PDF10A PDA36A PDA100A Many thanks and best regards, Ben Aernouts Department Biosystems, Division MeBioS KULeuven
tcohen  (posted 2012-05-15 09:49:00.0)
Response from Tim at Thorlabs: Thank you for your feedback! Our superseded products can be found by utilizing the search bar where the original supporting documentation is left intact. I am not sure that the part number you specified was our original part number. I will send you an overview of the old web presentation in order to determine the part number and provide supporting documentation for the correct product.
ryanbrock2011  (posted 2012-05-11 18:54:17.0)
Is the "New vs. Old" page mentioned in the older comments no longer on this site? I am looking for information on an old PDA-50 Si Amplified Photodetector
bdada  (posted 2012-01-25 15:15:00.0)
Response from Buki at Thorlabs: We specify at least +/- 12V, 125mA. However this is very conservative, especially if the PDA is driving a high impedance load. Most of the current usage is for driving the output. A 50Ohm load with the maximum output voltage (5V) will require a current of 100mA (5V/50Ohms). The amplifier itself uses approximately +/- 25mA from +/-12V supplies. The +12V supply needs to be able to supply an additional 100mA if it is driving a 50Ohm load. Please contact if you have any questions.
andrew.beeby  (posted 2012-01-25 10:37:37.0)
Could you advise what current the device draws at +/- 12V if we want to use our own power supply?
Thorlabs  (posted 2010-11-08 10:01:42.0)
Response from Javier at Thorlabs to Nathan: Thank you for your feedback. The PDA10CF and PDA10CS detectors have not been superseded. We are currently working with our web team to reactivate the shopping cart option so that you can order them through the web. You can also contact our sales department st or by phone at (973) 579 7227 to place an order.  (posted 2010-11-08 08:50:43.0)
Have you discontinued the PDA10CF & PDA10CS detectors? They are still included in the overview and specs tabs, but I cant find more detailed information or an option for purchasing? Or is there a replacement part (particularly for the variable gain version, but also for the fixed gain/high bandwidth version)? Thanks.
Thorlabs  (posted 2010-11-04 18:21:38.0)
Response from Javier at Thorlabs to imag: all of our photodiodes have a protective resin or coating. In order to remove dust, we would suggest gently blowing pressurized air onto the surface of the detector, from a ~6" distance. If further cleaning is needed, you can use ethyl alcohol an wipe off the dirt carefully. It is not recommended to use organic solvents, as they can degrade the quality of any resin coating or filters.
imag  (posted 2010-11-03 17:42:40.0)
I have a bunch of Thorlabs Si-photodiodes, biased and amplified. What is the procedure for the sensing area cleaning in the case if gets dirty or dusty ? Unlike conventional photodiodes, these detectors are not in some protective case with transparent window. Do they really have any protective layer on the Si ?
jens  (posted 2009-09-06 17:47:28.0)
A reply from Jens at Thorlabs: as for the maximum power we do not recommend to use more than 100mW over the detector area. You will find higher values in some publications, depending on wavelenght and exposure time and this value is more on the safe side. As to the inhomogenity the laser point located at different spots on the detector surface does indeed not produce the same conversion because of boundary conditions. These boundary conditions vary from diode to diode. To get a true estimate we can map out the area of the photo diode. I will contact you with additional data regarding the measurement. If possible the 2/3 rule (i.e. filling 2/3 of the detector aperture) should be followed.
flo6137  (posted 2009-08-31 12:38:28.0)
Hi, I am currently using a PDA100A but it seems that the sensitivity to the impinging laser light is not the same on all area of the photon detector. We have almost 10% of difference between different area. It might be possible that our PDA100A had been damaged by being exposed to a high power laser beam. But before buying a new one, could you please provide me some information about the accuracy of this photon detector (I mean the difference of sensitivity between the different cells of the detector) and about the maximum power that we can use without damaging the detector.
klee  (posted 2009-08-03 17:36:13.0)
A response from Ken at Thorlabs to asd: All the US and EC versions had different power supplies originally and the EC (220-240VAC) power supplies were more expensive. We did not change to the current new switchable power supply until about a year ago. We will be updating the prices shortly.
asd  (posted 2009-08-02 18:11:34.0)
How come the the PDA3A-EC is so much more expensive than the PDA36A? The other detectors dont show this skew in price and the PSUs are identical. Looks like a consumer annoying cock up.
klee  (posted 2009-07-09 10:00:13.0)
A response from Ken at Thorlabs to perry.gray: We do carry SM1 to C-mount adapters. SM1A10 has external SM1 Threads and internal C-Mount Threads while SM1A9 has internal SM1 Threads and external C-Mount Threads.
perry.gray  (posted 2009-07-08 21:35:37.0)
You guys need a C-mount adapter for your PDA series diodes so I can mount my existing c-mount tv camera lenses on my PDA diode housings
user  (posted 2009-06-09 13:16:54.0)
A response from Adam at Thorlabs to Letizia: Hi, We do not have data on the thermal drifts for these units. If you provide me with the temperature ranges you may be using the PDA25k at , I can check with our electronics engineers and see if we can provide more inforamtion. My email address is
user  (posted 2009-06-09 11:42:19.0)
Response from Adam at Thorlabs, Inc. Hi, I have spoken with our electronics engineers and there should be no need to distance the power supply from the photodiode. I am also checking with our engineers to see if we can provide any data about the shot noise. As soon as I have more information, I will send you an email. If you have further questions or concerns, feel free to contact me,
slamkadmi  (posted 2009-06-09 11:28:37.0)
Hello, I need to know if there is any requirement concerning the distance from the power supply to the photodiode. I have just seen a comment saying that "the power supply needs to be located about 5 meters away". Could you tell me more about that? I also need some data concerning the shot noise. Can the phase of the signal be deteriorated by the photodiode? In fact, we need to extract the phase from the output signal and we need a very high precision on the signal phase. If you do have any data, please let me know. Thanks in advance. Best regards
letizia.demaria  (posted 2009-04-15 03:47:47.0)
could you please specify the temperature coefficient (thermal drift) for PDA25k? thank you ldm
Laurie  (posted 2009-01-22 11:00:47.0)
Response from Laurie at Thorlabs to lee: Thank you for your interest in Thorlabs Products. A member of our technical support staff will be contacting you directly. We need a bit of clarification concerning your inquiry prior to discussing possible solutions.
lee  (posted 2009-01-20 04:13:57.0)
I plan to use PDA10A in an equipment, but the power supply needs to be located about 5 meters away. Ill be using a linear +/-12V power supply on DIN rail. I prefer to make the power supply cable in house, and so Id appreciate it if (1) Thorlabs sells the cable-side power connector (not the whole cable like PDA-C-72), or (2) gives relevant information such as connector manufacturer and part number.
Laurie  (posted 2008-12-10 13:37:22.0)
Response from Laurie at Thorlabs to jwerly: Thank you for your feedback concerning our PDA photodetectors. The transimpedance photocurrent amplifier assembly is built directly into the circuitry of the PDA detector, and thus, it is not possible to control the amplification externally or through some other method. Detectors like the PDA36A have switchable gain, but again, there is no way to adjust the amplification.
jwerly  (posted 2008-12-09 09:11:15.0)
Hello, I have a question about your PDA series. I would know how can we control the amplification. I mean, is it an automiticaly, a manualy or even a manualy by an electronic interface ? Regards, Julien Werly.
sal  (posted 2008-03-06 09:55:47.0)
Response from Sal at Thorlabs to jschumacher, ghegenbart, and acable: Numerous changes have been made to this page to address the postings below. The PDA8GS is a high-speed, fiber coupled detector that is now included with the other detectors in that family. The FPD310 high speed PIN photodiode module is accessible directly from its own window in the Biased and Amplified Detector Visual Navigation pane. Regarding this page, the pin description for the PDA Power Connector is in a diagram immediately next to the price and description of this component. All detectors are now grouped by material type (InGaAs and Ge are separated). The New vs. Old tab includes explicit references between current and superseded devices and the superseded devices are hot links that will lead to their documentation. This arrangement insures easy access to the old part information. The Overview tab has been completely reorganized to present the modules grouped both by high level feature (Switchable Gain, Wideband, etc.), application, and detector type (Si, InGaAs, etc.). The Specs tab also has been grouped by detector type. Gain figures are easy to read and units are expressed in both V/A and ohms since both units are generally used. Finally, under the Graphs tab a complete set of spectral responsivity data is included for each model number. We continually strive to assist our customers in finding the product that is best suited to their application. Thanks for your continued business.
technicalmarketing  (posted 2007-12-27 16:44:57.0)
In response to ghegenbarts comments, we have split the InGaAs and Ge subgroups as was done with the DETs page. We have also updated the product descriptions to be more uniform. Please note that acables comments are still being addressed by the technical marketing group. We thank you for your input, and hope that you find these changes to be helpful.
acable  (posted 2007-12-12 05:55:15.0)
Your "Specs" tab would be much easier to read if it was separated by detector type, when using the chart i am forced to piece together what Si detectors are available, it is great to have a large selection of products but as you expand the selection please realize that more thought should go into how you organize the presentation. I would also suggest a selection table right on the Overview tab, all the text is great for the first time visitor, added the table would just complete the overview picture faster for your more experienced customers. Another point that is confusing for me as a repeat customer is the non-uniformity of the product descriptions in the price boxes. Since i know the detector family fairly well and just need to pick out the right model it would be great to have all the relevant information right in your price table, there seems to be room. For me the order of importance is: What it Is: Handled with your Price Box Header Material: (which you handle well by separating the boxes by material) Bandwdith: (highest if switchable gain but provide foot note) Gain: (number if fixed and range if variable) Wavelength Range: (given by material in most cases) Ex: PDA10A, 150MHz BW, 5KOhm Gain, 200-1100nm Detector Also, my sense is that the transimpedence gain in units of Ohms is the standard way to specifiy an amplified detector, why the V/A, silly little thing but it caused me to have to pause.
acable  (posted 2007-12-12 05:27:23.0)
I came to this page specifically to cross reference an old PDA part number to a new one and was disapointed to find that this information was not provided on the "New vs Old Design" tab. Can you add a simple chart and then ensure the internal search feature can "see" the old part numbers. Does your search feature even have the ability to send a visitor to a specific tab.
ghegenbart  (posted 2007-11-26 08:14:26.0)
I suggest not to combine InGaAs and Ge in one product group but have them listed separately like it is done for the DETs.
jschumacher  (posted 2007-10-18 12:58:43.0)
please add pin description for PDA power connector

The following table lists Thorlabs' selection of photodiodes and photoconductive detectors. Item numbers in the same row contain the same detector element.

Photodetector Cross Reference
Wavelength Material Unmounted
150 - 550 nm GaP FGAP71 - SM05PD7A DET25K2 PDA25K2
200 - 1100 nm Si FDS010 - SM05PD2A
Si - - SM1PD2A - -
320 - 1000 nm Si - - - - PDA8A(/M)
320 - 1100 nm Si FD11A - SM05PD3A - PDF10A(/M)
Si - - - DET100A2 PDA100A2
340 - 1100 nm Si FDS10X10 - - - -
350 - 1100 nm Si FDS100
FDS100-CAL a
- SM05PD1A
Si FDS1010
FDS1010-CAL a
- -
400 - 1000 nm Si - - - - PDA015A(/M)
400 - 1100 nm Si FDS015 b - - - -
Si FDS025 b
FDS02 c
- - DET02AFC(/M)
400 - 1700 nm Si & InGaAs DSD2 - - - -
500 - 1700 nm InGaAs - - - DET10N2 -
750 - 1650 nm InGaAs - - - - PDA8GS
800 - 1700 nm InGaAs FGA015 - - - PDA015C(/M)
InGaAs FGA21
- SM05PD5A DET20C2 PDA20C(/M)
InGaAs FGA01 b
- - DET01CFC(/M) -
InGaAs FDGA05 b - - - PDA05CF2
InGaAs - - - DET08CFC(/M)
800 - 1800 nm Ge FDG03
- SM05PD6A DET30B2 PDA30B2
Ge FDG50 - - DET50B2 PDA50B2
Ge FDG05 - - - -
900 - 1700 nm InGaAs FGA10 - SM05PD4A DET10C2 PDA10CS2
900 - 2600 nm InGaAs FD05D - - DET05D2 -
FD10D - - DET10D2 PDA10D2
950 - 1650 nm InGaAs - - - - FPD310-FC-NIR
1.0 - 2.9 µm PbS - FDPS3X3 - - PDA30G(-EC)
1.0 - 5.8 µm InAsSb - - - - PDA10PT(-EC)
1.5 - 4.8 µm PbSe - FDPSE2X2 - - PDA20H(-EC)
2.0 - 5.4 µm HgCdTe (MCT) - - - - PDA10JT(-EC)
2.0 - 8.0 µm HgCdTe (MCT) VML8T0
VML8T4 d
- - - PDAVJ8
2.0 - 10.6 µm HgCdTe (MCT) VML10T0
VML10T4 d
- - - PDAVJ10
2.7 - 5.0 µm HgCdTe (MCT) VL5T0 - - - PDAVJ5
2.7 - 5.3 µm InAsSb - - - - PDA07P2
  • Calibrated Unmounted Photodiode
  • Unmounted TO-46 Can Photodiode
  • Unmounted TO-46 Can Photodiode with FC/PC Bulkhead
  • Photovoltaic Detector with Thermoelectric Cooler

InGaAs Amplified Photodetectors, Fixed Gain

Item #a Housing Featuresb Wavelength
Bandwidth Range Rise Time Gain NEP Typical Performance Graphs Active
Operating Temperature Range Power Supply Included
50 Ω Load
PDA015C 800 - 1700 nm DC - 380 MHz 1.0 ns 50 kV/A  25 kV/A 20 pW/Hz1/2 More Info 0.018 mm2
(Ø150 µm)
10 to 40 °C Yes
PDA05CF2 800 - 1700 nm DC - 150 MHz 2.3 ns 10 kV/A 5 kV/A 12.6 pW/Hz1/2 info 0.2 mm2
(Ø0.5 mm)d
10 to 50 °C Yes
PDF10C 800 - 1700 nm DC - 25 Hz 19 ms 1 x 108 kV/A - 7.5 x 10-3 pW/Hz1/2 More Info 0.2 mm2
(Ø0.5 mm)
18 to 28 °C Yes
PDA20C 800 - 1700 nm DC - 5 MHz 70 ns 500 kV/A 175 kV/A 22 pW/Hz1/2 More Info 3.14 mm2
(Ø2.0 mm)
10 to 50 °C Yes
PDA10D2 900 - 2600 nm DC - 25 MHz 15 ns 10 kV/A  5 kV/A 10.1 pW/Hz1/2 More Info 0.8 mm2
(Ø1.0 mm)d
10 to 50 °C Yes
FPD510-FS-NIR 950 - 1650 nm DC - 250 MHz 2 ns - 1.5 x 105 V/W 3.2 pW/Hz1/2 info 0.07 mm2 (Ø0.3 mm) 10 to 40 °C Yes
FPD610-FS-NIR 950 - 1650 nm DC - 600 MHz 1 ns - 2 x 106 V/W 6.6 pW/Hz1/2 info 5 x 10-3 mm2
(Ø0.08 mm)
10 to 40 °C Yes
  • Click on the links to view photos of the items.
  • Click the icons for details of the housing.
  • Click on the links to view an image of the detector element.
  • The detector active area surface is flush with the front of the housing.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Imperial Price Available
PDA015C Support Documentation
PDA015CInGaAs Fixed Gain Amplified Detector, 800 - 1700 nm, 380 MHz BW, 0.018 mm2, 8-32 Mounting Holes
Lead Time
PDF10C Support Documentation
PDF10CInGaAs fW Sensitivity Fixed Gain Amplified Detector, 800 - 1700 nm, 25 Hz, 0.2 mm2, 8-32 Mounting Holes
PDA20C Support Documentation
PDA20CCustomer Inspired! InGaAs Fixed Gain Amplified Detector, 800 - 1700 nm, 5 MHz BW, 3.14 mm2, 8-32 Mounting Holes
Lead Time
+1 Qty Docs Part Number - Universal Price Available
PDA05CF2 Support Documentation
PDA05CF2InGaAs Fixed Gain Amplified Detector, 800 - 1700 nm, 150 MHz BW, 0.2 mm2, Universal 8-32 / M4 Mounting Holes
PDA10D2 Support Documentation
PDA10D2InGaAs Fixed Gain Amplified Detector, 900 - 2600 nm, 25 MHz BW, 0.8 mm2, Universal 8-32 / M4 Mounting Holes
+1 Qty Docs Part Number - Metric Price Available
PDA015C/M Support Documentation
PDA015C/MInGaAs Fixed Gain Amplified Detector, 800 - 1700 nm, 380 MHz BW, 0.018 mm2, M4 Mounting Holes
PDF10C/M Support Documentation
PDF10C/MInGaAs fW Sensitivity Fixed Gain Amplified Detector, 800 - 1700 nm, 25 Hz, 0.2 mm2, M4 Mounting Holes
PDA20C/M Support Documentation
PDA20C/MCustomer Inspired! InGaAs Fixed Gain Amplified Detector, 800 - 1700 nm, 5 MHz BW, 3.14 mm2, M4 Mounting Holes
5-8 Days
FPD510-FS-NIR Support Documentation
FPD510-FS-NIRInGaAs Fixed Gain, High-Sensitivity PIN Amplified Detector, 950 - 1650 nm, DC - 250 MHz, 0.07 mm2, M4 Mounting Hole
FPD610-FS-NIR Support Documentation
FPD610-FS-NIRInGaAs Fixed Gain, High-Sensitivity PIN Amplified Detector, 950 - 1650 nm, DC - 600 MHz, 0.005 mm2, M4 Mounting Hole

InGaAs Amplified Photodetector, Switchable Gain

Item #a Housing Featuresb Wavelength
Bandwidth Range Gainc NEP Typical Performance Graphs ActiveAread Operating Temperature Range Power Supply Included
Hi-Z Load 50 Ω Load
PDA20CS2 800 - 1700 nm DC - 11 MHz 1.51 kV/A - 4.75 MV/A  0.75 kVA - 2.38 MV/A 1.95 -
61 pW/Hz1/2
More Info 3.14 mm2
(Ø2.0 mm)e
10 to 40 °C Yes
PDA10CS2 900 - 1700 nm DC - 13 MHz 1.51 kV/A - 4.75 MV/A 0.75 kVA - 2.38 MV/A 1.91 -
46 pW/Hz1/2
More Info 0.8 mm2
(Ø1.0 mm)e
10 to 40 °C Yes
FPD310-FS-NIR 950 - 1650 nm  1 MHz - 1.5 GHz - 2 x 103 - 2 x 104 Vpp/W 14.1 pW/Hz1/2 More Info 5 x 10-3 mm2
(Ø0.08 mm)
10 to 40 °C Yes
  • Click on the Item #'s to view an image of the detector.
  • Click the icons for details of the housing.
  • For complete Gain Specifications, see the Specs tab.
  • Click on the links to view an image of the detector element.
  • The detector active area surface is flush with the front of the housing.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
PDA20CS2 Support Documentation
PDA20CS2InGaAs Switchable Gain Amplified Detector, 800 - 1700 nm, 11 MHz BW, 3.14 mm2, Universal 8-32 / M4 Mounting Holes
PDA10CS2 Support Documentation
PDA10CS2InGaAs Switchable Gain Amplified Detector, 900 - 1700 nm, 13 MHz BW, 0.8 mm2, Universal 8-32 / M4 Mounting Holes
+1 Qty Docs Part Number - Metric Price Available
FPD310-FS-NIR Support Documentation
FPD310-FS-NIRInGaAs Switchable Gain, High Sensitivity PIN Amplified Detector, 950 - 1650 nm, 1 MHz - 1.5 GHz BW, 0.005 mm2, M4 Mounting Hole

PDA Power Supply Cable

Pinout for Cable

The PDA-C-72 power cord is offered for the PDA line of amplified photodetectors when using with a power supply other than the one included with the detector. The cord has tinned leads on one end and a PDA-compatible 3-pin connector on the other end. It can be used to power the PDA series of amplified photodetectors with any power supply that provides a DC voltage. The pin descriptions are shown to the right.

Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
PDA-C-72 Support Documentation
PDA-C-7272" PDA Power Supply Cable, 3-Pin Connector

±12 VDC Regulated Linear Power Supply

  • Replacement Power Supply for the PDA and PDF Amplified Photodetectors Sold Above
  • ±12 VDC Power Output
  • Current Limit Enabling Short Circuit and Overload Protection
  • On/Off Switch with LED Indicator
  • Switchable AC Input Voltage (100, 120, or 230 VAC)
  • 2 m (6.6 ft) Cable with LUMBERG RSMV3 Male Connector
  • UL and CE Compliant

The LDS12B ±12 VDC Regulated Linear Power Supply is intended as a replacement for the supply that comes with our PDA and PDF line of amplified photodetectors sold on this page. The cord has three pins: one for ground, one for +12 V, and one for -12 V (see diagram above). A region-specific power cord is shipped with the LDS12B power supply based on your location. This power supply can also be used with the PDB series of balanced photodetectorsPMM series of photomultiplier modules,APD series of avalanche photodetectors, and the FSAC autocorrelator for femtosecond lasers.

Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
LDS12B Support Documentation
LDS12B±12 VDC Regulated Linear Power Supply, 6 W, 100/120/230 VAC

Internally SM1-Threaded Fiber Adapters

These internally SM1-threaded (1.035"-40) adapters mate connectorized fiber to any of our externally SM1-threaded components, including our photodiode power sensors, our thermal power sensors, and our photodetectors. These adapters are compatible with the housing of the photodetectors on this page.

Item # S120-SMA S120-ST S120-SC S120-LC
Click Image to Enlarge S120-SMA S120-ST S120-SC S120-LC
Fiber Connector Typea SMA ST SC LC
Thread Internal SM1 (1.035"-40)
  • Other Connector Types Available upon Request
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
S120-SMA Support Documentation
S120-SMASMA Fiber Adapter Cap with Internal SM1 (1.035"-40) Thread
S120-ST Support Documentation
S120-STST/PC Fiber Adapter Cap with Internal SM1 (1.035"-40) Thread
S120-SC Support Documentation
S120-SCSC/PC Fiber Adapter Cap with Internal SM1 (1.035"-40) Thread
S120-LC Support Documentation
S120-LCLC/PC Fiber Adapter Cap with Internal SM1 (1.035"-40) Thread

Externally SM1-Threaded Fiber Adapters

Each disk has four dimples, two in the front surface and two in the back surface, that allow it to be tightened from either side with the SPW909 or SPW801 spanner wrench. The dimples do not go all the way through the disk so that the adapters can be used in light-tight applications when paired with SM1 lens tubes. Once the adapter is at the desired position, use an SM1RR retaining ring to secure it in place.

Adapter Image
(Click the Image to Enlarge)
Connector Type FC/PC FC/APC SMA ST/PC
Threading External SM1 (1.035"-40)
  • Please note that the SM1FCA has a mechanical angle of only 4°, even though the standard angle for these connectors is 8°. There is a 4° angle of deflection caused by the glass-air interface; when combined with the 4° mechanical angle, the output beam is aligned perpendicular to the adapter face.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
SM1FC Support Documentation
SM1FCFC/PC Fiber Adapter Plate with External SM1 (1.035"-40) Thread
SM1FCA Support Documentation
SM1FCAFC/APC Fiber Adapter Plate with External SM1 (1.035"-40) Thread
SM1SMA Support Documentation
SM1SMASMA Fiber Adapter Plate with External SM1 (1.035"-40) Thread
SM1ST Support Documentation
SM1STST/PC Fiber Adapter Plate with External SM1 (1.035"-40) Thread
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