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Ge Transimpedance Amplified Photodetectors


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Ge Transimpedance Amplified Photodetectors

Features

  • Detection Range: 800 - 1800 nm
  • Low-Noise, Wide Band Amplifiers
  • Bandwidth from DC to 460 kHz
  • 0 to 10 V Output
  • Compatible with SM1 (1.035"-40) Series and Some SM05 (0.535"-40) Series Products
  • Linear Power Supply Included

The Ge-based Transimpedance Amplified Photodetectors feature a switchable gain setting housed in a compact, low-profile package. These detectors are sensitive to light in the NIR spectral region from 800 nm to 1800 nm. The slim profile housing enables use in light paths with space constraints. All connections and controls are located perpendicular to the light path, providing increased accessibility. Amplification is provided by low noise transimpedance or voltage amplifiers that are capable of driving 50 Ω loads. Signal output is via a BNC connector. Thorlabs offers a wide variety of BNC, BNC-to-SMA, and SMC cables, as well as a variety of BNC, SMA, and SMC adapters.

Each housing provides two 8-32 tapped mounting holes (M4 for - EC) centered on the detector surface for vertical or horizontal post mounting. The housings also feature external SM1 threading and internal SM05 threading that are compatible with most Thorlabs SM1 (1.035"-40)- and SM05 (0.535"-40)-threaded accessories. Additionally, an internally threaded SM1 coupler is included with each detector. This allows convenient mounting of SM1-compatible accessories, optics, and cage assembly accessories. The internal SM05 threading is only suitable for mating to an externally threaded SM05 lens tube (components such as fiber adapters cannot be threaded onto the SM05 threading). SM1-threaded fiber adapters may be used with any of these detectors. Externally SM1-threaded adapters should be mated to the included internally SM1-threaded adapter, while internally SM1-threaded adapters can be mated directly to the housing. A 120 VAC AC/DC linear power supply is included (230 VAC for - EC versions).

Due to limitations in the IC, the high-speed amplifier used in these devices may become unstable, exhibiting oscillations or negative output if the linear power supply voltage is applied when the module is on. The unit should always be powered up using the power switch on the power supply or the unit itself. Hot plugging the unit is not recommended. Additionally, inhomogeneities at the edges of the active area of the detector can generate unwanted capacitance and resistance effects that distort the time-domain response of the photodetector output. Thorlabs therefore recommends that the incident light on the photodetector be well centered on the active area. The SM1 (1.035"-40) threading on the housing is ideally suited for mounting a Ø1" focusing lens or pinhole in front of the detector element.

Performance Specifications

SensorItem #Active
Area
WavelengthPeak
Response
BandwidthNEP Rangea
(W/Hz½)
Rise Timeb
Ge (NIR)PDA50B19.6 mm2
(Ø5.0 mm)
800 - 1800 nm0.85 A/W
@ 1550 nm
DC - 460 kHz4.63 x 10-12 -
1.75 x 10-11
760 ns
PDA30B7.0 mm2
(Ø3.0 mm)
800 - 1800 nm0.88 A/W
@ 1550 nm
DC - 460 kHz3.38 x 10-12 -
4.44 x 10-11
760 ns

a A NEP range is given for the switch gain detectors, a max NEP is given for the fixed gain detectors.
b Please note that rise times depend on the chosen gain level. As one increases the gain of a given optical amplifier, the bandwidth is reduced, and hence, the rise time increases.

Gain Specifications 

Switchable Gain
Photodetector
Gain Step
(dB)
Gain w/ Hi-Z LoadGain w/ 50 Ω LoadOutput Voltage
w/ Hi-Z Load
Output Voltage
w/ 50 Ω Load
PDA50B and PDA30B01.5 kV/A0.75 kV/A0 - 10 V
0 - 5 V
104.75 kV/A2.38 kV/A
2015 kV/A7.5 kV/A
3047.5 kV/A23.8 kV/A
40150 kV/A75 kV/A
50475 kV/A238 kV/A
601.5 MV/A750 kV/A
704.75 MV/A2.38 MV/A

Note: Gain figures can also be expressed in units of Ω.

PDA Series Compact Design
PDA Series Design, scale in inches [mm ].

Compact PDA Series Design

Thorlabs' Amplified Photodiode series features a slim design, which allows the detector access to the light path even between closely spaced optical elements.

The power supply input and the BNC output are located on the same outer edge of the package, further reducing the device thickness and allowing easier integration into tight optic arrangements. The Ge PDA detectors can fit into spaces as thin as 0.83" (21.1 mm) when the SM1 coupler is removed. With the SM1 coupler attached, the smallest width the detector can fit into is 1.03" (26.2 mm).

Additionally, the detectors have two tapped mounting holes perpendicular to each other so that the unit can be mounted in a horizontal or vertical orientation. This dual mounting feature offsets the fact that the cables protrude out the side of the package, thus requiring more free space above or alongside your beam path.

The switchable gain detectors feature an eight-position rotary gain switch (pictured below right) mounted on an outside edge perpendicular to the power supply and BNC output connections. The location of the gain switch allows for easy adjustments while the detector is mounted.

PDA detector Bottom and Side view

GE PDA Amplified Photodetectors Mounting Options

The GE PDA 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 photodetectoramplified photodetector disassembledamplified photodetector close up
Picture of a PDA series photodetector as it will look when unpackaged.Picture of a DET series photodetector with the included SM1T1 and its retaining ring removed from the front of the housing. Thorlabs' PDA series photodetectors feature the same mounting options.A close up picture of the front of the PDA10A 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 8-32 (M4) threaded holes.

mounted amplified photodetector verticalmounted amplified photodetector horizontal
DET 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
DET series photodetector mounted onto an SM1L30C 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 when it is shipped. This will expose external SM1 threading that is deep enough to thread the photodetector directly to a CP02 30 mm cage plate. When the CP02 cage plate is tightened down onto the PDA photodetector housing, the cage plate will not necessarily be square with the detector. To fix this, back off the cage plate until it is square with the photodetector and then use the retaining ring included with the SM1T1 to lock the PDA photodetector into the desired location.

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, a 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 DET 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 DET series photodetector in a horizontal configuration. The top picture shows the detector directely coupled to a CP02 cage plate.
The bottom picture shows a DET 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.

Application

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. A PDA series photodetector is interchangable with the DET series photodetector shown in the picture.

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 #QuantityDescriptionItem #QuantityDescription
KC11Mirror MountCT111/2" Travel Translator
BB1-E022Broadband Dielectric Laser MirrorsSM1D121SM1 Threaded Lens Tube Iris
ER484" Cage RodsSM1L30C1SM1 3" Slotted Lens Tube
ER646" Cage RodsSM1V051Ø1" Adjustable Length Lens Tube
CM1-BS0131Cube-Mounted BeamsplitterCP08FP130 mm Cage Plate for FiberPorts
BA21Post Base (not shown in picture)PAF-X-5-A1FiberPort
TR21Ø1/2" Post, 2" in LengthP1-460A-FC-21Single Mode Fiber Patch Cable
PH21Ø1/2" Post HolderDET36A / PDA36A1Biased / Amplified Photodiode Detector

BNC Female Output

BNC Female

0 - 10 V Output

PDA-C-72 Power Supply

Pinout for PDA Power Connector

The following table lists the amplified detectors found on this page, along with the unmounted and mounted photodiodes and biased detectors which use the same internal photodiode.

 Photodiode Cross Reference
WavelengthMaterialUnmounted PhotodiodeUnmounted PhotoconductorMounted PhotodiodeBiased DetectorAmplified Detector
150 - 550 nmGaPFGAP71-SM05PD7ADET25KPDA25K
200 - 1100 nmSiFDS010-SM05PD2A
SM05PD2B
DET10APDA10A
200 - 1100 nmSi--SM1PD2A--
320 - 1100 nmSi----PDA8A
320 - 1100 nmSi----PDF10A
340 - 1100 nmSiFDS10X10---PDA100A
350 - 1100 nmSiFDS100
FDS100-CAL*
-SM05PD1A
SM05PD1B
DET36APDA36A
400 - 1100 nmSiFDS02--DET02AFC-
400 - 1100 nmSiFDS1010
FDS1010-CAL*
-SM1PD1A
SM1PD1B
DET100APDA100A
400 - 1700 nmSi & InGaAsDSD2----
500 - 1700 nmInGaAs---DET10N-
700 - 1800 nmInGaAs----PDA10CF
800 - 1700 nmInGaAs----PDF10C
800 - 1800 nmInGaAsFGA10-SM05PD4ADET10CPDA10CS
800 - 1800 nmInGaAsFGA21
FGA21-CAL*
-SM05PD5ADET20CPDA20C
PDA20CS
800 - 1800 nmGeFDG03
FDG03-CAL*
-SM05PD6ADET30BPDA30B
800 - 1800 nmGeFDG05
FDG05-CAL*
--DET50BPDA50B
800 - 1800 nmGeFDG1010-SM1PD5A--
900 - 1700 nmInGaAsFGA01FC--DET01CFC-
1.0 - 2.9 µmPbS-FGPS3X3--PDA30G
1.2 - 2.6 µmInGaAsFGA20--DET10DPDA10D
1.5 - 4.8 µmPbSe-FGPSE2X2--PDA20H

* Calibrated Unmounted Photodiodes

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Posted Comments:
Poster: jjurado
Posted Date: 2011-02-16 09:24:00.0
Response from Javier at Thorlabs to daniel.grodensky: Thank you very much for contacting us with your request. The dark state noise level is specified to be below -80dBm, measured with "span 5MHz, 3kHz resolution" which refers to the settings of the RF analyzer when measuring the frequency spectrum of the output of the detector under dark conditions (i.e. optical input blocked from light). In this setting, you will find the noise floor to be below -80dBm, which corresponds to 22.5µV RMS in a 50-Ohm system. Taking into account the 3kHz span, this corresponds to a noise level of 0.41µV/sqrt(Hz), or 1.6pW/sqrt(Hz) at the input. We specify the -80dBm as the maximum noise floor over the whole frequency range; usually the APD210 performs much better than that, down to -92dBm, which actually corresponds to the specified calculated NEP of 0.4pW/sqrt(Hz).
Poster: daniel.grodensky
Posted Date: 2011-02-08 10:04:07.0
I am interested in APD210, but have a question: What are the full conditions for your dark state noise level (-80dBm = 10pW), or more exactly whats the specified bandwidth? For better of my understanding, having NEP of 0.4pW/sqrHz means that at 1GHz bandwidth the NEP is 12.6nW or -49dBm, the number that 3 orders higher than dark state noise level. Thanks a lot in advance
Poster: Javier
Posted Date: 2010-06-16 11:21:10.0
Response from Javier at Thorlabs to last poster: the gain adjustment of the APD210 and APD310 detectors controls the APD bias voltage by means of a digital potentiometer that is essentially a resistor network with 100 discrete steps. So, for the APD210, for example, which has a maximum gain of 2.5x10^5 V/W (at 1 GHz, 800 nm), each gain step consists of ~2500 V/W.
Poster:
Posted Date: 2010-06-16 10:26:55.0
Hi, What is the minimum gain for APD210 and APD310, also Gain [V/W] at each step?
Poster: apalmentieri
Posted Date: 2009-12-28 14:41:00.0
A response from Adam at Thorlabs: The APD210 and APD310 have frequency ranges of 1-1600Mhz(APD210) and 1-1800MHz(APD310) respectively. Please note that the 1000MHz listed in the item description refers to the 3dB bandwidth, which is 5-1000MHz for both the APD310 and APD210.
Poster:
Posted Date: 2009-12-28 04:18:45.0
Item description says 1000MHz, I dont think that is correct
Poster: yue77
Posted Date: 2009-09-25 05:30:07.0
Dear team. I am interested in APD210, but have two questions: 1. What are the full conditions for your dark state noise level? 2. How did you calculate NEP, could you provide the necessary parameters? Thanks a lot in advance.
Poster: klee
Posted Date: 2009-07-10 21:16:12.0
A response from Ken at Thorlabs to Mattias.Heinrich: Yes, you can use a fiber with these detectors and SM05SMA is the correct adapter if you your fiber is terminated with SMA connector. We also have SM05FC and SM05ST for FC/PC and ST connectors.
Poster: Mattias.Heinrich
Posted Date: 2009-07-10 11:19:23.0
Hi. Is it possible to couple the detector to a fiber using e.g. the SM05SMA fiber adapter or which other positioning/alignment would you recommend. Thanks in advance.
Poster: Tyler
Posted Date: 2008-07-23 16:21:35.0
A response from Tyler at Thorlabs to ennui3: Quantum efficiency is defined as the ratio of the number of electrons excited into the conduction band divided by the number of photons absorbed. The QE varies from 0 to an ideal maximum of 1 in standard photodiodes. Since the APD210 is an avalanche photodiode a single photon can potentially generate many conduction electrons and as a result I do not think that the QE is the best measure to be used with this device. With a standard photodiode you can calculate the QE from the responsivity (A/W). QE=(Rhc)/(le) Where R is the responsivity in (A/W), h is Planck’s constant, c is the speed of light, l is the wavelength of the light, and e is the magnitude of the charge of an electron. Thank you for your interest in the APD210 and if you have further questions please post them or contact one of our application engineers.
Poster: ennui3
Posted Date: 2008-07-18 03:00:27.0
dear. I want to know the quantumn efficiency of this product. especially. I want to know Q.E. of wave length at 650nm~750nm. Does the photo sensitivity mean the Q.E.? thank you for reading this letter.
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Amplified Ge Photodetectors: NIR Wavelengths
Item #PDA50BPDA30B
Click on the Image to Enlarge

PDA50B

PDA30B

Element Photo

Ge

Ge

Wavelength Range

800 - 1800 nm

800 - 1800 nm

Responsivity Curve

More Info

More Info

Detector Size Ø5.0 mm Ø3.0 mm
Gain 8 x 10 dB Steps 8 x 10 dB Steps
Bandwidth Range DC - 460 kHz DC - 460 kHz
NEP (W/Hz1/2) 4.63x10-12 - 1.75x10-11 1.95x10-12 - 4.44x10-11
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal/Imperial Price Available / Ships
PDA50B Support Documentation PDA50B Ge Switchable Gain Detector, 800-1800 nm, 460 kHz BW, 19.6 mm2, 120 VAC $489.00
Today
PDA30B Support Documentation PDA30B Ge Switchable Gain Detector, 800-1800 nm, 460 kHz BW, 7.0 mm2, 120 VAC $450.00
Today
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PDA50B-EC Support Documentation PDA50B-EC Ge Switchable Gain Detector, 800-1800 nm, 460 kHz BW, 19.6 mm2, 230 VAC $489.00
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PDA30B-EC Support Documentation PDA30B-EC Ge Switchable Gain Detector, 800-1800 nm, 460 kHz BW, 7.0 mm2, 230 VAC $450.00
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PDA Power Supply Cable
Pinout for Cable

The PDA-C-72 is a power cord for the PDA line of amplified photodetectors. 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 suitable linear power supply. PDA pin descriptions are shown here.

Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal/Imperial Price Available / Ships
PDA-C-72 Support Documentation PDA-C-72 72" PDA Power Supply Cable, 3-Pin Connector $18.50
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Internally Threaded SM1 Fiber Adapters

Compatible with Devices with External SM1 Threads:

  • S120 and S140C Photodiode Power Sensors
  • S300 Series Thermal Power Sensors (except S350C & S370C)
  • APD110 and PDF10 Series Photoreceivers
Item #S120-FCS120-SMAS120-STS120-SCS120-LC
Adapter Image
(Click the Image
to Enlarge)
S120-FC S120-SMA S120-ST S120-SC S120-LC
Connector Type* FC/PC SMA ST SC LC
Thread Internal SM1 Internal SM1 Internal SM1 Internal SM1 Internal SM1

*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/Imperial Price Available / Ships
S120-FC Support Documentation S120-FC FC/PC Fiber Adapter Cap with Internal SM1 (1.035"-40) Thread $38.00
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S120-SMA Support Documentation S120-SMA SMA Fiber Adapter Cap with Internal SM1 (1.035"-40) Thread $38.00
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S120-ST Support Documentation S120-ST ST Fiber Adapter Cap with Internal SM1 (1.035"-40) Thread $38.00
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S120-SC Support Documentation S120-SC SC Fiber Adapter Cap with Internal SM1 (1.035"-40) Thread $48.00
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S120-LC Support Documentation S120-LC LC Fiber Adapter Cap with Internal SM1 (1.035"-40) Thread $48.00
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