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All Fiber Doppler Velocity Interferometer Systems
a new kind of VISAR

Series G PDM
Series G Unamplified
Single Photodetectors
for light levels
of 0.1 mW and higher


Series F PDM
Series F Amplified Single Photodetectors
for light levels down to nanowatts


Series F Differential PDM
Series J Amplified
 Differential Photodetectors

like Series F single detectors,
but only the difference is amplified



Power Supply

recommended
for DC coupled PDMs
and all Differentials


International Orders
International Order Policies

 

 

Martin, Froeschner & Associates

Series F Fast Compact Photodetector Modules

Now with sensitivities to over one million V/W and speeds to 10 GHz.

Faster, more compact, and cheaper than our Award Winning Series 99 Photodetectors.

A new line of inexpensive and compact fiber-coupled photodiode modules simplify capturing fast transient light signals for analysis. These devices are intended to approximate as closely as possible, a length of fiber optic cable that can be connected directly onto the input jacks of your oscilloscope or other electronic data acquisition device. Conversion of the optical signal to electronic current and voltage occurs at the last possible moment, within a mm or so of the input jacks of your scope. Co-ax cable and the problems of reflections, termination loads, phase distortion and so forth are totally eliminated. The devices are extremely compact and rugged, taking up about as much room as a typical BNC terminator

M,F&A's continuously improved Amplified Differential Photodetector Modules allow detection of the difference between two optical signals at bandwidths up to 10 GHz and overall optical conversion gains of up to one million volts/watt or more. They are perfectly suited for detection of the phase difference between two otherwise identical signals such as in range finding or in phase encoded communication protocols. Other applications include the detection of small optical modulations on a high power or unpredictably variable background.

In these modules the signal differencing is done at the optical input stage, before amplification, where the two photodiodes are arranged in a “totem-pole” configuration, as in TTL logic circuits.   The amplifier input is taken from the node between the two photodiodes, so the amplifier sees only the difference between the two photodiode currents. 

These modules are available with the same broad range of photodiode and amplifier choices as our Series F Photodetector Modules.

Dimensions: 0.65" (16mm) diameter by 1" to 1.75" (25 to 40 mm), excluding connectors and optical fiber
Construction: machined from solid 6061-T6 Aluminum, internal components potted in resin
Power: shielded four-conductor cable to External Power Supply

 

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Optical Fiber and Connector

We will build your modules with whatever optical fiber, cable and connectors you specify. We normally stock single-mode 9/125 µm and both 50/125 µm and 62.5/125 µm multimode fiber with 0.9mm polymer buffer and 3mm Kevlar jacket. Other types such as 100/140 µm are available. The fiber to photodiode connection is angle polished for low (-45dB) back reflection.

The input end of the optical fiber will be fitted with whatever type of optical fiber connector you desire. The range of normal options include: none, i.e. a bare fiber pigtail, 2 mm ceramic ferrule only, NTT-FC, SC, ST and SMA. The fiber end itself will be polished to any of the standard specifications: flat, PC, SPC or APC (8o). If you need something else, just specify so on the Order Form.

 

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Optional Light Collecting Optics

If the signal you want to analyze is in the form of a beam in free-space we can provide light collecting optics instead of or in addition to the optical fiber connectors described above. A 6 mm diameter fixed focus aspheric lens assembly is available. We also offer a micro-alignable fixture with 18 mm aperture focusable achromatic lens. Precision fine thread adjustments allow you to maximize the coupling of the incoming beam into the fiber. The unit is also directly compatible with "micro-rail" optical component systems made by Newport, Melles-Griot, ThorLabs and others and is "C" threaded for compatibility with Edmund Scientific's modular component line. Finally, large aperture catadioptric systems for collecting light from weak, distended or distant sources can be provided. Details available upon inquiry.

 

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Photodiode Selection

graph of Responsivity vs Wavelength of PhotodiodesThe two major considerations in selecting the photodiode for your application are spectral response and speed. Photodiodes based on different semiconductor materials have, in general, different ranges of light wavelength to which they are most sensitive.

For example, Silicon based diodes are most sensitive in the 400nm (nearly UV) to 1000nm (near IR) spectral range and cover the visible well. InGaAs is relatively insensitive to visible light but responds well to the IR used in information systems.

The intrinsic speed of the photodiode is also determined by the semiconductor material. The higher electron mobility in InGaAs allows response times which are simply not attainable with Si. Our latest GaAs model offers unprecedented speed in the visible range. Other factors which might be important to your needs, such as Dark Current and Capacitance are also listed in the table on Photodiode Specifications.

The photodiode in all our modules is reverse biased to minimize intrinsic capacitance for maximally fast response.

 

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Photodiode Specifications

Specifications are listed for the usual photodiodes. Others are available, call or write for details.

 

GaAs

InGaAs-1

InGaAs-2

InGaAs-3

Spectral Range

450-870 nm

850-1700 nm

850-1700 nm

950-1650 nm

Responsivity

0.60 A/W at 850

0.9 A/W@1550

0.9 A/W@1550

0.9 A/W@1550

Bandwidth (-3db)

10 GHz

3.5 GHz

>7.5 GHz

>10 GHz

Rise/Fall Time

<35 ps

100 ps

<50 ps

<35 ps

Capacitance

0.2 pF

0.6 pF

0.17 pF

<0.2 pF

Active Area

75 µm dia.

100 µm dia.

50 µm dia.

30 µm dia.

Dark Current

<0.3 nA

<0.4 nA

<0.4 nA

<0.4 nA

Fiber Compatibility

up to 62.5 µm

up to 100 µm

up to 50 µm

single mode

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Transimpedance Amplifier Options

When the light level gets below the mW regime, the expected signal is uncomfortably near the noise floor of most systems. In order to get acceptable signal levels from very low light levels the current from the photodiode must be amplified. In the Series F we use hybrid bipolar technology in Darlington configurations. Expected signal levels can be estimated using the previous equation, but substituting the Transimpedance Gain from the table below in place of the load resistance. It should be noted that the gain figures in the specification below are approximate and that actual performance may differ by up to a factor of two depending on amplifier product variations, output loading and so on.  Other amplifiers are available, call or write for details.

 

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Transimpedance Amplifier Specifications

True DC Coupling with Offset Null - Single Stage

 

Mod 1D

Mod 2D

Mod 4D

Bandwidth (-3dB)

DC to 10 Ghz

DC to 7 GHz

DC to 2.8 GHz

Rise/Fall Time

35 ps

50 ps

125 ps

Transimpedance

200 ohms

300 ohms

2,500 ohms

Noise Figure

5.3 dB @ 2GHz

4.7 dB @ 2GHz

2.6 dB @ 1.5GHz

Output Power (P1dB)

11.3 dBm

12.4 dBm

-2 dBm

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AC Coupling - Single Stage

 

Mod 1A

Mod 2A

Mod 4A

Bandwidth (-3dB)

DC to 10 Ghz

DC to 7 GHz

DC to 2.8 GHz

Rise/Fall Time

35 ps

50 ps

125 ps

Transimpedance

200 ohms

300 ohms

2,500 ohms

Noise Figure

5.3 dB @ 2GHz

4.7 dB @ 2GHz

2.6 dB @ 1.5GHz

Output Power (P1dB)

11.3 dBm

12.4 dBm

-2 dBm

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We have recently greatly increased the amplification available in the AC coupled Photodetector Modules. The new internal multi-stage AC coupled transimpedance amplifiers provide overall conversion gains as high as 60,000 volts/watt in two stages and over a million volts/watt in three stages, allowing detection of sub-microwatt signals.


AC Coupling - Two Stage

 

Mod 11A

Mod 22A

Mod 42A

Mod 44A

Bandwidth (-3dB)

30 kHz to 7 GHz

30 kHz to 5 GHz

30 kHz to 2.8 GHz

30 kHz to 2.0 GHz

Rise/Fall Time

50 ps

70 ps

125ps

175ps

Transimpedance

800 ohms

1,800 ohms

7,500 ohms

60,000 ohms

Noise Figure

6.00 dB @ 2 GHz

5.15 dB @ 2 GHz

2.78 dB @ 1.5 GHz

2.68 dB @ 1.5 GHz

Output Power (P1dB)

11.3 dBm

12.4 dBm

12.4 dBm

-2 dBm

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AC Coupling - Three Stage

 

Mod 111A

Mod 222A

Mod 422A

Mod 442A

Mod 444A

Bandwidth (-3dB)

30kHz to 6GHz

30kHz to 4.5GHz

30kHz to 2.6GHz

30kHz to 2GHz

30kHz to 1.76GHz

Rise/Fall Time

60 ps

75 ps

135 ps

175 ps

200 ps

Transimpedance

3,200 ohms

10,800 ohms

45,000 ohms

200,000 ohms

1.6 x 106 ohms

Noise Figure

6.16 dB @ 2 GHz

5.22 dB @ 2 GHz

2.81 dB @ 1.5 GHz

2.68 dB @ 1.5 GHz

2.68 dB @ 1.5 GHz

Output Power (P1dB)

11.3 dBm

12.4 dBm

12.4 dBm

12.4 dBm

-2dBm

Note: Due to the relatively low output power of the Mod 4 amplifier, those modules with an amplifier Model Number ending in 4 will have Transimpedances about one-half of the value specified above when driving a 50 ohm termination load. For example, the Mod 44A delivers approximately 60,000 volts/amp into a high impedance termination and about 30,000 volts/amp into 50 ohms. For all other models the specified values are valid for either Hi-Z or 50 ohm termination.

Keep in mind that the transimpedance amplifier is an option. If your light levels are adequate, use the basic configuration Series G unamplified but biased photodiode without the added current drain, cost and potential additional noise of an amplifier.

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Estimation of Signal Level

You can estimate the signal level (voltage) that you can expect to see, for your light intensity, directly from the Responsivity as shown in the graph above and in the table below, from:

V [volts] = (I2 – I1 )[watts] • Responsivity [amps/watt] • Z [ohms]

where V is the output signal, I2  and  I1  are the two input light intensities and Z is the amplifier Transimpedance.

 

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Noise Specifications and Measurements

Measurements of the noise spectrum have been made by independent labs on several of our systems. In all measurements the results were consistent with or better than the specifications shown.

An InGaAs-2 Mod1D with DC Offset Null contributed about 1.5mV rms over 20GHz with power on to both amplifiers and the photodiode and no light input. (The scope by itself had an intrinsic noise floor of about 1.2mV rms.) Calculations show this to be consistent with the Noise Figure specified below. The equivalent optical noise density at the input is about 50pW Hz -1/2. An AC coupled InGaAs-2 Mod2A system tested at one of the National Laboratories showed a 0.3mV rms noise floor, also consistent with the Noise Figure. The equivalent optical input noise density is about 30pW Hz-1/2. This system reliably receives digital data at 2.5Gb/s with light levels as low as a few microwatts.

The noise from the photodiodes themselves is several orders of magnitude below that of the amplifiers and may be ignored.

In general, we have found that the noise contributed by our amplified photodiode systems is below or at most comparable to the intrinsic noise floor (about 1mV RMS) of most high speed oscilloscopes and digital data acquisition systems

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Output Electrical Connector

Electronic output connector choices include BNC, TNC, SMA and SMC in either gender. Wiltron-K, 7/16 and others are available at some extra cost. Please note that BNC connectors are not recommended above 2 to 4 GHz. If you need something really unusual, specify on your Request for Quotation or call to discuss your needs.

 

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Output Coupling and DC Offset Null Option

The output signal can be connected directly to the output connector, DC coupling, or through a capacitor, AC output coupling.

Amplified versions which are DC coupled would have an output offset bias of several volts when the photodiode is dark, due to transistor biasing. This offset is eliminated with the Offset Null configuration which uses a second matched reference amplifier to drive the ground side of the output connector. A multi-turn precision pot in the Power Supply controls the input to this second amplifier so that any residual offset due to amplifier mismatch, photodiode dark current or background light can be trimmed out.

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Termination

These modules are designed to be mounted directly onto the input jack of your scope. When used this way there is no coax cable to cause reflections so terminating with exactly 50 ohms is not necessary. The output impedance of the amplified modules is already low so you may set the input impedance of your scope to 1Mohm. The amplifiers will drive a 50 ohm load but there may be a reduction in signal level for certain amplifier configurations as explained above.

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Power Considerations

The amplified Series F modules are powered through a shielded multi-conductor cable.  This cable is fitted with a connector which is compatible with the M,F&A Power Supply.  Any power supply is a potential source of noise. The M,F&A Power Supply provides noise free power to the photodiode and amplifiers from Nickel metal hydride batteries which are re-charged when the photodetector module is not in use. When the photodetector module is active, the system is completely disconnected from the external AC source. A larger rack mount version capable of powering up to four Series F Photodetector Modules is also available.

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Series F Amplified Photodetector Module Summary and Prices

Input Optical Connector:

·                   none

·                   2.5mm ceramic ferrule

·                   NTT-FC

·                   SC

·                   ST

·                   SMA

·                   other_______________

Polish:

·                   UPC
(compatible with flat, PC, and SPC)

·                   PC

·                   APC 8 degrees

·                   other ______________

Optical Cable:

·                   9/125 µm

·                   50/125 µm

·                   62.5/125 µm

·                   other______________

Jacket:

·                   0.9mm buffer only

·                   3mm Kevlar and Polymer over 0.9mm buffer

·                   ______________

Length:

·                   1 meter (standard)

·                   other_________________

Light-Collection Optics:

·                   none

·                   6mm fixed aspheric ($225)

·                   alignable Micro-Rail and "C" thread compatible ($395)

·                   Large Aperture (inquire)

Photodiodes :

·                   GaAs, 450-870nm, 10 GHz ($1,095)

·                   InGaAs-1, 850-1700nm, 3.5 GHz ($795)

·                   InGaAs-2, 850-1700nm, >7.5 GHz ($995)

·                   InGaAs-3, 950-1650nm, >10 GHz ($1,095)

Amplifier and Coupling Options:

True DC Coupling, DC with Offset Null

·                   Mod 1D, 10GHz ($575)

·                   Mod 2D, 7GHz ($575)

·                   Mod 4D, 2.8GHz, 2,500 ohms ($575)

AC Coupling Only

·                   Mod 1A, 10GHz ($275)

·                   Mod 2A, 7GHz ($275)

·                   Mod 4A, 2.8GHz, 2,500 ohms ($275)

·                   Mod 11A, 7GHz ($450)

·                   Mod 22A, 5GHz ($450)

·                   Mod 42A, 2.8GHz, 7,500 ohms($450)

·                   Mod 44A, 2.8GHz, 60,000 ohms($450)

·                   Mod 111A, 3,200 ohms ($625)

·                   Mod 222A, 10,800 ohms ($625)

·                   Mod 422A, 45,000 ohms ($625)

·                   Mod 442A, 200,000 ohms ($625)

·                   Mod 444A, 1.6 x 106 ohms ($625)

Output Electronic Connector:

·                   BNC

·                   TNC

·                   SMA

·                   SMC

·                   other________

Gender:

·                   male plug (as shown)

·                   female jack

Power Configuration:

·                   external power cable, 1 meter shielded

External Power Supply:
(shipped as a separate item)

·                   12volt rechargeable gel-cell with EMI/RFI shielding ($275)

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How to Order

We will build your Photodetectors to your specifications. The price of your detector is simply the sum of the prices of the chosen specified options.  Email us your specifications from the list under Summary and Prices above. We will return a formal quotation to confirm your specifications and expected delivery time. Quantity discounts are available, send a Request for Quotation.

Please note that these modules contain technology at the leading edge of the state of the art. Prices and specifications are subject to change.

 

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Martin, Froeschner & Associates
14300 Mines Road, Livermore, California, 94550
USA

tel: (+1) 925 989 4930
fax: (+1) 925 449 4647
email: sales@mfaoptics.com

 

  Latest update June 2011

©1999-2011

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Contact Us:

tel: +1 925 989 4930
fax: +1 925 449 4647


email: sales@mfaoptics.com

Martin, Froeschner & Associates
14300 Mines Road
Livermore, California
94550
USA



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