"; _cf_contextpath=""; _cf_ajaxscriptsrc="/cfthorscripts/ajax"; _cf_jsonprefix='//'; _cf_websocket_port=8578; _cf_flash_policy_port=1244; _cf_clientid='8BE1CA9E5531366B69938D64D36018DB';/* ]]> */
Ultrafast Fiber Optic Photodetectors
Single Mode, 30 GHz,
The included ECM100 clamp can be used to securely mount the detector on a Ø1/2" post.
Multimode, 25 GHz,
Click to Enlarge
While each DXM Series model is designed and intended for operation over the specified wavelength range, each will respond, with reduced performance, to optical input at shorter wavelengths, as shown by the shaded regions. See the Responsivity plots in the Specs tab for details. Please contact Tech Support for more information.
Janis Valdmanis, Ph.D. Optics
We Design, Develop, and Manufacture
|Frequency Responseb||DC - 12 GHz||DC - 25 GHz||DC - 30 GHz||DC - 20 GHz|
|Internal Fiber Type (Core Diameter)||SMF-28 (9 µm)||OM4 (50 µm)||SMF-28 (9 µm)||OM4 (50 µm)||SMF-28 (9 µm)||OM4 (50 µm)||SMF-28 (9 µm)|
|Impulse Response (FWHM)b||29 ps||19 ps||15 ps||18 ps|
(Into External 50 Ω Load)
|15 V/W||14 V/W||12.5 V/W||11 V/W||19 V/W||16.5 V/W||22.5 V/W|
(At the FC/PC Connector)
|Single Mode Input||0.6 A/W||0.5 A/W||0.5 A/W (850 nm)
0.8 A/W (1310 nm)
0.7 A/W (1550 nm)
|0.9 A/W (1310 nm)
0.9 A/W (1550 nm)
|Multimode Input||-||0.55 A/W||-||0.45 A/W||-||0.45 A/W (850 nm)
0.7 A/W (1310 nm)
0.6 A/W (1550 nm)
|Optical Return Loss||Single Mode Input||-30 dB||-25 dB||-30 dB||-25 dB||-25 dB (850 nm)
-25 dB (1310 nm)
-20 dB (1550 nm)
|-15 dB (850 nm)
-15 dB (1310 nm)
-15 dB (1550 nm)
|-25 dB (1310 nm)
-30 dB (1550 nm)
|Multimode Input||-||-18 dB||-||-18 dB||-||-10 dB (850 nm)
-10 dB (1310 nm)
-10 dB (1550 nm)
|Peak Optical Input Power (Max)c||75 mW||100 mW||50 mW||50 mW|
|Noise Equivalent Power (NEP)d||43 pW/Hz1/2||47 pW/Hz1/2||51 pW/Hz1/2||57 pW/Hz1/2||34 pW/Hz1/2||40 pW/Hz1/2||28 pW/Hz1/2|
|Dark Current (Max)||50 nA|
|Average Optical Input Power (Abs. Max)c||+10 dBm (10 mW)|
|RF Output Voltage (Max)e||1 V|
|Reverse Termination Impedance
|Click the Icons to View Data Graphs|
|Analog Output Transimpedance Gaina||200 mV / mA|
|Analog Outputa||3.5 V (Max Linear)|
|Analog Output Impedancea||High Z|
|Digital Display Output (Max)||20 mA|
|Digital Display Output Resolution||1 nA|
|Fiber Connector||FC/PC, 2.0 mm Narrow Key|
|RF Output Connector||Female 2.92 mm, 50 Ω|
|Current Monitor Connector||Female SMA|
|Power Supplyb,c||+5 VDC, Mini-B USB Connector
(Max Current 500 mA)
|Battery Capacity||500 mA·h|
|Battery Charging Timec||2 h (Typical for Full Charge)|
|Operating Temperature Range||10 °C to 40 °C|
|Storage Temperature Range||0 °C to 50 °C|
|Relative Humidity (Max)||85%|
|Dimensions (without ECM100)||103.0 mm x 61.4 mm x 29.6 mm
(4.05" x 2.42" x 1.17")
ESD Sensitive Components: Please note that the components inside the DXM series units are ESD sensitive. Take all appropriate precautions to discharge personnel and equipment before making any electrical connections to the unit. This especially applies to coaxial connecting cables that can accumulate capacitive charge.
Charging the Detector: The detector arrives with the battery partially charged. The battery can be fully charged using the included charger and USB adapter cable connected to the USB charger jack indicated in Figure 1. The yellow indicator LED, which is also located on the input panel, illuminates to confirm it is charging properly, and the green LED next to it illuminates when the unit is fully charged. The battery may also be charged using USB chargers for phones, tablets, or similar products. These will charge the battery at a maximum rate of 500 mA. Non-dedicated charging USB ports (e.g. those on a PC) will charge at a lower 100 mA rate.
Mounting the Detector: The included ECM100 mounting clamp, also available below, has a single counterbore that accepts a 8-32 (M4) cap screw (not included). Screw the clamp to the desired base or post before snapping it to the side of the detector housing and securing it using the integrated 5/64" (2 mm) locking screw.
RF and Photocurrent Monitor Output: Connection cables attached to the RF output port, shown in Figure 3, and SMA photocurrent monitor port, shown in Figure 1, must be properly shielded. Attach the RF output of the DXM series unit to the measurement instrument using suitable cables or adapters, such at Thorlabs' microwave cables and adapters. The measurement instrument must have a 50 Ω input and adequate bandwidth to resolve the high-speed signal from the DXM series ultrafast detector.
Optical Fiber Input: Ensure the input optical power does not exceed +10 dBm. The FC/PC bulkhead connector used to couple the optical input signal to the detector is located on the input panel of the unit, shown in Figure 1. Fiber connector tips should be cleaned properly before making any connections. While multimode versions of the DXM series may use either single mode or multimode fiber inputs, single mode versions require 9 µm core single mode fiber.
DC Photocurrent Monitor: The DC photocurrent can be monitored directly by viewing the built-in digital display shown in Figure 2, as well as by using most voltmeters to read the analog voltage signal output via the high-impedance SMA jack located on the input panel shown in Figure 1. The units on the displayed digital current measurement can be toggled between µA and mA using the button on the front panel. There may be a small discrepancy (within specification) between the screen and SMA monitor output signal. The digital display reports a wide range of current values, up to 20 mA with a resolution of 1 nA, with the display automatically changing range in response to the signal magnitude. The analog voltage signal sent to the SMA connector has a linear relationship with the measured DC photocurrent up to 3.5 V: the transimpedance gain of the current monitor provides 200 mV per 1 mA of photocurrent. This linear relationship limits the current range reported by the analog SMA output signal, so that the range is smaller than that provided by the digital display.
Cleaning the Housing: Use a soft cloth moistened with mild glass cleaner. Do not spray directly onto unit.
(Female 2.92 mm)
|F1||Photocurrent Monitor Display
|F2||Range Toggle Switch|
(FC/PC, 2.0 mm Narrow Key)
|L2||Current Monitor Output
|L3||Charging Status Indicator LEDs|
|L5||Mini-B USB Charger Jack for +5 VDC Input|
When your application requirements are not met by our range of catalog products or their variety of user-configurable features, please contact me to discuss how we may serve your custom or OEM needs.
Explore the benefits of using a Thorlabs high-speed instrument in your setup and under your test conditions with a demo unit. Contact me for details.
Thorlabs' Ultrafast Optoelectronics Team designs, develops, and manufactures high-speed components and instrumentation for a variety of photonics applications having frequency responses up to 70 GHz. Our extensive experience in high-speed photonics is supported by core expertise in RF/microwave design, optics, fiber optics, optomechanical design, and mixed-signal electronics. As a division of Thorlabs, a company with deep vertical integration and a portfolio of over 20,000 products, we are able to provide and support a wide selection of equipment and continually expand our offerings.
Our catalog and custom products include a range of integrated fiber-optic transmitters, modulator drivers and controllers, detectors, receivers, pulsed lasers, variable optical attenuators, and a variety of accessories. Beyond these products, we welcome opportunities to design and produce custom and OEM products that fall within our range of capabilities and expertise. Some of our key capabilities are:
Our catalog product line includes a range of integrated fiber-optic transmitters, modulator drivers and controllers, detectors, pulsed lasers, and accessories. In addition to these, we offer related items, such as receivers and customized catalog products. The following sections give an overview of our spectrum of custom and catalog products, from fully integrated instruments to component-level modules.
To meet a range of requirements, our fiber-optic instruments span a variety of integration levels. Each complete transmitter includes a tunable laser, a modulator with driver amplifier and bias controller, full control of optical output power, and an intuitive touchscreen interface. The tunable lasers, modulator drivers, and modulator bias controllers are also available separately. These instruments have full remote control capability and can be addressed using serial commands sent from a PC.
Customization options include internal laser sources, operating wavelength ranges, optical fiber types, and amplifier types.
Our component-level, custom and catalog fiber-optic products take advantage of our module design and hermetic sealing capability. Products include detectors with frequency responses up to 50 GHz, and we also specialize in developing fiber-optic receivers, operating up to and beyond 40 GHz, for instrumentation markets. Closely related products include our amplifier modules, which we offer upon request, variable optical attenuators, microwave cables, and cable accessories.
Customization options include single mode and multimode optical fiber options, where applicable, and detectors optimized for time or frequency domain operation.
Our free-space instruments include detectors with frequency responses around 1 GHz and pulsed lasers. Our pulsed lasers generate variable-width, nanosecond-duration pulses, and a range of models with different wavelengths and optical output powers are offered. User-adjustable repetition rates and trigger in/out signals provide additional flexibility, and electronic delay-line products enable experimental synchronization of multiple lasers. We can also adapt our pulsed laser catalog offerings to provide gain-switching capability for the generation of pulses in the 100 ps range.
Customization options for the pulsed lasers include emission wavelength, optical output powers, and sub-nanosecond pulse widths.
Determining whether emission from a pulsed laser is compatible with a device or application can require referencing parameters that are not supplied by the laser's manufacturer. When this is the case, the necessary parameters can typically be calculated from the available information. Calculating peak pulse power, average power, pulse energy, and related parameters can be necessary to achieve desired outcomes including:
Pulsed laser radiation parameters are illustrated in Figure 1 and described in the table. For quick reference, a list of equations are provided below. The document available for download provides this information, as well as an introduction to pulsed laser emission, an overview of relationships among the different parameters, and guidance for applying the calculations.
Peak power and average power calculated from each other:
|Peak power calculated from average power and duty cycle*:|
|*Duty cycle () is the fraction of time during which there is laser pulse emission.|
Figure 1: Parameters used to describe pulsed laser emission are indicated in the plot (above) and described in the table (below). Pulse energy (E) is the shaded area under the pulse curve. Pulse energy is, equivalently, the area of the diagonally hashed region.
|Pulse Energy||E||Joules [J]||A measure of one pulse's total emission, which is the only light emitted by the laser over the entire period. The pulse energy equals the shaded area, which is equivalent to the area covered by diagonal hash marks.|
|Period||Δt||Seconds [s]||The amount of time between the start of one pulse and the start of the next.|
|Average Power||Pavg||Watts [W]||The height on the optical power axis, if the energy emitted by the pulse were uniformly spread over the entire period.|
|Instantaneous Power||P||Watts [W]||The optical power at a single, specific point in time.|
|Peak Power||Ppeak||Watts [W]||The maximum instantaneous optical power output by the laser.|
|Pulse Width||Seconds [s]||A measure of the time between the beginning and end of the pulse, typically based on the full width half maximum (FWHM) of the pulse shape. Also called pulse duration.|
|Repetition Rate||frep||Hertz [Hz]||The frequency with which pulses are emitted. Equal to the reciprocal of the period.|
Is it safe to use a detector with a specified maximum peak optical input power of 75 mW to measure the following pulsed laser emission?
The energy per pulse:
seems low, but the peak pulse power is:
It is not safe to use the detector to measure this pulsed laser emission, since the peak power of the pulses is >5 orders of magnitude higher than the detector's maximum peak optical input power.
The each of our DXM Series includes one ECM100 anodized aluminum clamp, which snaps onto the bottom of the detector's housing and is secured by tightening the flexure lock using the 2 mm (5/64") hex locking screw. Additional ECM100 clamps are available separately. The ECM100 is part of Thorlabs' family of aluminum side clamps that are designed to securely mount Thorlabs' rectangular electronics housings.
The ECM100 has one #8 (M4) counterbored through hole, allowing the clamp to be mounted onto a Ø1/2" post or any surface with an 8-32 (M4) tap. The clamp must be mounted via the counterbored through hole before the electronics housing is attached, as the counterbore will not be accessible once the housing is secured in the clamp.
The DS5 is a 5 V regulated power supply with a USB Type-A female port. It can be used with any USB-compatible device that accepts a 5 VDC output, and is directly compatible with our DXM series of ultrafast fiber optic detectors and our RXM series of ultrafast fiber optic receivers when used with the USB-AB-72 USB cable (sold separately). In addition to the USB-AB-72, we also offer other USB 2.0 cables. A region-specific adapter plug is shipped with the DS5 power supply unit based on your location.