Quantum and Interband Cascade Lasers: Distributed Feedback, HHL Package
![](https://www.thorlabs.us/Images/GuideImages/10151_DFB_QCL_HHL_1.jpg)
- DFB QCLs and ICL in Thermoelectrically Cooled HHL Packages
- Center Wavelengths Between 3.00 and 11.00 µm (3333 and 909 cm-1)
- Output Power up to 150 mW, Depending on Model
- Custom Wavelengths, Packages, and Output Powers
Available Upon Request
QD8500HHLH
Horizontal HHL Package
(Linewidth Shown is Limited by Measurement Resolution)
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MIR Laser Types | |
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Fabry-Perot | TO Can |
Two-Tab C-Mount | |
D-Mount | |
HHL | |
Turnkey | |
Distributed Feedback |
Two-Tab C-Mount |
D-Mount | |
HHL | |
Turnkey |
Webpage Features | |
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Clicking this icon opens a window that contains specifications and mechanical drawings. |
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Clicking this icon allows you to download our standard support documentation. |
Choose Item |
Clicking the words "Choose Item" opens a drop-down list containing all of the in-stock lasers around the desired center wavelength. The red icon next to the serial number then allows you to download L-I-V and spectral measurements for that serial-numbered device. |
Features
- Single-Wavelength Distributed Feedback Quantum or Interband Cascade Lasers (DFB QCLs and ICLs)
- High Heat Load Package Simplifies Thermal Management and System Integration
- Collimated Laser Emission Through Wedged Window
- Used in Chemical Analysis, Sensing, and IR Countermeasures
- Custom Packages and Wavelengths from 3 to 12 µm Available via Tech Support
The MIR quantum and interband cascade lasers on this webpage are offered in high heat load (HHL) packages with industry-standard pinouts and package dimensions. Each package incorporates a built-in thermistor and thermoelectric cooler (TEC) for active temperature management and prolonged laser lifetime, and also includes an internal aspheric lens that collimates the laser's output.
Distributed feedback QCLs and ICLs emit at a well defined center wavelength, making them popular for applications such as chemical sensing and sample analysis. They provide single transverse mode operation. By tuning the input current and operating temperature, the laser output can be tuned over a narrow range of at least 1 cm-1. Before shipment, the output spectrum, optical power, and L-I-V curve are measured for each serial-numbered device by an automated test station. These measurements are available below and are also included on a data sheet with the laser.
Our ICLs emit a horizontally polarized beam at wavelengths as long as 4.0 µm, while our QCLs emit a vertically polarized beam at wavelengths as long as 11 µm. ICLs will also typically have lower voltage requirements and threshold currents, thus leading to lower optical output powers. Conversely, QCLs will consume more power and will therefore have higher output powers.
Some of Thorlabs' high heat load DFB quantum and interband cascade lasers are uniquely suited for gas sensing and analysis. Select high heat load QCLs are designed to emit at wavelengths ideal for many gases commonly studied in spectroscopy (see the Spectroscopy tab for more information). These DFB quantum cascade lasers are guaranteed to reach their specified wavelengths within their tuning range and are single wavelength, allowing them to be tuned to specific gas spectra. Thorlabs also sells the ID3250HHLH interband cascade laser, which can be used for methane sensing. A list of these QCLs can be found in the Spectroscopy tab above, and more information is available by clicking on the blue info icons () next to the relevant Item #s below.
Package Details
As measured from the bottom of the package, the emission height is 12.7 ± 0.13 mm. The output beam is collimated by an AR-coated black diamond aspheric lens and then coupled out of the package through a wedged zinc sulfide (ZnS) window. This wedge prevents back reflections from returning to the laser chip, but also causes the output beam to deviate downward from the normal by either 2.0° ± 1.5° or 2.0° ± 0.75°, as shown in the Drawing tab of the blue info icons () below. Our stocked lasers are sealed, although the seal is not hermetic; hermetically sealed versions are available by contacting Tech Support.
Each laser is electrically isolated from its mount. Heat loads for these lasers can be up to 38 W, so they must be mounted on a thermally conductive surface to prevent heat buildup. Thorlabs' LCM100(/M) liquid-cooled mount is designed specifically to provide additional thermal regulation of the HHL laser package. The CAB4007A and CAB4007B dual laser diode and TEC connector cables are also available to connect an ITC400xQCL series controller to the LCM100(/M) mount or directly to an HHL laser package, respectively. Please note that third-party cables for high heat load packages are typically not rated for the 4.5 A maximum current of the internal thermoelectric cooler. The Handling tab contains more tips and information. These QCLs and ICLs are specified for CW output. While pulsed output is possible, this application prohibits current tuning, and performance is not guaranteed. These lasers do not have built-in monitor photodiodes and therefore cannot be operated in constant power mode.
For OEM applications, Thorlabs also offers QCLs on a compact D-mount package (12.0 mm × 4.5 mm × 2.8 mm).
![High-Power QCLs](https://www.thorlabs.us/images/TabImages/Custom_DFB_QCL_Wavelengths_G2-250.gif)
Click to Enlarge
Available Wavelengths for Custom DFB Lasers
DFB QCLs at Custom Wavelengths
Thorlabs manufactures custom and OEM quantum cascade lasers in high volumes. We maintain a broad chip inventory at our Jessup, Maryland laser manufacturing facility (see the graph to the left), and can deliver DFB lasers with custom center wavelengths that are qualified to a user-defined wavelength precision.
More details are available on the Custom & OEM Lasers tab. To inquire about pricing and availability, please contact us. A semiconductor specialist will contact you within 24 hours or the next business day.
Current and Temperature Controllers
Use the tables below to select a compatible controller for our MIR lasers. The first table lists the controllers with which a particular MIR laser is compatible, and the second table contains selected information on each controller. Complete information on each controller is available in its full web presentation. We particularly recommend our ITC4002QCL and ITC4005QCL controllers, which have high compliance voltages of 17 V and 20 V, respectively. Together, these drivers support the current and voltage requirements of our entire line of Mid-IR Lasers. To get L-I-V and spectral measurements of a specific, serial-numbered device, click "Choose Item" next to the part number below, then click on the Docs Icon next to the serial number of the device.
Laser and Controller Compatibility
Laser Item # | Wavelength | Current Controllers | Dual Current / Temperature Controllers | ||
---|---|---|---|---|---|
Small Benchtop | Large Benchtop | Large Benchtop | Rack Mounted | ||
ID3250HHLHa | 3.00 to 3.50 µm (3333 to 2857 cm-1) |
LDC205C LDC210C |
- | ITC4002QCL | - |
ID3750HHLHa | 3.50 to 4.00 µm (2857 to 2500 cm-1) |
LDC205C LDC210C |
- | ITC4002QCL | - |
QD4500HHLHa | 4.00 to 5.00 µm (2500 to 2000 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
QD4472HHa | 4.472 µm (2236 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
QD4602HHa | 4.602 µm (2173 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
QD5500HHLHa | 5.00 to 6.00 µm (2000 to 1667 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
QD5263HHa | 5.263 µm (1900 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
QD6500HHLHa | 6.00 to 7.00 µm (1667 to 1429 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
QD6134HHa | 6.134 µm (1630 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
QD7500HHLHa | 7.00 to 8.00 µm (1429 to 1250 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
QD7416HHa | 7.416 µm (1900 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
QD7716HHa | 7.716 µm (1296 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
QD7901HHa | 7.901 µm (1266 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
QD8500HHLHa | 8.00 - 9.00 µm (1250 - 1111 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
QD8912HHa | 8.912 µm (1122.1 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
QD9500HHLHa | 9.00 - 10.00 µm (1111 - 1000 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
QD9062HHa | 9.062 µm (1103.5 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
QD9697HHa | 9.697 µm (1031 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
QD10500HHLHa | 10.00 to 11.00 µm (1000 to 909 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
QD10530HHa | 10.530 µm (949.7 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
QD10549HHa | 10.549 µm (948 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
QD10622HHa | 10.622 µm (941 cm-1) |
- | - | ITC4002QCL, ITC4005QCL | - |
Controller Selection Guide
Controller Item # | Controller Type | Controller Package | Current Range | Current Resolution | Voltage |
---|---|---|---|---|---|
LDC205C | Current | Small Benchtop (146 mm x 66 mm x 290 mm) |
0 to ±0.5 A | 10 µA | >10 V |
LDC210C | 0 to ±1 A | 100 µA | |||
ITC4002QCL | Current / Temperature | Large Benchtop (263 mm x 122 mm x 307 mm) |
0 to 2 A | 100 µA (Front Panel) 32 µA (Remote Control) |
17 V |
ITC4005QCL | 0 to 5 A | 1 mA (Front Panel) 80 µA (Remote Control) |
20 V |
Do
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Do Not
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Handling High Heat Load Lasers
Proper precautions must be taken when handling and using high heat load lasers. Otherwise, permanent damage to the device will occur. Members of our Technical Support staff are available to discuss possible operation issues.
Avoid Static
Since these lasers are sensitive to electrostatic shock, they should always be handled using standard static avoidance practices.
Avoid Dust and Other Particulates
Contamination of the window must be avoided. Do not blow on the window or expose it to smoke, dust, oils, or adhesive films. The window is particularly sensitive to dust accumulation. During standard operation, dust can burn onto it, which will lead to premature degradation of the laser performance. If operating a high heat load laser for long periods of time outside a cleanroom, it should be sealed in a container to prevent dust accumulation.
Use a Current Source Specifically Designed for Lasers
These lasers should always be used with a high-quality constant current driver specifically designed for use with lasers. Lab-grade power supplies will not provide the low current noise required for stable operation, nor will they prevent current spikes that result in immediate and permanent damage.
Thermally Regulate the Laser
Temperature regulation is required to operate the laser for any amount of time. The temperature regulation apparatus should be rated to dissipate the maximum heat load that can be drawn by the laser. For our high heat load DFB QCLs and ICLs, this value is 38 W.
The bottom face of the high heat load package is machined flat to make proper thermal contact with a heat sink. Ideally, the heat sink will be actively temperature regulated to ensure proper heat conduction. Thorlabs' LCM100(/M) Liquid-Cooled Mount for HHL lasers is capable of disipating up to 140 W of heat at 25 °C making it an ideal choice for temperature-controlled operation of HHL lasers. A fan may also serve to move the heat away from the package and prevent thermal runaway. However, the fan should not blow air on or at the laser itself. Thermal grease, pyrolytic graphite, and water cooling methods may also be employed for temperature regulation.
For assistance in picking a suitable temperature controller for your application, please contact Tech Support.
Carefully Make Electrical Connections
When making electrical connections, care must be taken. The flux fumes created by soldering can cause laser damage, so care must be taken to avoid this.
Although soldering to the leads of our HHL lasers is possible, we generally recommend using cables specifically designed for HHL packages. Thorlabs' CAB4007B LD / TEC cable is specifically designed to connect any standard HHL laser package directly to the ITC400xQCL series of laser diode and TEC controllers. The CAB4007A LD / TEC cable can be used to connect an ITC400xQCL controller directly to the LCM100(/M) mount. Please note that third-party cables for high heat load packages are typically not rated for the 4.5 A maximum current of the internal thermoelectric cooler. If soldering to the leads on an HHL package, the maximum soldering temperature and time are 250 °C and 10 seconds, respectively.
Minimize Physical Handling
As any interaction with the package carries the risk of contamination and damage, any movement of the laser should be planned in advance and carefully carried out. It is important to avoid mechanical shocks. Dropping the laser package from any height can cause the unit to permanently fail.
Selected Distributed Feedback QCLs and ICLsa | ||
---|---|---|
Item # | Nominal Center Frequency | Targeted Gas |
ID3250HHLH | 3076 cm-1 (3.25 µm) | CH4 (Methane) |
QD4472HH | 2236 cm-1 (4.472 µm) | N2O (Nitrous Oxide) |
QD4602HH | 2173 cm-1 (4.602 µm) | CO (Carbon Monoxide) |
QD5263HH | 1900 cm-1 (5.263 µm) | NO (Nitric Oxide) |
QD6134HH | 1630 cm-1 (6.134 µm) | NO2 (Nitrogen Dioxide) |
QD7416HH | 1348 cm-1 (7.416 µm) | SO2 (Sulfur Dioxide) |
QD7716HH | 1296 cm-1 (7.716 µm) | N2O (Nitrous Oxide) |
QD7901HH | 1266 cm-1 (7.901 µm) | H2S (Hydrogen Sulfide) |
QD8912HH | 1122.1 cm-1 (8.912 µm) | NH3 (Ammonia) |
QD9062HH | 1103.5 cm-1 (9.062 µm) | NH3 (Ammonia) |
QD9697HH | 1031 cm-1 (9.697 µm) | O3 (Ozone) |
QD10530HH | 949.7 cm-1 (10.530 µm) | C2H4 (Ethylene) |
QD10549HH | 948 cm-1 (10.549 µm) | SF6 (Sulfur Hexafluoride) |
QD10622HH | 941 cm-1 (10.622 µm) | N2H4 (Hydrazine) |
Gas-Phase Spectroscopy Using Distributed Feedback Lasers
Distributed Feedback Quantum and Interband Cascade Lasers (DFB QCLs and ICLs) offer many attractive features for spectroscopy. They emit at a single wavelength within the mid-IR, where many gaseous species characteristically absorb. Moreover, their emission wavelength is easily tuned (typical tuning range: 1 - 5 cm-1) by changing the drive current and operating temperature of the laser, making them ideal for isolating narrow gas absorption lines. Finally, quantum cascade lasers offer relatively high output power (typically 40 - 120 mW at rollover current), helping improve measurement sensitivity. ICLs will typically have a low output power, but a far lower power consumption.
The DFB QCLs on this page emit at wavelengths that range from 4.472 to 11.00 µm (2173 cm-1 to 909 cm-1), while our DFB ICLs emit at wavelengths that range from 3.00 to 4.00 µm (3333 cm-1 to 2500 cm-1). If we do not stock the wavelength required for your application, custom wavelengths are available by contacting Tech Support.
The tuning range of individual DFB QCLs and ICLs depends greatly on the actual laser device. Each DFB QCL or ICL is a unique device with its own threshold current, rollover current, and spectrum. Since the wavelength and power of DFB QCLs and ICLs change over the tuning range, operating the lasers near the rollover current is not always desirable in spectroscopy measurements, which require specific wavelengths. The driving current and operating temperature of DFB QCLs and ICLs can be adjusted to change the output signal to the desired wavelength and power.
An example absorption spectrum of nitric oxide (NO) is shown below on the left. The highlighted blue region, centered on 1900 cm-1, overlaps with the tuning range of the QD5263HH QCL; tuning data from a sample QD5263HH QCL is shown below to the right for comparison. The QD5263HH QCLs can be precisely tuned to the NO absorption peak at 1900 cm-1. Click on the blue icons () below for more information on how the emission of each laser in the table above overlaps with the absorption profile of the targeted gas.
DFB QCLs and ICLs are ideal for use in photoacoustic spectroscopy, a technique based on the photoacoustic effect that is able to accurately detect trace gas concentrations for a wide variety of applications. Thorlabs offers an Acoustic Detection Module that can be used with our DFB QCLs and ICLs to build custom QEPAS sensors that target the absorption of a specific gas. We also offer a Quartz-Enhanced Photoacoustic Sensor that targets a methane absorption line to detect trace amounts of methane in a gas.
![]() Click to Enlarge The shaded region overlaps the tuning range of the QD5263HH distributed feedback QCL. See the graph to the right for tuning data from a sample QD5263HH QCL. |
![]() Click to Enlarge Tuning data for a sample QD5263HH distributed feedback QCL. See the graph to the left for the absorption peaks of nitric oxide (NO) that can be detected using this laser. |
![Laser Packages of QCLs](https://www.thorlabs.us/images/TabImages/Custom_QCL_Packages_A4-400.jpg)
Click to Enlarge
Some of Our Available Packages
![Wire Bonding](https://www.thorlabs.us/images/TabImages/Wire_Bonding_QCL_A1-150.jpg)
Click for Details
Wire Bonding a Quantum Cascade Laser on a C-Mount
Custom & OEM Quantum Cascade and Interband Cascade Lasers
At our semiconductor manufacturing facility in Jessup, Maryland, we build fully packaged mid-IR lasers and gain chips. Our engineering team performs in-house epitaxial growth, wafer fabrication, and laser packaging. We maintain chip inventory from 3 µm to 12 µm, and our vertically integrated facilities are well equipped to fulfill unique requests.
High-Power Fabry-Perot QCLs
For Fabry-Perot lasers, we can reach multi-watt output power on certain custom orders. The available power depends upon several factors, including the wavelength and the desired package.
DFB QCLs at Custom Wavelengths
For distributed feedback (DFB) lasers, we can deliver a wide range of center wavelengths with user-defined wavelength precision. Our semiconductor specialists will take your application requirements into account when discussing the options with you.
The graphs below and photos to the right illustrate some of our custom capabilities. Please visit our semiconductor manufacturing capabilities presentation to learn more.
![Custom QCL Wavelengths](https://www.thorlabs.us/images/TabImages/Custom_QCL_Wavelengths_G2-300.gif)
Click to Enlarge
Available Wavelengths for Custom QCLs and ICLs
![High-Power QCLs](https://www.thorlabs.us/images/TabImages/High-Power_QCLs_G4-300.gif)
Click to Enlarge
Maximum Output Power of Custom Fabry-Perot QCLs
![QCL Gain Chips](https://www.thorlabs.us/images/TabImages/QCL_Gain_Chips_G1-300.gif)
Click to Enlarge
Electroluminescence Spectra of Available Gain Chip Material
Insights into QCLs and ICLs
Scroll down to read about:
- QCLs and ICLs: Operating Limits and Thermal Rollover
Click here for more insights into lab practices and equipment.
QCLs and ICLs: Operating Limits and Thermal Rollover
![L-I curves for QCL mount held at different temperatures](https://www.thorlabs.us/images/tabimages/QCL_LI_Curve_Set_General_A2-330.gif)
Click to Enlarge
Figure 2: This set of L-I curves for a QCL laser illustrates that the mount temperature can affect the peak operating temperature, but that using a temperature controlled mount does not remove the danger of applying a driving current large enough to exceed the rollover point and risk damaging the laser.
![L-I curve for QCL laser, rollover region indicated](https://www.thorlabs.us/images/tabimages/QCL_LI_Curve_General_A2-330.gif)
Click to Enlarge
Figure 1: This example of an L-I curve for a QCL laser illustrates the typical non-linear slope and rollover region exhibited by QCL and ICL lasers. Operating parameters determine the heat load carried by the lasing region, which influences the peak output power. This laser was installed in a temperature controlled mount set to 25 °C.
The light vs. driving current (L-I) curves measured for quantum and interband cascade Lasers (QCLs and ICLs) include a rollover region, which is enclosed by the red box in Figure 1.
The rollover region includes the peak output power of the laser, which corresponds to a driving current of just under 500 mA in this example. Applying higher drive currents risks damaging the laser.
Laser Operation
These lasers operate by forcing electrons down a controlled series of energy steps, which are created by the laser's semiconductor layer structure and an applied bias voltage. The driving current supplies the electrons.
An electron must give up some of its energy to drop down to a lower energy level. When an electron descends one of the laser's energy steps, the electron loses energy in the form of a photon. But, the electron can also lose energy by giving it to the semiconductor material as heat, instead of emitting a photon.
Heat Build Up
Lasers are not 100% efficient in forcing electrons to surrender their energy in the form of photons. The electrons that lose their energy as heat cause the temperature of the lasing region to increase.
Conversely, heat in the lasing region can be absorbed by electrons. This boost in energy can scatter electrons away from the path leading down the laser's energy steps. Later, scattered electrons typically lose energy as heat, instead of as photons.
As the temperature of the lasing region increases, more electrons are scattered, and a smaller fraction of them produce light instead of heat. Rising temperatures can also result in changes to the laser's energy levels that make it harder for electrons to emit photons. These processes work together to increase the temperature of the lasing region and to decrease the efficiency with which the laser converts current to laser light.
Operating Limits are Determined by the Heat Load
Ideally, the slope of the L-I curve would be linear above the threshold current, which is around 270 mA in Figure 1. Instead, the slope decreases as the driving current increases, which is due to the effects from the rising temperature of the lasing region. Rollover occurs when the laser is no longer effective in converting additional current to laser light. Instead, the extra driving creates only heat. When the current is high enough, the strong localized heating of the laser region will cause the laser to fail.
A temperature controlled mount is typically necessary to help manage the temperature of the lasing region. But, since the thermal conductivity of the semiconductor material is not high, heat can still build up in the lasing region. As illustrated in Figure 2, the mount temperature affects the peak optical output power but does not prevent rollover.
The maximum drive current and the maximum optical output power of QCLs and ICLs depend on the operating conditions, since these determine the heat load of the lasing region.
Date of Last Edit: Dec. 4, 2019
Posted Comments: | |
Mike H
 (posted 2022-10-05 17:46:08.467) I don't see any information about pinouts for the HHL package. They don't appear to match any of the cables suggested with the QCL drivers. ksosnowski
 (posted 2022-10-07 11:25:40.0) Thanks for reaching out to Thorlabs. The pinouts for each diode can be found on the last page of the spec sheet. Unfortunately we do not have a cable or mount for the HHL package currently. Although soldering to the leads of our HHL lasers is possible, we generally recommend using cables specifically designed for HHL packages. Please note that third-party cables for high heat load packages are typically not rated for the 4.5 A maximum current of the internal thermoelectric cooler. If soldering to the leads on an HHL package, the maximum soldering temperature and time are 250 °C and 10 seconds, respectively. harshad pansuriya
 (posted 2021-12-20 03:42:18.6) we are interesting for this product
we are working in gas analyzer development jgreschler
 (posted 2021-12-23 10:44:01.0) Thank you for reaching out to Thorlabs. I have reached out to you directly to discuss this further. user
 (posted 2020-07-28 07:57:43.757) Hello,
I would like to know if I can push the power output of the laser diode to higher values then the ones given here. The way that I understood the limitations of the diode is as follows: When applying a DC current to the diode there is a threshold such that increasing the current intensity will not result in higher output powers, but rather just heat up the laser diode. So I was wondering if I could circumvent the heat build-up inside the diode by only using the laser diode to shot pulses of the order of 100 micros. My hope is that during those short pulses higher power output values will be reached without overheating the lasing material.
I was wondering if this strategy is legit or if it will most likely damage the laser diode. I am happy about any thoughts or comments. Thanks in advance. YLohia
 (posted 2020-07-30 03:11:27.0) Hello, thank you for contacting Thorlabs. It is indeed possible to get high powers out of these, either with pulsed operation or with adequate cooling. I have reached out to you directly to discuss this further. |
The rows shaded green below denote single-frequency lasers. |
Item # | Wavelength | Output Power | Operating Current | Operating Voltage | Beam Divergence | Laser Mode | Package | |
---|---|---|---|---|---|---|---|---|
Parallel | Perpendicular | |||||||
L375P70MLD | 375 nm | 70 mW | 110 mA | 5.4 V | 9° | 22.5° | Single Transverse Mode | Ø5.6 mm |
L404P400M | 404 nm | 400 mW | 370 mA | 4.9 V | 13° (1/e2) | 42° (1/e2) | Multimode | Ø5.6 mm |
LP405-SF10 | 405 nm | 10 mW | 50 mA | 5.0 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
L405P20 | 405 nm | 20 mW | 38 mA | 4.8 V | 8.5° | 19° | Single Transverse Mode | Ø5.6 mm |
LP405C1 | 405 nm | 30 mW | 75 mA | 4.3 V | 1.4 mrad | 1.4 mrad | Single Transverse Mode | Ø3.8 mm, SM Pigtail with Collimator |
L405G2 | 405 nm | 35 mW | 50 mA | 4.9 V | 10° | 21° | Single Transverse Mode | Ø3.8 mm |
DL5146-101S | 405 nm | 40 mW | 70 mA | 5.2 V | 8° | 19° | Single Transverse Mode | Ø5.6 mm |
L405A1 | 405 nm | 175 mW (Min) | 150 mA | 5.0 V | 9° | 20° | Single Transverse Mode | Ø5.6 mm |
LP405-MF300 | 405 nm | 300 mW | 350 mA | 4.5 V | - | - | Multimode | Ø5.6 mm, MM Pigtail |
L405G1 | 405 nm | 1000 mW | 900 mA | 5.0 V | 13° | 45° | Multimode | Ø9 mm |
LP450-SF25 | 450 nm | 25 mW | 75 mA | 5.0 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
L450G3 | 450 nm | 100 mW (Min) | 80 mA | 5.2 V | 8.4° | 21.5° | Single Transverse Mode | Ø3.8 mm |
L450G2 | 450 nm | 100 mW (Min) | 80 mA | 5.0 V | 8.4° | 21.5° | Single Transverse Mode | Ø5.6 mm |
L450P1600MM | 450 nm | 1600 mW | 1200 mA | 4.8 V | 7° | 19 - 27° | Multimode | Ø5.6 mm |
L473P100 | 473 nm | 100 mW | 120 mA | 5.7 V | 10 | 24 | Single Transverse Mode | Ø5.6 mm |
LP488-SF20 | 488 nm | 20 mW | 70 mA | 6.0 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
LP488-SF20G | 488 nm | 20 mW | 80 mA | 5.5 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
L488P60 | 488 nm | 60 mW | 75 mA | 6.8 V | 7° | 23° | Single Transverse Mode | Ø5.6 mm |
LP515-SF3 | 515 nm | 3 mW | 50 mA | 5.3 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
L515A1 | 515 nm | 10 mW | 50 mA | 5.4 V | 6.5° | 21° | Single Transverse Mode | Ø5.6 mm |
LP520-SF15A | 520 nm | 15 mW | 100 mA | 7.0 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
LP520-SF15 | 520 nm | 15 mW | 140 mA | 6.5 V | - | - | Single Transverse Mode | Ø9 mm, SM Pigtail |
L520A1 | 520 nm | 30 mW (Min) | 80 mA | 5.5 V | 8° | 22° | Single Transverse Mode | Ø5.6 mm |
PL520 | 520 nm | 50 mW | 250 mA | 7.0 V | 7° | 22° | Single Transverse Mode | Ø3.8 mm |
L520P50 | 520 nm | 45 mW | 150 mA | 7.0 V | 7° | 22° | Single Transverse Mode | Ø5.6 mm |
L520A2 | 520 nm | 110 mW (Min) | 225 mA | 5.9 V | 8° | 22° | Single Transverse Mode | Ø5.6 mm |
DJ532-10 | 532 nm | 10 mW | 220 mA | 1.9 V | 0.69° | 0.69° | Single Transverse Mode | Ø9.5 mm (non-standard) |
DJ532-40 | 532 nm | 40 mW | 330 mA | 1.9 V | 0.69° | 0.69° | Single Transverse Mode | Ø9.5 mm (non-standard) |
LP633-SF50 | 633 nm | 50 mW | 170 mA | 2.6 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
HL63163DG | 633 nm | 100 mW | 170 mA | 2.6 V | 8.5° | 18° | Single Transverse Mode | Ø5.6 mm |
LPS-635-FC | 635 nm | 2.5 mW | 70 mA | 2.2 V | - | - | Single Transverse Mode | Ø9 mm, SM Pigtail |
LPS-PM635-FC | 635 nm | 2.5 mW | 60 mA | 2.2 V | - | - | Single Transverse Mode | Ø9.0 mm, PM Pigtail |
L635P5 | 635 nm | 5 mW | 30 mA | <2.7 V | 8° | 32° | Single Transverse Mode | Ø5.6 mm |
HL6312G | 635 nm | 5 mW | 50 mA | <2.7 V | 8° | 31° | Single Transverse Mode | Ø9 mm |
LPM-635-SMA | 635 nm | 8 mW | 50 mA | 2.2 V | - | - | Multimode | Ø9 mm, MM Pigtail |
LP635-SF8 | 635 nm | 8 mW | 60 mA | 2.3 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
HL6320G | 635 nm | 10 mW | 60 mA | 2.2 V | 8° | 31° | Single Transverse Mode | Ø9 mm |
HL6322G | 635 nm | 15 mW | 75 mA | 2.4 V | 8° | 30° | Single Transverse Mode | Ø9 mm |
L637P5 | 637 nm | 5 mW | 20 mA | <2.4 V | 8° | 34° | Single Transverse Mode | Ø5.6 mm |
LP637-SF50 | 637 nm | 50 mW | 140 mA | 2.6 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
LP637-SF70 | 637 nm | 70 mW | 220 mA | 2.7 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
HL63142DG | 637 nm | 100 mW | 140 mA | 2.7 V | 8° | 18° | Single Transverse Mode | Ø5.6 mm |
HL63133DG | 637 nm | 170 mW | 250 mA | 2.8 V | 9° | 17° | Single Transverse Mode | Ø5.6 mm |
HL6388MG | 637 nm | 250 mW | 340 mA | 2.3 V | 10° | 40° | Multimode | Ø5.6 mm |
L637G1 | 637 nm | 1200 mW | 1100 mA | 2.5 V | 10° | 32° | Multimode | Ø9 mm (non-standard) |
L638P040 | 638 nm | 40 mW | 92 mA | 2.4 V | 10° | 21° | Single Transverse Mode | Ø5.6 mm |
L638P150 | 638 nm | 150 mW | 230 mA | 2.7 V | 9 | 18 | Single Transverse Mode | Ø3.8 mm |
L638P200 | 638 nm | 200 mW | 280 mA | 2.9 V | 8 | 14 | Single Transverse Mode | Ø5.6 mm |
L638P700M | 638 nm | 700 mW | 820 mA | 2.2 V | 9° | 35° | Multimode | Ø5.6 mm |
HL6358MG | 639 nm | 10 mW | 40 mA | 2.4 V | 8° | 21° | Single Transverse Mode | Ø5.6 mm |
HL6323MG | 639 nm | 30 mW | 100 mA | 2.5 V | 8.5° | 30° | Single Transverse Mode | Ø5.6 mm |
HL6362MG | 640 nm | 40 mW | 90 mA | 2.5 V | 10° | 21° | Single Transverse Mode | Ø5.6 mm |
LP642-SF20 | 642 nm | 20 mW | 90 mA | 2.5 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
LP642-PF20 | 642 nm | 20 mW | 110 mA | 2.5 V | - | - | Single Transverse Mode | Ø5.6 mm, PM Pigtail |
HL6364DG | 642 nm | 60 mW | 120 mA | 2.5 V | 10° | 21° | Single Transverse Mode | Ø5.6 mm |
HL6366DG | 642 nm | 80 mW | 150 mA | 2.5 V | 10° | 21° | Single Transverse Mode | Ø5.6 mm |
HL6385DG | 642 nm | 150 mW | 250 mA | 2.6 V | 9° | 17° | Single Transverse Mode | Ø5.6 mm |
L650P007 | 650 nm | 7 mW | 28 mA | 2.2 V | 9° | 28° | Single Transverse Mode | Ø5.6 mm |
LPS-660-FC | 658 nm | 7.5 mW | 65 mA | 2.6 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
LP660-SF20 | 658 nm | 20 mW | 80 mA | 2.6 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
LPM-660-SMA | 658 nm | 22.5 mW | 65 mA | 2.6 V | - | - | Multimode | Ø5.6 mm, MM Pigtail |
HL6501MG | 658 nm | 30 mW | 75 mA | 2.6 V | 8.5° | 22° | Single Transverse Mode | Ø5.6 mm |
L658P040 | 658 nm | 40 mW | 75 mA | 2.2 V | 10° | 20° | Single Transverse Mode | Ø5.6 mm |
LP660-SF40 | 658 nm | 40 mW | 135 mA | 2.5 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
LP660-SF60 | 658 nm | 60 mW | 210 mA | 2.4 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
HL6544FM | 660 nm | 50 mW | 115 mA | 2.3 V | 10° | 17° | Single Transverse Mode | Ø5.6 mm |
LP660-SF50 | 660 nm | 50 mW | 140 mA | 2.3 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
HL6545MG | 660 nm | 120 mW | 170 mA | 2.45 V | 10° | 17° | Single Transverse Mode | Ø5.6 mm |
L660P120 | 660 nm | 120 mW | 175 mA | 2.5 V | 10° | 17° | Single Transverse Mode | Ø5.6 mm |
L670VH1 | 670 nm | 1 mW | 2.5 mA | 2.6 V | 10° | 10° | Single Transverse Mode | TO-46 |
LPS-675-FC | 670 nm | 2.5 mW | 55 mA | 2.2 V | - | - | Single Transverse Mode | Ø9 mm, SM Pigtail |
HL6748MG | 670 nm | 10 mW | 30 mA | 2.2 V | 8° | 25° | Single Transverse Mode | Ø5.6 mm |
HL6714G | 670 nm | 10 mW | 55 mA | <2.7 V | 8° | 22° | Single Transverse Mode | Ø9 mm |
HL6756MG | 670 nm | 15 mW | 35 mA | 2.3 V | 8° | 24° | Single Transverse Mode | Ø5.6 mm |
LP685-SF15 | 685 nm | 15 mW | 55 mA | 2.1 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
HL6750MG | 685 nm | 50 mW | 70 mA | 2.3 V | 9° | 21° | Single Transverse Mode | Ø5.6 mm |
HL6738MG | 690 nm | 30 mW | 85 mA | 2.5 V | 8.5° | 19° | Single Transverse Mode | Ø5.6 mm |
LP705-SF15 | 705 nm | 15 mW | 55 mA | 2.3 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
HL7001MG | 705 nm | 40 mW | 75 mA | 2.5 V | 9° | 18° | Single Transverse Mode | Ø5.6 mm |
LP730-SF15 | 730 nm | 15 mW | 70 mA | 2.5 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
HL7302MG | 730 nm | 40 mW | 75 mA | 2.5 V | 9° | 18° | Single Transverse Mode | Ø5.6 mm |
L760VH1 | 760 nm | 0.5 mW | 3 mA (Max) | 2.2 V | 12° | 12° | Single Frequency | TO-46 |
DBR760PN | 761 nm | 9 mW | 125 mA | 2.0 V | - | - | Single Frequency | Butterfly, PM Pigtail |
L763VH1 | 763 nm | 0.5 mW | 3 mA (Max) | 2.0 V | 10° | 10° | Single Frequency | TO-46 |
DBR767PN | 767 nm | 23 mW | 220 mA | 1.87 V | - | - | Single Frequency | Butterfly, PM Pigtail |
DBR770PN | 770 nm | 35 mW | 220 mA | 1.92 V | - | - | Single Frequency | Butterfly, PM Pigtail |
L780P010 | 780 nm | 10 mW | 24 mA | 1.8 V | 8° | 30° | Single Transverse Mode | Ø5.6 mm |
DBR780PN | 780 nm | 45 mW | 250 mA | 1.9 V | - | - | Single Frequency | Butterfly, PM Pigtail |
L785P5 | 785 nm | 5 mW | 28 mA | 1.9 V | 10° | 29° | Single Transverse Mode | Ø5.6 mm |
LPS-PM785-FC | 785 nm | 6.5 mW | 60 mA | - | - | - | Single Transverse Mode | Ø5.6 mm, PM Pigtail |
LPS-785-FC | 785 nm | 10 mW | 65 mA | 1.85 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
LP785-SF20 | 785 nm | 20 mW | 85 mA | 1.9 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
DBR785S | 785 nm | 25 mW | 230 mA | 2.0 V | - | - | Single Frequency | Butterfly, SM Pigtail |
DBR785P | 785 nm | 25 mW | 230 mA | 2.0 V | - | - | Single Frequency | Butterfly, PM Pigtail |
L785P25 | 785 nm | 25 mW | 45 mA | 1.9 V | 8° | 30° | Single Transverse Mode | Ø5.6 mm |
FPV785S | 785 nm | 50 mW | 410 mA | 2.2 V | - | - | Single Frequency | Butterfly, SM Pigtail |
FPV785P | 785 nm | 50 mW | 410 mA | 2.1 V | - | - | Single Frequency | Butterfly, PM Pigtail |
LP785-SAV50 | 785 nm | 50 mW | 500 mA | 2.2 V | - | - | Single Frequency | Ø9 mm, SM Pigtail |
L785P090 | 785 nm | 90 mW | 125 mA | 2.0 V | 10° | 17° | Single Transverse Mode | Ø5.6 mm |
LP785-SF100 | 785 nm | 100 mW | 300 mA | 2.0 V | - | - | Single Transverse Mode | Ø9 mm, SM Pigtail |
FPL785P | 785 nm | 200 mW | 500 mA | 2.1 V | - | - | Single Transverse Mode | Butterfly, PM Pigtail |
FPL785S-250 | 785 nm | 250 mW (Min) | 500 mA | 2.0 V | - | - | Single Transverse Mode | Butterfly, SM Pigtail |
LD785-SEV300 | 785 nm | 300 mW | 500 mA (Max) | 2.0 V | 8° | 16° | Single Frequency | Ø9 mm |
LD785-SH300 | 785 nm | 300 mW | 400 mA | 2.0 V | 7° | 18° | Single Transverse Mode | Ø9 mm |
FPL785C | 785 nm | 300 mW | 400 mA | 2.0 V | 7° | 18° | Single Transverse Mode | 3 mm x 5 mm Submount |
LD785-SE400 | 785 nm | 400 mW | 550 mA | 2.0 V | 7° | 16° | Single Transverse Mode | Ø9 mm |
FPV785M | 785 nm | 600 mW | 1100 mA | 1.9 V | - | - | Multimode | Butterfly, MM Pigtail |
L795VH1 | 795 nm | 0.25 mW | 1.2 mA | 1.8 V | 20° | 12° | Single Frequency | TO-46 |
DBR795PN | 795 nm | 40 mW | 230 mA | 2.0 V | - | - | Single Frequency | Butterfly, PM Pigtail |
DBR808PN | 808 nm | 42 mW | 250 mA | 2 V | - | - | Single Frequency | Butterfly, PM Pigtail |
LP808-SA60 | 808 nm | 60 mW | 150 mA | 1.9 V | - | - | Single Transverse Mode | Ø9 mm, SM Pigtail |
M9-808-0150 | 808 nm | 150 mW | 180 mA | 1.9 V | 8° | 17° | Single Transverse Mode | Ø9 mm |
L808P200 | 808 nm | 200 mW | 260 mA | 2 V | 10° | 30° | Multimode | Ø5.6 mm |
FPL808P | 808 nm | 200 mW | 600 mA | 2.1 V | - | - | Single Transverse Mode | Butterfly, PM Pigtail |
FPL808S | 808 nm | 200 mW | 750 mA | 2.3 V | - | - | Single Transverse Mode | Butterfly, SM Pigtail |
L808H1 | 808 nm | 300 mW | 400 mA | 2.1 V | 14° | 6° | Single Transverse Mode | Ø9 mm |
LD808-SE500 | 808 nm | 500 mW | 750 mA | 2.2 V | 7° | 14° | Single Transverse Mode | Ø9 mm |
LD808-SEV500 | 808 nm | 500 mW | 800 mA (Max) | 2.2 V | 8° | 14° | Single Frequency | Ø9 mm |
L808P500MM | 808 nm | 500 mW | 650 mA | 1.8 V | 12° | 30° | Multimode | Ø5.6 mm |
L808P1000MM | 808 nm | 1000 mW | 1100 mA | 2 V | 9° | 30° | Multimode | Ø9 mm |
DBR816PN | 816 nm | 45 mW | 250 mA | 1.95 V | - | - | Single Frequency | Butterfly, PM Pigtail |
LP820-SF80 | 820 nm | 80 mW | 230 mA | 2.3 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
L820P100 | 820 nm | 100 mW | 145 mA | 2.1 V | 9° | 17° | Single Transverse Mode | Ø5.6 mm |
L820P200 | 820 nm | 200 mW | 250 mA | 2.4 V | 9° | 17° | Single Transverse Mode | Ø5.6 mm |
DBR828PN | 828 nm | 24 mW | 250 mA | 2.0 V | - | - | Single Frequency | Butterfly, PM Pigtail |
LPS-830-FC | 830 nm | 10 mW | 120 mA | - | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
LPS-PM830-FC | 830 nm | 10 mW | 50 mA | 2.0 V | - | - | Single Transverse Mode | Ø5.6 mm, PM Pigtail |
LP830-SF30 | 830 nm | 30 mW | 115 mA | 1.9 V | - | - | Single Transverse Mode | Ø9 mm, SM Pigtail |
HL8338MG | 830 nm | 50 mW | 75 mA | 1.9 V | 9° | 22° | Single Transverse Mode | Ø5.6 mm |
L830H1 | 830 nm | 250 mW | 3 A (Max) | 2 V | 8° | 10° | Single Transverse Mode | Ø9 mm |
FPL830P | 830 nm | 300 mW | 900 mA | 2.22 V | - | - | Single Transverse Mode | Butterfly, PM Pigtail |
FPL830S | 830 nm | 350 mW | 900 mA | 2.5 V | - | - | Single Transverse Mode | Butterfly, SM Pigtail |
LD830-SE650 | 830 nm | 650 mW | 900 mA | 2.3 V | 7° | 13° | Single Transverse Mode | Ø9 mm |
LD830-MA1W | 830 nm | 1 W | 2 A | 2.1 V | 7° | 24° | Multimode | Ø9 mm |
LD830-ME2W | 830 nm | 2 W | 3 A (Max) | 2.0 V | 8° | 21° | Multimode | Ø9 mm |
L840P200 | 840 nm | 200 mW | 255 mA | 2.4 V | 9 | 17 | Single Transverse Mode | Ø5.6 mm |
L850VH1 | 850 nm | 1 mW | 6 mA (Max) | 2 V | 12° | 12° | Single Frequency | TO-46 |
L850P010 | 850 nm | 10 mW | 50 mA | 2 V | 10° | 30° | Single Transverse Mode | Ø5.6 mm |
L850P030 | 850 nm | 30 mW | 65 mA | 2 V | 8.5° | 30° | Single Transverse Mode | Ø5.6 mm |
FPV852S | 852 nm | 20 mW | 400 mA | 2.2 V | - | - | Single Frequency | Butterfly, SM Pigtail |
FPV852P | 852 nm | 20 mW | 400 mA | 2.2 V | - | - | Single Frequency | Butterfly, PM Pigtail |
DBR852PN | 852 nm | 24 mW | 300 mA | 2.0 V | - | - | Single Frequency | Butterfly, PM Pigtail |
LP852-SF30 | 852 nm | 30 mW | 115 mA | 1.9 V | - | - | Single Transverse Mode | Ø9 mm, SM Pigtail |
L852P50 | 852 nm | 50 mW | 75 mA | 1.9 V | 9° | 22° | Single Transverse Mode | Ø5.6 mm |
LP852-SF60 | 852 nm | 60 mW | 150 mA | 2.0 V | - | - | Single Transverse Mode | Ø9 mm, SM Pigtail |
L852P100 | 852 nm | 100 mW | 120 mA | 1.9 V | 8° | 28° | Single Transverse Mode | Ø9 mm |
L852P150 | 852 nm | 150 mW | 170 mA | 1.9 V | 8° | 18° | Single Transverse Mode | Ø9 mm |
L852SEV1 | 852 nm | 270 mW | 400 mA (Max) | 2.0 V | 9° | 12° | Single Frequency | Ø9 mm |
L852H1 | 852 nm | 300 mW | 415 mA (Max) | 2 V | 7° | 15° | Single Transverse Mode | Ø9 mm |
FPL852P | 852 nm | 300 mW | 900 mA | 2.35 V | - | - | Single Transverse Mode | Butterfly, PM Pigtail |
FPL852S | 852 nm | 350 mW | 900 mA | 2.5 V | - | - | Single Transverse Mode | Butterfly, SM Pigtail |
LD852-SE600 | 852 nm | 600 mW | 950 mA | 2.3 V | 7° (1/e2) | 13° (1/e2) | Single Transverse Mode | Ø9 mm |
LD852-SEV600 | 852 nm | 600 mW | 1050 mA (Max) | 2.2 V | 8° | 13° (1/e2) | Single Frequency | Ø9 mm |
LP880-SF3 | 880 nm | 3 mW | 25 mA | 2.2 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
L880P010 | 880 nm | 10 mW | 30 mA | 2.0 V | 12° | 37° | Single Transverse Mode | Ø5.6 mm |
L895VH1 | 895 nm | 0.2 mW | 1.4 mA | 1.6 V | 20° | 13° | Single Frequency | TO-46 |
DBR895PN | 895 nm | 12 mW | 300 mA | 2 V | - | - | Single Frequency | Butterfly, PM Pigtail |
LP904-SF3 | 904 nm | 3 mW | 30 mA | 1.5 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
L904P010 | 904 nm | 10 mW | 50 mA | 2.0 V | 10° | 30° | Single Transverse Mode | Ø5.6 mm |
LP915-SF40 | 915 nm | 40 mW | 130 mA | 1.5 V | - | - | Single Transverse Mode | Ø9 mm, SM Pigtail |
DBR935PN | 935 nm | 13 mW | 300 mA | 1.75 V | - | - | Single Frequency | Butterfly, PM Pigtail |
LP940-SF30 | 940 nm | 30 mW | 90 mA | 1.5 V | - | - | Single Transverse Mode | Ø9 mm, SM Pigtail |
M9-940-0200 | 940 nm | 200 mW | 270 mA | 1.9 V | 8° | 28° | Single Transverse Mode | Ø9 mm |
L960H1 | 960 nm | 250 mW | 400 mA | 2.1 V | 11° | 12° | Single Transverse Mode | Ø9 mm |
FPV976S | 976 nm | 30 mW | 400 mA (Max) | 2.2 V | - | - | Single Frequency | Butterfly, SM Pigtail |
FPV976P | 976 nm | 30 mW | 400 mA (Max) | 2.2 V | - | - | Single Frequency | Butterfly, PM Pigtail |
DBR976PN | 976 nm | 33 mW | 450 mA | 2.0 V | - | - | Single Frequency | Butterfly, PM Pigtail |
L976SEV1 | 976 nm | 270 mW | 400 mA (Max) | 2.0 V | 9° | 12° | Single Frequency | Ø9 mm |
BL976-SAG3 | 976 nm | 300 mW | 470 mA | 2.0 V | - | - | Single Transverse Mode | Butterfly, SM Pigtail |
BL976-PAG500 | 976 nm | 500 mW | 830 mA | 2.0 V | - | - | Single Transverse Mode | Butterfly, PM Pigtail |
BL976-PAG700 | 976 nm | 700 mW | 1090 mA | 2.0 V | - | - | Single Transverse Mode | Butterfly, PM Pigtail |
BL976-PAG900 | 976 nm | 900 mW | 1480 mA | 2.5 V | - | - | Single Transverse Mode | Butterfly, PM Pigtail |
L980P010 | 980 nm | 10 mW | 25 mA | 2 V | 10° | 30° | Single Transverse Mode | Ø5.6 mm |
LP980-SF15 | 980 nm | 15 mW | 70 mA | 1.5 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
L980P030 | 980 nm | 30 mW | 50 mA | 1.5 V | 10° | 35° | Single Transverse Mode | Ø5.6 mm |
L980P100A | 980 nm | 100 mW | 150 mA | 1.6 V | 6° | 32° | Multimode | Ø5.6 mm |
LP980-SA60 | 980 nm | 60 mW | 230 mA | 2.0 V | - | - | Single Transverse Mode | Ø9.0 mm, SM Pigtail |
LP980-SA100 | 980 nm | 100 mW | 180 mA | 1.5 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
L980H1 | 980 nm | 200 mW | 300 mA (Max) | 2.0 V | 8° | 13° | Single Transverse Mode | Ø9 mm |
L980P200 | 980 nm | 200 mW | 300 mA | 1.5 V | 6° | 30° | Multimode | Ø5.6 mm |
DBR1060SN | 1060 nm | 130 mW | 650 mA | 2.0 V | - | - | Single Frequency | Butterfly, SM Pigtail |
DBR1060PN | 1060 nm | 130 mW | 650 mA | 1.8 V | - | - | Single Frequency | Butterfly, PM Pigtail |
DBR1064S | 1064 nm | 40 mW | 150 mA | 2.0 V | - | - | Single Frequency | Butterfly, SM Pigtail |
DBR1064P | 1064 nm | 40 mW | 150 mA | 2.0 V | - | - | Single Frequency | Butterfly, PM Pigtail |
DBR1064PN | 1064 nm | 110 mW | 550 mA | 2.0 V | - | - | Single Frequency | Butterfly, PM Pigtail |
LPS-1060-FC | 1064 nm | 50 mW | 220 mA | 1.4 V | - | - | Single Transverse Mode | Ø9 mm, SM Pigtail |
M9-A64-0200 | 1064 nm | 200 mW | 280 mA | 1.7 V | 8° | 28° | Single Transverse Mode | Ø9 mm |
L1064H1 | 1064 nm | 300 mW | 700 mA | 1.92 V | 7.6° | 13.5° | Single Transverse Mode | Ø9 mm |
L1064H2 | 1064 nm | 450 mW | 1100 mA | 1.92 V | 7.6° | 13.5° | Single Transverse Mode | Ø9 mm |
DBR1083PN | 1083 nm | 100 mW | 500 mA | 1.75 V | - | - | Single Frequency | Butterfly, PM Pigtail |
L1270P5DFB | 1270 nm | 5 mW | 15 mA | 1.1 V | 7° | 9° | Single Frequency | Ø5.6 mm |
L1290P5DFB | 1290 nm | 5 mW | 16 mA | 1.0 V | 7° | 9° | Single Frequency | Ø5.6 mm |
LP1310-SAD2 | 1310 nm | 2.0 mW | 40 mA | 1.1 V | - | - | Single Frequency | Ø5.6 mm, SM Pigtail |
LP1310-PAD2 | 1310 nm | 2.0 mW | 40 mA | 1.0 V | - | - | Single Frequency | Ø5.6 mm, PM Pigtail |
LPS-PM1310-FC | 1310 nm | 2.5 mW | 20 mA | 1.1 V | - | - | Single Transverse Mode | Ø5.6 mm, PM Pigtail |
L1310P5DFB | 1310 nm | 5 mW | 16 mA | 1.0 V | 7° | 9° | Single Frequency | Ø5.6 mm |
ML725B8F | 1310 nm | 5 mW | 20 mA | 1.1 V | 25° | 30° | Single Transverse Mode | Ø5.6 mm |
LPSC-1310-FC | 1310 nm | 50 mW | 350 mA | 2 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
FPL1053S | 1310 nm | 130 mW | 400 mA | 1.7 V | - | - | Single Transverse Mode | Butterfly, SM Pigtail |
FPL1053P | 1310 nm | 130 mW | 400 mA | 1.7 V | - | - | Single Transverse Mode | Butterfly, PM Pigtail |
FPL1053T | 1310 nm | 300 mW (Pulsed) | 750 mA | 2 V | 15° | 28° | Single Transverse Mode | Ø5.6 mm |
FPL1053C | 1310 nm | 300 mW (Pulsed) | 750 mA | 2 V | 15° | 27° | Single Transverse Mode | Chip on Submount |
L1310G1 | 1310 nm | 2000 mW | 5 A | 1.5 V | 7° | 24° | Multimode | Ø9 mm |
L1330P5DFB | 1330 nm | 5 mW | 14 mA | 1.0 V | 7° | 9° | Single Frequency | Ø5.6 mm |
L1370G1 | 1370 nm | 2000 mW | 5 A | 1.4 V | 6° | 22° | Multimode | Ø9 mm |
BL1425-PAG500 | 1425 nm | 500 mW | 1600 mA | 2.0 V | - | - | Single Transverse Mode | Butterfly, PM Pigtail |
BL1436-PAG500 | 1436 nm | 500 mW | 1600 mA | 2.0 V | - | - | Single Transverse Mode | Butterfly, PM Pigtail |
L1450G1 | 1450 nm | 2000 mW | 5 A | 1.4 V | 7° | 22° | Multimode | Ø9 mm |
BL1456-PAG500 | 1456 nm | 500 mW | 1600 mA | 2.0 V | - | - | Single Transverse Mode | Butterfly, PM Pigtail |
L1470P5DFB | 1470 nm | 5 mW | 19 mA | 1.0 V | 7° | 9° | Single Frequency | Ø5.6 mm |
L1480G1 | 1480 nm | 2000 mW | 5 A | 1.6 V | 6° | 20° | Multimode | Ø9 mm |
L1490P5DFB | 1490 nm | 5 mW | 24 mA | 1.0 V | 7° | 9° | Single Frequency | Ø5.6 mm |
L1510P5DFB | 1510 nm | 5 mW | 20 mA | 1.0 V | 7° | 9° | Single Frequency | Ø5.6 mm |
L1530P5DFB | 1530 nm | 5 mW | 21 mA | 1.0 V | 7° | 9° | Single Frequency | Ø5.6 mm |
LPS-1550-FC | 1550 nm | 1.5 mW | 30 mA | 1.0 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
LPS-PM1550-FC | 1550 nm | 1.5 mW | 30 mA | 1.1 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
LP1550-SAD2 | 1550 nm | 2.0 mW | 40 mA | 1.0 V | - | - | Single Frequency | Ø5.6 mm, SM Pigtail |
LP1550-PAD2 | 1550 nm | 2.0 mW | 40 mA | 1.0 V | - | - | Single Frequency | Ø5.6 mm, PM Pigtail |
L1550P5DFB | 1550 nm | 5 mW | 20 mA | 1.0 V | 8° | 10° | Single Frequency | Ø5.6 mm |
ML925B45F | 1550 nm | 5 mW | 30 mA | 1.1 V | 25° | 30° | Single Transverse Mode | Ø5.6 mm |
SFL1550S | 1550 nm | 40 mW | 300 mA | 1.5 V | - | - | Single Frequency | Butterfly, SM Pigtail |
SFL1550P | 1550 nm | 40 mW | 300 mA | 1.5 V | - | - | Single Frequency | Butterfly, PM Pigtail |
LPSC-1550-FC | 1550 nm | 50 mW | 250 mA | 2 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
FPL1009S | 1550 nm | 100 mW | 400 mA | 1.4 V | - | - | Single Transverse Mode | Butterfly, SM Pigtail |
FPL1009P | 1550 nm | 100 mW | 400 mA | 1.4 V | - | - | Single Transverse Mode | Butterfly, PM Pigtail |
ULN15PC | 1550 nm | 140 mW | 650 mA | 3.0 V | - | - | Single Frequency | Extended Butterfly, PM Pigtail |
ULN15PT | 1550 nm | 140 mW | 650 mA | 3.0 V | - | - | Single Frequency | Extended Butterfly, PM Pigtail |
FPL1001C | 1550 nm | 150 mW | 400 mA | 1.4 V | 18° | 31° | Single Transverse Mode | Chip on Submount |
FPL1055T | 1550 nm | 300 mW (Pulsed) | 750 mA | 2 V | 15° | 28° | Single Transverse Mode | Ø5.6 mm |
FPL1055C | 1550 nm | 300 mW (Pulsed) | 750 mA | 2 V | 15° | 28° | Single Transverse Mode | Chip on Submount |
L1550G1 | 1550 nm | 1700 mW | 5 A | 1.5 V | 7° | 28° | Multimode | Ø9 mm |
DFB1550 | 1555 nm | 100 mW (Min) | 1000 mA (Max) | 3.0 V | - | - | Single Frequency | Butterfly, SM Pigtail |
DFB1550N | 1555 nm | 130 mW (Min) | 1800 mA (Max) | 3.0 V | - | - | Single Frequency | Butterfly, SM Pigtail |
DFB1550P | 1555 nm | 100 mW (Min) | 1000 mA (Max) | 3.0 V | - | - | Single Frequency | Butterfly, PM Pigtail |
DFB1550PN | 1555 nm | 130 mW (Min) | 1800 mA (Max) | 3.0 V | - | - | Single Frequency | Butterfly, PM Pigtail |
L1570P5DFB | 1570 nm | 5 mW | 25 mA | 1.0 V | 7° | 9° | Single Frequency | Ø5.6 mm |
L1575G1 | 1575 nm | 1700 mW | 5 A | 1.5 V | 6° | 28° | Multimode | Ø9 mm |
LPSC-1625-FC | 1625 nm | 50 mW | 350 mA | 1.5 V | - | - | Single Transverse Mode | Ø5.6 mm, SM Pigtail |
FPL1054S | 1625 nm | 80 mW | 400 mA | 1.7 V | - | - | Single Transverse Mode | Butterfly, SM Pigtail |
FPL1054P | 1625 nm | 80 mW | 400 mA | 1.7 V | - | - | Single Transverse Mode | Butterfly, PM Pigtail |
FPL1054C | 1625 nm | 250 mW (Pulsed) | 750 mA | 2 V | 15° | 28° | Single Transverse Mode | Chip on Submount |
FPL1054T | 1625 nm | 200 mW (Pulsed) | 750 mA | 2 V | 15° | 28° | Single Transverse Mode | Ø5.6 mm |
DFB1642 | 1642 nm | 80 mW | 900 mA (Max) | 3.0 V | - | - | Single Frequency | Butterfly, SM Pigtail |
DFB1642P | 1642 nm | 80 mW | 900 mA (Max) | 3.0 V | - | - | Single Frequency | Butterfly, PM Pigtail |
DFB1646 | 1646 nm | 80 mW | 900 mA (Max) | 3.0 V | - | - | Single Frequency | Butterfly, SM Pigtail |
DFB1646P | 1646 nm | 80 mW | 900 mA (Max) | 3.0 V | - | - | Single Frequency | Butterfly, PM Pigtail |
FPL1059S | 1650 nm | 80 mW | 400 mA | 1.7 V | - | - | Single Transverse Mode | Butterfly, SM Pigtail |
FPL1059P | 1650 nm | 80 mW | 400 mA | 1.7 V | - | - | Single Transverse Mode | Butterfly, PM Pigtail |
DFB1650 | 1650 nm | 80 mW | 900 mA (Max) | 3.0 V | - | - | Single Frequency | Butterfly, SM Pigtail |
DFB1650P | 1650 nm | 80 mW | 900 mA (Max) | 3.0 V | - | - | Single Frequency | Butterfly, PM Pigtail |
FPL1059C | 1650 nm | 225 mW (Pulsed) | 750 mA | 2 V | 15° | 28° | Single Transverse Mode | Chip on Submount |
FPL1059T | 1650 nm | 225 mW (Pulsed) | 750 mA | 2 V | 15° | 28° | Single Transverse Mode | Ø5.6 mm |
DFB1654 | 1654 nm | 80 mW | 900 mA (Max) | 3.0 V | - | - | Single Frequency | Butterfly, SM Pigtail |
DFB1654P | 1654 nm | 80 mW | 900 mA (Max) | 3.0 V | - | - | Single Frequency | Butterfly, PM Pigtail |
FPL1940S | 1940 nm | 15 mW | 400 mA | 2 V | - | - | Single Transverse Mode | Butterfly, SM Pigtail |
FPL2000S | 2 µm | 15 mW | 400 mA | 2 V | - | - | Single Transverse Mode | Butterfly, SM Pigtail |
FPL2000C | 2 µm | 30 mW | 400 mA | 5.2 V | 8° | 19° | Single Transverse Mode | Chip on Submount |
ID3250HHLH | 3.00 - 3.50 µm (DFB) | 5 mW | 400 mA (Max) | 5 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
IF3400T1 | 3.40 µm (FP) | 30 mW | 300 mA | 4 V | 40° | 70° | Single Transverse Mode | Ø9 mm |
ID3750HHLH | 3.50 - 4.00 µm (DFB) | 5 mW | 300 mA (Max) | 5 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QF3850T1 | 3.85 µm (FP) | 200 mW | 600 mA (Max) | 13.5 V | 30° | 40° | Single Transverse Mode | Ø9 mm |
QF3850HHLH | 3.85 µm (FP) | 320 mW (Min) | 1100 mA (Max) | 13 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Transverse Mode | Horizontal HHL |
QF4040HHLH | 4.05 µm (FP) | 320 mW (Min) | 1100 mA (Max) | 13 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Transverse Mode | Horizontal HHL |
QD4500CM1 | 4.00 - 5.00 µm (DFB) | 40 mW | 500 mA (Max) | 10.5 V | 30° | 40° | Single Frequency | Two-Tab C-Mount |
QD4500HHLH | 4.00 - 5.00 µm (DFB) | 80 mW | 500 mA (Max) | 11 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QF4050T2 | 4.05 µm (FP) | 70 mW | 250 mA | 12 V | 30° | 40° | Single Transverse Mode | Ø9 mm |
QF4050C2 | 4.05 µm (FP) | 300 mW | 400 mA | 12 V | 30 | 42 | Single Transverse Mode | Two-Tab C-Mount |
QF4050T1 | 4.05 µm (FP) | 300 mW | 600 mA (Max) | 12.0 V | 30° | 40° | Single Transverse Mode | Ø9 mm |
QF4050D2 | 4.05 µm (FP) | 800 mW | 750 mA | 13 V | 30° | 40° | Single Transverse Mode | D-Mount |
QF4050D3 | 4.05 µm (FP) | 1200 mW | 1000 mA | 13 V | 30° | 40° | Single Transverse Mode | D-Mount |
QD4472HH | 4.472 µm (DFB) | 85 mW | 500 mA (Max) | 11 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QF4600T2 | 4.60 µm (FP) | 200 mW | 500 mA (Max) | 13.0 V | 30° | 40° | Single Transverse Mode | Ø9 mm |
QF4600T1 | 4.60 µm (FP) | 400 mW | 800 mA (Max) | 12.0 V | 30° | 40° | Single Transverse Mode | Ø9 mm |
QF4600C2 | 4.60 µm (FP) | 600 mW | 600 mA | 12 V | 30° | 42° | Single Transverse Mode | Two-Tab C-Mount |
QF4600T3 | 4.60 µm (FP) | 1000 mW | 800 mA (Max) | 13 V | 30° | 40° | Single Transverse Mode | Ø9 mm |
QF4600D4 | 4.60 µm (FP) | 2500 mW | 1800 mA | 12.5 V | 40° | 30° | Single Transverse Mode | D-Mount |
QF4600D3 | 4.60 µm (FP) | 3000 mW | 1700 mA | 12.5 V | 30° | 40° | Single Transverse Mode | D-Mount |
QD4602HH | 4.602 µm (DFB) | 150 mW | 1000 mA (Max) | 12 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QF4650HHLH | 4.65 µm (FP) | 1500 mW (Min) | 1100 mA | 12 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Transverse Mode | Horizontal HHL |
QD5500CM1 | 5.00 - 6.00 µm (DFB) | 40 mW | 700 mA (Max) | 9.5 V | 30° | 45° | Single Frequency | Two-Tab C-Mount |
QD5500HHLH | 5.00 - 6.00 µm (DFB) | 150 mW | 500 mA (Max) | 11 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QD5250C2 | 5.20 - 5.30 µm (DFB) | 60 mW | 700 mA (Max) | 9.5 V | 30° | 45° | Single Frequency | Two-Tab C-Mount |
QD5263HH | 5.263 µm (DFB) | 130 mW | 1000 mA (Max) | 12 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QD6500CM1 | 6.00 - 7.00 µm (DFB) | 40 mW | 650 mA (Max) | 10 V | 35° | 50° | Single Frequency | Two-Tab C-Mount |
QD6500HHLH | 6.00 - 7.00 µm (DFB) | 80 mW | 600 mA (Max) | 11 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QD6134HH | 6.134 µm (DFB) | 50 mW | 1000 mA (Max) | 12 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QD7500CM1 | 7.00 - 8.00 µm (DFB) | 40 mW | 600 mA (Max) | 10 V | 40° | 50° | Single Frequency | Two-Tab C-Mount |
QD7500HHLH | 7.00 - 8.00 µm (DFB) | 50 mW | 700 mA (Max) | 12 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QD7500DM1 | 7.00 - 8.00 µm (DFB) | 100 mW | 600 mA (Max) | 11.5 V | 40° | 55° | Single Frequency | D-Mount |
QD7416HH | 7.416 µm (DFB) | 100 mW | 1000 mA (Max) | 12 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QD7716HH | 7.716 µm (DFB) | 30 mW | 1000 mA (Max) | 12 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QF7900HB | 7.9 µm (FP) | 700 mW | 1600 mA (Max) | 9 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Transverse Mode | Horizontal HHL |
QD7901HH | 7.901 µm (DFB) | 50 mW | 700 mA (Max) | 10 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QD8050CM1 | 8.00 - 8.10 µm (DFB) | 100 mW | 1000 mA (Max) | 9.5 V | 55° | 70° | Single Frequency | Two-Tab C-Mount |
QD8500CM1 | 8.00 - 9.00 µm (DFB) | 100 mW | 900 mA (Max) | 9.5 V | 40° | 55° | Single Frequency | Two-Tab C-Mount |
QD8500HHLH | 8.00 - 9.00 µm (DFB) | 100 mW | 600 mA (Max) | 10.2 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QF8450C2 | 8.45 µm (FP) | 300 mW | 750 mA | 9 V | 40° | 60° | Single Transverse Mode | Two-Tab C-Mount |
QF8500HB | 8.5 µm (FP) | 500 mW | 2000 mA (Max) | 9 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Transverse Mode | Horizontal HHL |
QD8650CM1 | 8.60 - 8.70 µm (DFB) | 50 mW | 900 mA (Max) | 9.5 V | 55° | 70° | Single Frequency | Two-Tab C-Mount |
QD8912HH | 8.912 µm (DFB) | 150 mW | 1000 mA (Max) | 12 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QD9500CM1 | 9.00 - 10.00 µm (DFB) | 60 mW | 800 mA (Max) | 9.5 V | 40° | 55° | Single Frequency | Two-Tab C-Mount |
QD9500HHLH | 9.00 - 10.00 µm (DFB) | 100 mW | 600 mA (Max) | 10.2 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QD9062HH | 9.062 µm (DFB) | 130 mW | 1000 mA (Max) | 12 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QF9150C2 | 9.15 µm (FP) | 200 mW | 850 mA | 11 V | 40° | 60° | Single Transverse Mode | Two-Tab C-Mount |
QF9200HB | 9.2 µm (FP) | 250 mW | 2000 mA (Max) | 9 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Transverse Mode | Horizontal HHL |
QF9500T1 | 9.5 µm (FP) | 300 mW | 550 mA | 12 V | 40° | 55° | Single Transverse Mode | Ø9 mm |
QD9550C2 | 9.50 - 9.60 µm (DFB) | 60 mW | 800 mA (Max) | 9.5 V | 40° | 55° | Single Frequency | Two-Tab C-Mount |
QF9550CM1 | 9.55 µm (FP) | 80 mW | 1500 mA | 7.8 V | 35° | 60° | Single Transverse Mode | Two-Tab C-Mount |
QD9697HH | 9.697 µm (DFB) | 80 mW | 1000 mA (Max) | 12 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QD10500CM1 | 10.00 - 11.00 µm (DFB) | 40 mW | 600 mA (Max) | 10 V | 40° | 55° | Single Frequency | Two-Tab C-Mount |
QD10500HHLH | 10.00 - 11.00 µm (DFB) | 50 mW | 700 mA (Max) | 12 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QD10530HH | 10.530 µm (DFB) | 50 mW | 1000 mA (Max) | 12 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QD10549HH | 10.549 µm (DFB) | 60 mW | 1000 mA (Max) | 12 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
QD10622HH | 10.622 µm (DFB) | 60 mW | 1000 mA (Max) | 12 V | 6 mrad (0.34°) | 6 mrad (0.34°) | Single Frequency | Horizontal HHL |
The rows shaded green above denote single-frequency lasers. |
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