Volume-Holographic-Grating- (VHG) Stabilized SF Lasers, TO Cans
![](https://www.thorlabs.de/Images/GuideImages/13676_VHGLaserDiodeTOCan_1.jpg )
- 785 nm, 808 nm, 852 nm, or 976 nm VHG-Stabilized Laser Diodes
- Wavelength-Stabilized Output Over Operating Temperature Range
- Ø9 mm TO Can Package
LD785-SEV300
785 nm, 300 mW, Ø9 mm TO Can
This high-resolution optical spectrum was obtained using one of Thorlabs’ Optical Spectrum Analyzers (OSA201C), which provides 8 pm resolution at 785 nm.
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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
- 785 nm, 808 nm, 852 nm, or 976 nm Center Wavelength
- Wavelength-Stabilized Output
- Ø9 mm TO Can Package
Applications
- Raman Spectroscopy
- Microscopy
Thorlabs' Volume-Holographic-Grating- (VHG) Stabilized Lasers are laser diodes that use feedback from a volume holographic grating to provide narrow-linewidth, single-frequency operation. This allows the laser to achieve 10 MHz typical linewidths for Item #s LD785-SEV300, LD808-SEV500, and LD852-SEV600, and excellent side mode suppression ratios (typically 40 dB or higher) for all of the VHG stabilized laser diodes on this page. Typical performance graphs can be viewed by clicking on the blue icons () in the tables below. More information on the stabilized temperature range can be found on the individualized data sheet for each laser diode.
These VHG-stabilized lasers are housed in compact Ø9 mm TO can packages with E pin codes. As they do not contain internal isolators, we recommend using an NIR Optical Isolator when the output is collimated. Single-frequency performance is only guaranteed with >35 dB isolation from back reflections. We also offer VHG lasers in butterfly packages and a 785 nm laser in an SM fiber pigtail package with an FC/APC connector (Item # LP785-SAV50).
While a center wavelength is listed for each laser diode below, this is only a typical number. The center wavelength of a particular unit varies from production run to production run, so the diode you receive may not operate at the typical center wavelength. After clicking "Choose Item" below, a list will appear that contains the center wavelength, output power, and operating current of each in-stock unit. Clicking on the red Docs Icon next to the serial number provides access to a PDF with serial-number-specific L-I-V and spectral characteristics.
Laser diodes are sensitive to electrostatic shock. Please take the proper precautions when handling the device, such as using an ESD wrist strap.
Thorlabs also offers pigtailed volume-holographic-grating-stabilized and distributed feedback (DFB) single-frequency lasers and external cavity and distributed bragg reflector (DBR) butterfly-packaged single-frequency lasers. The DFB lasers provide similar linewidths to the VHG-stabilized lasers, but provide mode-hop free tuning of several nanometers while maintaining single-frequency operation. Our DBR single-frequency lasers offer a similar linewidth to the VHG-stabilized lasers, but have a temperature- and current-tunable center wavelength. A description of the differences between each type of laser is provided on the SFL Guide tab.
Video Insight: Setting Up a TO Can Laser Diode
Installing a TO can laser diode in a mount and setting it up to run under temperature and current control presents many opportunities to make a mistake that could damage or destroy the laser. This step-by-step guide includes tips for keeping humans and laser diodes safe from harm.
When operated within their specifications, laser diodes have extremely long lifetimes. Most failures occur from mishandling or operating the lasers beyond their maximum ratings. Laser diodes are among the most static-sensitive devices currently made and proper ESD protection should be worn whenever handling a laser diode. Due to their extreme electrostatic sensitivity, laser diodes cannot be returned after their sealed package has been opened. Laser diodes in their original sealed package can be returned for a full refund or credit.
Handling and Storage Precautions
Because of their extreme susceptibility to damage from electrostatic discharge (ESD), care should be taken whenever handling and operating laser diodes.
Wrist Straps
Use grounded anti-static wrist straps whenever handling diodes.
Anti-Static Mats
Always work on grounded anti-static mats.
Laser Diode Storage
When not in use, short the leads of the laser together to protect against ESD damage.
Operating and Safety Precautions
Use an Appropriate Driver
Laser diodes require precise control of operating current and voltage to avoid overdriving the laser. In addition, the laser driver should provide protection against power supply transients. Select a laser driver appropriate for your application. Do not use a voltage supply with a current-limiting resistor since it does not provide sufficient regulation to protect the laser diode.
Power Meters
When setting up and calibrating a laser diode with its driver, use a NIST-traceable power meter to precisely measure the laser output. It is usually safest to measure the laser diode output directly before placing the laser in an optical system. If this is not possible, be sure to take all optical losses (transmissive, aperture stopping, etc.) into consideration when determining the total output of the laser.
Reflections
Flat surfaces in the optical system in front of a laser diode can cause some of the laser energy to reflect back onto the laser’s monitor photodiode, giving an erroneously high photodiode current. If optical components are moved within the system and energy is no longer reflected onto the monitor photodiode, a constant-power feedback loop will sense the drop in photodiode current and try to compensate by increasing the laser drive current and possibly overdriving the laser. Back reflections can also cause other malfunctions or damage to laser diodes. To avoid this, be sure that all surfaces are angled 5-10°, and when necessary, use optical isolators to attenuate direct feedback into the laser.
Heat Sinks
Laser diode lifetime is inversely proportional to operating temperature. Always mount the laser diode in a suitable heat sink to remove excess heat from the laser package.
Voltage and Current Overdrive
Be careful not to exceed the maximum voltage and drive current listed on the specification sheet with each laser diode, even momentarily. Also, reverse voltages as little as 3 V can damage a laser diode.
ESD-Sensitive Device
Laser diodes are susceptible to ESD damage even during operation. This is particularly aggravated by using long interface cables between the laser diode and its driver due to the inductance that the cable presents. Avoid exposing the laser diode or its mounting apparatus to ESD at all times.
ON/OFF and Power-Supply-Coupled Transients
Due to their fast response times, laser diodes can be easily damaged by transients less than 1 µs. High-current devices such as soldering irons, vacuum pumps, and fluorescent lamps can cause large momentary transients, and thus surge-protected outlets should always be used when working with laser diodes.
If you have any questions regarding laser diodes, please contact Thorlabs Technical Support for assistance.
ECL, DFB, VHG-Stabilized, and DBR Single-Frequency Lasers
![ECL Laser Diagram](https://www.thorlabs.de/images/tabimages/External_Cavity_Laser_0114_300.gif)
Click to Enlarge
Figure 1: ECL Lasers have a Grating Outside of the Gain Chip
A wide variety of applications require tunable single-frequency operation of a laser system. In the world of diode lasers, there are currently four main configurations to obtain a single-frequency output: external cavity laser (ECL), distributed feedback (DFB), volume holographic grating (VHG), and distributed Bragg reflector (DBR). All four are capable of single-frequency output through the utilization of grating feedback. However, each type of laser uses a different grating feedback configuration, which influences performance characteristics such as output power, tuning range, and side mode suppression ratio (SMSR). We discuss below some of the main differences between these four types of single-frequency diode lasers.
External Cavity Laser
The External Cavity Laser (ECL) is a versatile configuration that is compatible with most standard free space diode lasers. This means that the ECL can be used at a variety of wavelengths, dependent upon the internal laser diode gain element. A lens collimates the output of the diode, which is then incident upon a grating (see Figure 1). The grating provides optical feedback and is used to select the stabilized output wavelength. With proper optical design, the external cavity allows only a single longitudinal mode to lase, providing single-frequency laser output with high side mode suppression ratio (SMSR > 45 dB).
One of the main advantages of the ECL is that the relatively long cavity provides extremely narrow linewidths (several hundred kHz). Additionally, since it can incorporate a variety of laser diodes, it remains one of the few configurations that can provide narrow linewidth emission at blue or red wavelengths. The ECL can have a large tuning range (>100 nm) but is often prone to mode hops, which are very dependent on the ECL's mechanical design as well as the quality of the antireflection (AR) coating on the laser diode.
![DBR Laser Diagram](https://www.thorlabs.de/images/tabimages/DBFvsDBR_dwg_DBF-300.gif)
Click to Enlarge
Figure 2: DFB Lasers Have a Bragg Reflector Along the Length of the Active Gain Medium
Distributed Feedback Laser
The Distributed Feedback (DFB) Laser (available in NIR with TO can, pigtailed TO can, and butterfly packaging, and MIR with two-tab C-mount, D-mount, and HHL packaging) incorporates the grating within the laser diode structure itself (see Figure 2). This corrugated periodic structure coupled closely to the active region acts as a Bragg reflector, selecting a single longitudinal mode as the lasing mode. If the active region has enough gain at frequencies near the Bragg frequency, an end reflector is unnecessary, relying instead upon the Bragg reflector for all optical feedback and mode selection. Due to this “built-in” selection, a DFB can achieve single-frequency operation over broad temperature and current ranges. To aid in mode selection and improve manufacturing yield, DFB lasers often utilize a phase shift section within the diode structure as well.
The lasing wavelength for a DFB is approximately equal to the Bragg wavelength:
where λ is the wavelength, neff is the effective refractive index, and Λ is the grating period. By changing the effective index, the lasing wavelength can be tuned. This is accomplished through temperature and current tuning of the DFB.
The DFB has a relatively narrow tuning range: about 2 nm at 850 nm, about 4 nm at 1550 nm, or at least 1 cm-1 in the mid-IR (4.00 - 11.00 µm). However, over this tuning range, the DFB can achieve single-frequency operation, which means that this is a continuous tuning range without mode hops. Because of this feature, DFBs have become a popular and majority choice for real-world applications such as telecom and sensors. Since the cavity length of a DFB is rather short, the linewidths are typically from several hundred kHz to 10 MHz. Additionally, the close coupling between the grating structure and the active region results in lower maximum output power compared to ECL and DBR lasers.
![DBR Laser Diagram](https://www.thorlabs.de/images/tabimages/VHG_Laser_Diode_300.gif)
Click to Enlarge
Figure 3: VHG Lasers have a Volume Holographic Grating Outside of the Active Gain Medium
Volume-Holographic-Grating-Stabilized Laser
A Volume-Holographic-Grating-(VHG)-Stabilized Laser also uses a Bragg reflector, but in this case a transmission grating is placed in front of the laser diode output (see Figure 3). Since the grating is not part of the laser diode structure, it can be thermally decoupled from the laser diode, improving the wavelength stability of the device. The grating typically consists of a piece of photorefractive material (typically glass) which has a periodic variation in the index of refraction. Only the wavelength of light that satisfies the Bragg condition for the grating is reflected back into the laser cavity, which results in a laser with extremely wavelength-stable emission. A VHG-Stabilized laser can produce output with a similar linewidth to a DFB laser at higher powers that is wavelength-locked over a wide range of currents and temperatures.
![DBR Laser Diagram](https://www.thorlabs.de/images/tabimages/DBFvsDBR_dwg_DBR-300.gif)
Click to Enlarge
Figure 4: DBR Lasers have a Bragg Reflector Outside of the Active Gain Medium
Distributed Bragg Reflector Laser
Similar to DFBs, Distributed Bragg Reflector (DBR) lasers incorporate an internal grating structure. However, whereas DFB lasers incorporate the grating structure continuously along the active region (gain region), DBR lasers place the grating structure(s) outside this region (see Figure 4). In general a DBR can incorporate various regions not typically found in a DFB that yield greater control and tuning range. For instance, a multiple-electrode DBR laser can include a phase-controlled region that allows the user to independently tune the phase apart from the grating period and laser diode current. When utilized together, the DBR can provide single-frequency operation over a broad tuning range. For example, high end sample-grating DBR lasers can have a tuning range as large as 30 - 40 nm. Unlike the DFB, the output is not mode hop free; hence, careful control of all inputs and temperature must be maintained.
In contrast to the complicated control structure for the multiple-electrode DBR, a simplified version of the DBR is engineered with just one electrode. This single-electrode DBR eliminates the complications of grating and phase control at the cost of tuning range. For this architecture type, the tuning range is similar to a DFB laser but will mode hop as a function of the applied current and temperature. Despite the disadvantage of mode hops, the single-electrode DBR does provide some advantages over its DFB cousin, namely higher output power because the grating is not continuous along the length of the device. Both DBR and DFB lasers have similar laser linewidths. Currently, Thorlabs offers only single-electrode DBR lasers.
Ultra-Low-Noise Hybrid Laser
Thorlabs Ultra-Low-Noise (ULN) Hybrid Lasers each consist of a single angled facet (SAF) gain chip coupled to an exceptionally long fiber Bragg grating (FBG). They are designed to create a laser cavity, similar to an ECL, through the length of fiber. This cavity provides the ULN hybrid laser with a very narrow line width on the order of 100 Hz and low relative intensity noise of -165 dBc/Hz (typical). The FBG reflects a portion of the light emitted from the gain medium while remaining thermally isolated from it. The grating period can be changed by introducing thermal stress to the fiber, allowing users to temperature tune the laser output while being able to independently stabilize the gain medium's temperature. Because the laser's configuration provides excellent low-noise performance, it is likely the laser will not be the limiting factor at low-noise levels. It is critical to monitor the laser's environment to limit external noise contributions like acoustic and seismic vibrations, as well as driving the laser with a low-noise current source.
![Hybrid Laser Diagram](https://www.thorlabs.de/images/tabimages/Hybrid_Laser_Diode_D1-300.gif)
Click to Enlarge
Figure 5: Thorlabs Hybrid Lasers have a Fiber Bragg Grating Coupled to the Active Gain Medium
Conclusion
ECL, DFB, VHG, and DBR laser diodes provide single-frequency operation over their designed tuning range. The ECL can be designed for a larger selection of wavelengths than either the DFB or DBR. While prone to mode hops, it also provides the narrowest linewidth (several hundred kHz) of the three choices. In appropriately designed instruments, ECLs can also provide extremely broad tuning ranges (>100 nm).
The DFB laser is the most stable single-frequency, tunable laser of the four. It can provide mode-hop-free performance over its entire tuning range (<5 nm), making it one of the most popular forms of single-frequency laser for much of industry. It often has low output power due to inherent properties of the continuous grating feedback structure, but higher powers can be achieved with different packaging styles.
The VHG laser provides the most stable wavelength performance over a range of temperatures and currents and can provide higher powers than are typical in DFB lasers. This stability makes it excellent for use in OEM applications.
The single-electrode DBR laser provides similar linewidth and tuning range as the DFB (<5 nm). However, the single-electrode DBR will have periodic mode hops in its tuning curve.
Hybrid lasers can be used to achieve extremely low-noise signals. In order to take advantage of this characteristic, the laser must be isolated from unwanted noise sources, such as acoustic and seismic vibrations and drive current noise.
Posted Comments: | |
Stefan Englbrecht
 (posted 2024-06-25 10:21:53.313) Hello,
Please let me know the line width and wavelenght stability of this diode (nm/°C)
Thank you!
best regards
Stefan cdolbashian
 (posted 2024-07-01 04:43:57.0) Thank you for reaching out to us with this inquiry. The example temperature tuning can be see with the additional specs, but clicking the blue "i" icon on the product page. Serialized tuning data is shipped with the product. Regarding linewidth, we would expect ~15MHz. |
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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Item # | Info | Wavelength | Power (Typical)a |
Operating Current (Max)a,b |
Pin Code |
Package | Built-In Isolator |
Compatible Socket |
Wavelength Tested |
Laser Mode |
Recommended | |
---|---|---|---|---|---|---|---|---|---|---|---|---|
Mount | Driver | |||||||||||
L852SEV1c | ![]() |
852 nm | 270 mW | 400 mA | E | Ø9 mm TO Cand | No | S8060 or S8060-4 |
Yes | Single Frequencye |
LDM90(/M) | ITC4001f |
LD852-SEV600c | ![]() |
852 nm | 600 mW | 1050 mA | E | Ø9 mm TO Cand | No | S8060 or S8060-4 |
Yes | Single Frequencye |
LDM90(/M) | ITC4001f |