Visible Laser Diodes: Center Wavelengths from 404 nm to 690 nm


  • Output Powers Up to 1600 mW
  • Multiple Package Styles
  • In-House Manufactured and Third-Party Options Available

Ø9 mm

Ø5.6 mm

Pigtailed Laser Diode, PM Fiber

Application Idea

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LD Controller, TEC Controller,
LD/TEC Mount, and Accessories

Pigtailed Laser Diode, SM Fiber with Collimated Output

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Laser Diode Selection Guidea
Shop by Wavelength
UV (375 nm)
Visible (404 nm - 690 nm)
NIR (705 nm - 2000 nm)
MIR (4.05 µm - 11.00 µm)
Shop by Package / Type
  • Our complete selection of laser diodes is available on the LD Selection Guide tab above.

Webpage Features
info icon Clicking this icon opens a window that contains specifications and mechanical drawings.
info icon 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.
Contact ThorlabsLaser Diode Tutorial

Features

  • Output Powers from 1 mW to 1600 mW
  • Center Wavelengths Available from 404 nm to 690 nm
  • Various Packages Available: TO Can and TO Pigtails
  • Compatible with Thorlabs' Laser Diode and TEC Controllers

This webpage contains Thorlabs' laser diodes with center wavelengths from 404 nm to 690 nm. Diodes are arranged by wavelength and then power. The tables below list basic specifications to help you narrow down your search quickly. The blue button in the Info column within the tables opens a pop-up window that contains more detailed specifications for each item, as well as mechanical drawings.

Notes on Center Wavelength
While the center wavelength is listed for each laser diode, 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. Diodes can be temperature tuned, which will alter the lasing wavelength. A number of items below are listed as Wavelength Tested, which means that the dominant wavelength of each unit has been measured and recorded. After clicking "Choose Item" below, a list will appear that contains the dominant 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.

Packages and Mounts
We offer these visible laser diodes in various packages including standard Ø3.8 mm, Ø5.6 mm, and Ø9 mm TO cans, as well as TO-46, Ø9.5 mm, and fiber-pigtailed TO cans with outputs of either standard fiber connectors or collimators. We have categorized the pin configuration of TO-packaged diodes in standard A, B, C, D, E, F, G, and H pin codes (see image below). This pin code allows the user to easily determine compatible mounts.

Laser Mode and Linewidth
We offer laser diodes with different output characteristics (power, wavelength, beam size, shape, etc.). Most lasers offered here are single transverse mode (single mode or SM) and a few are designed for higher-power multiple-transverse-mode (multimode or MM) operation. For better side mode suppression ratio (SMSR) performance, other devices such as DFB lasers, DBR lasers, or external cavity lasers should be considered. Please see our Laser Diode Tutorial for more information on these topics and laser diodes in general.

Usage Tips
Laser diodes are sensitive to electrostatic shock. Please take the proper precautions when handling the device; see electrostatic shock accessories. These lasers are also sensitive to optical feedback, which can cause significant fluctuations in the output power of the laser diode depending on the application.

For all of the pigtailed laser diodes with fiber connectors at the output, the laser should be off when connecting or disconnecting the device from other fibers, particularly for lasers with power levels above 10 mW. We recommend cleaning the fiber connector before each use if there is any chance that dust or other contaminants may have deposited on the surface. The laser intensity at the center of the fiber tip can be very high and may burn the tip of the fiber if contaminants are present. While the connectors on the pigtailed laser diodes are cleaned and capped before shipping, we cannot guarantee that they will remain free of contamination after they are removed from the package.

Members of our Tech Support staff are available to help you select a laser diode and to discuss possible operation issues.

Pin Codes
Laser Diode Pin Diagram
For warranty information for laser diodes, please refer to the LD Operation tab.
Pin Code Monitor Photodiode
A Yes
B Yes
C Yes
D Yes
E No
F Yes
G No
H No

Choosing a Collimation Lens for Your Laser Diode

Since the output of a laser diode is highly divergent, collimating optics are necessary. Aspheric lenses do not introduce spherical aberration and therefore are commonly chosen when the collimated laser beam is to be between one and five millimeters. A simple example will illustrate the key specifications to consider when choosing the correct lens for a given application. The second example below is an extension of the procedure, which will show how to circularize an elliptical beam.

Example 1: Collimating a Diverging Beam

  • Laser Diode to be Used: L780P010
  • Desired Collimated Beam Diameter: Ø3 mm (Major Axis)

When choosing a collimation lens, it is essential to know the divergence angle of the source being used and the desired output diameter. The specifications for the L780P010 laser diode indicate that the typical parallel and perpendicular FWHM beam divergences are 8° and 30°, respectively. Therefore, as the light diverges, an elliptical beam will result. To collect as much light as possible during the collimation process, consider the larger of these two divergence angles in any calculations (i.e., in this case, use 30°). If you wish to convert your elliptical beam into a round one, we suggest using an anamorphic prism pair, which magnifies one axis of your beam; for details, see Example 2 below.

Assuming that the thickness of the lens is small compared to the radius of curvature, the thin lens approximation can be used to determine the appropriate focal length for the asphere. Assuming a divergence angle of 30° (FWHM) and desired beam diameter of 3 mm:

laser diode collimation drawing focal length calculation
Θ = Divergence Angle Ø = Beam Diameter f = Focal Length r = Collimated Beam Radius = Ø/2

Note that the focal length is generally not equal to the needed distance between the light source and the lens.

With this information known, it is now time to choose the appropriate collimating lens. Thorlabs offers a large selection of aspheric lenses. For this application, the ideal lens is a molded glass aspheric lens with focal length near 5.6 mm and our -B antireflection coating, which covers 780 nm. The C171TMD-B (mounted) or 354171-B (unmounted) aspheric lenses have a focal length of 6.20 mm, which will result in a collimated beam diameter (major axis) of 3.3 mm. Next, check to see if the numerical aperture (NA) of the diode is smaller than the NA of the lens:

0.30 = NALens > NADiode ≈ sin(15°) = 0.26

Up to this point, we have been using the full-width at half maximum (FWHM) beam diameter to characterize the beam. However, a better practice is to use the 1/e2 beam diameter. For a Gaussian beam profile, the 1/e2 diameter is almost equal to 1.7X the FWHM diameter. The 1/e2 beam diameter therefore captures more of the laser diode's output light (for greater power delivery) and minimizes far-field diffraction (by clipping less of the incident light).

A good rule of thumb is to pick a lens with an NA twice that of the laser diode NA. For example, either the A390-B or the A390TM-B could be used as these lenses each have an NA of 0.53, which is more than twice the approximate NA of our laser diode (0.26). These lenses each have a focal length of 4.6 mm, resulting in an approximate major beam diameter of 2.5 mm. In general, using a collimating lens with a short focal length will result in a small collimated beam diameter and a large beam divergence, while a lens with a large focal length will result in a large collimated beam diameter and a small divergence.

Example 2: Circularizing an Elliptical Beam

Using the laser diode and aspheric lens chosen above, we can use an anamorphic prism pair to convert our collimated, elliptical beam into a circular beam.

Prism Ray Diagram

Whereas earlier we considered only the larger divergence angle, we now look at the smaller beam divergence of 8°. From this, and using the effective focal length of the A390-B aspheric lens chosen in Example 1, we can determine the length of the semi-minor axis of the elliptical beam after collimation:

r' = f * tan(Θ'/2) = 4.6 mm * tan(4°) = 0.32 mm

The minor beam diameter is double the semi-minor axis, or 0.64 mm. In order to magnify the minor diameter to be equal to the major diameter of 2.5 mm, we will need an anamorphic prism pair that yields a magnification of 3.9. Thorlabs offers both mounted and unmounted prism pairs. Mounted prism pairs provide the benefit of a stable housing to preserve alignment, while unmounted prism pairs can be positioned at any angle to achieve the exact desired magnification. 

The PS883-B mounted prism pair provides a magnification of 4.0 for a 950 nm wavelength beam. Because shorter wavelengths undergo greater magnification when passing through the prism pair, we can expect our 780 nm beam to be magnified by slightly more than 4.0X. Thus, the beam will still maintain a small degree of ellipticity.

Alternatively, we can use the PS871-B unmounted prism pair to achieve the precise magnification of the minor diameter necessary to produce a circular beam. Using the data available here, we see that the PS871-B achieves a magnification of 4.0 when the prisms are positioned at the following angles for a 670 nm wavelength beam:

α1: +34.608° α2: -1.2455°

Refer to the diagram to the right for α1 and α2 definitions. Our 780 nm laser will experience slightly less magnification than a 670 nm beam passing through the prisms at these angles. Some trial and error may be required to achieve the exact desired magnification. In general: 

  • To increase magnification, rotate the first prism clockwise (increasing α1) and rotate the second prism counterclockwise (decreasing α2).
  • To reduce magnification, rotate the first prism counterclockwise (decreasing α1) and rotate the second prism clockwise (increasing α2).
Remember that the prism pair introduces a linear offset between the input and output beams which increases with greater magnification.

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.

Laser Safety and Classification

Safe practices and proper usage of safety equipment should be taken into consideration when operating lasers. The eye is susceptible to injury, even from very low levels of laser light. Thorlabs offers a range of laser safety accessories that can be used to reduce the risk of accidents or injuries. Laser emission in the visible and near infrared spectral ranges has the greatest potential for retinal injury, as the cornea and lens are transparent to those wavelengths, and the lens can focus the laser energy onto the retina. 

Laser Glasses Laser Curtains Blackout Materials
Enclosure Systems Laser Viewing Cards Alignment Tools
Shutter and Controllers Laser Safety Signs

Safe Practices and Light Safety Accessories

  • Laser safety eyewear must be worn whenever working with Class 3 or 4 lasers.
  • Regardless of laser class, Thorlabs recommends the use of laser safety eyewear whenever working with laser beams with non-negligible powers, since metallic tools such as screwdrivers can accidentally redirect a beam.
  • Laser goggles designed for specific wavelengths should be clearly available near laser setups to protect the wearer from unintentional laser reflections.
  • Goggles are marked with the wavelength range over which protection is afforded and the minimum optical density within that range.
  • Laser Safety Curtains and Laser Safety Fabric shield other parts of the lab from high energy lasers.
  • Blackout Materials can prevent direct or reflected light from leaving the experimental setup area.
  • Thorlabs' Enclosure Systems can be used to contain optical setups to isolate or minimize laser hazards.
  • A fiber-pigtailed laser should always be turned off before connecting it to or disconnecting it from another fiber, especially when the laser is at power levels above 10 mW.
  • All beams should be terminated at the edge of the table, and laboratory doors should be closed whenever a laser is in use.
  • Do not place laser beams at eye level.
  • Carry out experiments on an optical table such that all laser beams travel horizontally.
  • Remove unnecessary reflective items such as reflective jewelry (e.g., rings, watches, etc.) while working near the beam path.
  • Be aware that lenses and other optical devices may reflect a portion of the incident beam from the front or rear surface.
  • Operate a laser at the minimum power necessary for any operation.
  • If possible, reduce the output power of a laser during alignment procedures.
  • Use beam shutters and filters to reduce the beam power.
  • Post appropriate warning signs or labels near laser setups or rooms.
  • Use a laser sign with a lightbox if operating Class 3R or 4 lasers (i.e., lasers requiring the use of a safety interlock).
  • Do not use Laser Viewing Cards in place of a proper Beam Trap.

 

Laser Classification

Lasers are categorized into different classes according to their ability to cause eye and other damage. The International Electrotechnical Commission (IEC) is a global organization that prepares and publishes international standards for all electrical, electronic, and related technologies. The IEC document 60825-1 outlines the safety of laser products. A description of each class of laser is given below:

Class Description Warning Label
1 This class of laser is safe under all conditions of normal use, including use with optical instruments for intrabeam viewing. Lasers in this class do not emit radiation at levels that may cause injury during normal operation, and therefore the maximum permissible exposure (MPE) cannot be exceeded. Class 1 lasers can also include enclosed, high-power lasers where exposure to the radiation is not possible without opening or shutting down the laser.  Class 1
1M Class 1M lasers are safe except when used in conjunction with optical components such as telescopes and microscopes. Lasers belonging to this class emit large-diameter or divergent beams, and the MPE cannot normally be exceeded unless focusing or imaging optics are used to narrow the beam. However, if the beam is refocused, the hazard may be increased and the class may be changed accordingly.  Class 1M
2 Class 2 lasers, which are limited to 1 mW of visible continuous-wave radiation, are safe because the blink reflex will limit the exposure in the eye to 0.25 seconds. This category only applies to visible radiation (400 - 700 nm).  Class 2
2M Because of the blink reflex, this class of laser is classified as safe as long as the beam is not viewed through optical instruments. This laser class also applies to larger-diameter or diverging laser beams.  Class 2M
3R Class 3R lasers produce visible and invisible light that is hazardous under direct and specular-reflection viewing conditions. Eye injuries may occur if you directly view the beam, especially when using optical instruments. Lasers in this class are considered safe as long as they are handled with restricted beam viewing. The MPE can be exceeded with this class of laser; however, this presents a low risk level to injury. Visible, continuous-wave lasers in this class are limited to 5 mW of output power.  Class 3R
3B Class 3B lasers are hazardous to the eye if exposed directly. Diffuse reflections are usually not harmful, but may be when using higher-power Class 3B lasers. Safe handling of devices in this class includes wearing protective eyewear where direct viewing of the laser beam may occur. Lasers of this class must be equipped with a key switch and a safety interlock; moreover, laser safety signs should be used, such that the laser cannot be used without the safety light turning on. Laser products with power output near the upper range of Class 3B may also cause skin burns.  Class 3B
4 This class of laser may cause damage to the skin, and also to the eye, even from the viewing of diffuse reflections. These hazards may also apply to indirect or non-specular reflections of the beam, even from apparently matte surfaces. Great care must be taken when handling these lasers. They also represent a fire risk, because they may ignite combustible material. Class 4 lasers must be equipped with a key switch and a safety interlock.  Class 4
All class 2 lasers (and higher) must display, in addition to the corresponding sign above, this triangular warning sign.  Warning Symbol

Insights into Beam Characterization

Scroll down to read about:

  • Beam Size Measurement Using a Chopper Wheel

Click here for more insights into lab practices and equipment.

 

Beam Size Measurement Using a Chopper Wheel

 

Arc length of a beam spot, as defined by the parameters of a chopper wheel.
Click to Enlarge

Figure 2: The blade traces an arc length of through the center of the beam and has an angular rotation rate of f. The chopper wheel shown is MC1F2.

Chopper wheel setup used to estimate beam diameter.
Click to Enlarge

Figure 1: An approximate measurement of beam size can be found using the illustrated setup. As the blade of the chopper wheel passes through the beam, an S-curve is traced out on the oscilloscope.

Gaussian beam intensity profile with 1/e2 diameter noted.
Click to Enlarge

Figure 4: The diameter of a Gaussian beam is often given in terms of the 1/e2 full width.

Rising edge of S-curve used to estimated beam diameter..
Click to Enlarge

Figure 3: Rise time (tr ) of the intensity signal is typically measured between the 10% and 90% points on the curve. The rise time depends on the wheel's rotation rate and the beam diameter.

Camera and scanning-slit beam profilers are tools for characterizing beam size and shape, but these instruments cannot provide an accurate measurement if the beam size is too small or the wavelength is outside of the operating range.

A chopper wheel, photodetector, and oscilloscope can provide an approximate measurement of the beam size (Figure 1). As the rotating chopper wheel's blade passes through the beam, an S-shaped trace is displayed on the oscilloscope.

When the blade sweeps through the angle θ , the rise or fall time of the S-curve is proportional to the size of the beam along the direction of the blade's travel (Figure 2). A point on the blade located a distance from the center of the wheel sweeps through an arc length (Rθ ) that is approximately equal to the size of the beam along this direction.

To make this beam size measurement, the combined response of the detector and oscilloscope should be much faster than the signal's rate of change. 

Example: S-Curve with Rising Edge
The angle (θ = ft) subtended by the beam depends on the signal's rise time (Figure 3) and the wheel's rotation rate (f ), whose units are Hz or revolutions/s. The arc length ( = R ⋅ ft) through the beam can be calculated using this angle. For a small Gaussian-shaped beam (Figure 4), a first approximation of the 1/ebeam diameter (),

includes a factor of 1.56, which accounts for the portion of the beam measured between the 10% and 90% intensity points being smaller than the 1/e2 beam diameter.

Date of Last Edit: June 22, 2021
Content improved by our readers!


Posted Comments:
Lara Piemontese  (posted 2024-08-27 09:40:51.913)
Hello,I am interested in buying the laser diode HL63163DG because of its higher power with respect to the others. However I have two requirements: the first one is to maintain the polarization (which I don't understand how it is oriented) and the second one is of course the collimation. How can I collimate the output beam and together maintain the polarization? Thank you very much for your help
Zhang Chen  (posted 2024-01-03 14:31:40.733)
Hi, What does it mean that the compliance voltage of LDC220C is greater than 4V??Could I use it to drive L450P1600MM with a working voltage of 4.8V?Thank you!
jweimar  (posted 2024-01-09 03:49:56.0)
Dear Zhang, thank you for your feedback. That means that the Compliance Voltage can be greater than 4V for smaller currents. I will reach out to you directly to discuss this further with you.
Paulo Lourenço  (posted 2023-08-07 17:27:37.087)
Hi there. From what I understood, the LD PL450B requires an S038S package and is not compatible to strain relief cable. Will I still be able to use it with an LTN330-A collimation package? If so, what shall I use instead? Thank you, Paulo Lourenço
ksosnowski  (posted 2023-08-18 06:05:17.0)
Hello Paulo, thanks for reaching out to Thorlabs. Our LTN330-A collimator attachment is only designed to attach to the SR9x cables and our LDHx cageplates. The threading is an otherwise uncommon 13/32"-40TPI one to best fit these laser package sizes. While you are correct that we do not have an SR9 cable option for the 3.8mm size to match this, we do have some passive mounts like S1LM38 which can connect this diode format into an optic tube/cage system. However given the total electrical input power P=IV of your Pin Code G laser, I would strongly recommend use of an actively cooled mount like LDM38. Our LDMx series mounts have front mounting points to attach further optics like collimators as well. From there we also have mounts for different small asphere lens sizes like the one that comes in LTN330-A. Our lens adapter LMRA6.35 is a ring which the lens can be glued into to adapter the outer diameter to 1/2". This will allow mounting of the optic in standard 1/2" lens tubes or cageplates to connect with the laser diode.
大揮 松林  (posted 2023-01-12 09:52:03.457)
L405G2の購入を検討しているのですが,このレーザーダイオードでコリメート光を作る場合どのレンズが適切でしょうか?
cdolbashian  (posted 2023-01-23 11:40:46.0)
Thank you for reaching out to us with this request! I have contacted you directly to assist in selecting components for your experimental design.
D Miller  (posted 2021-06-02 19:40:59.217)
Do you know the degree of polarization for L450P1600MM? Thanks.
YLohia  (posted 2021-06-15 11:05:59.0)
Thank you for contacting Thorlabs. Unfortunately, we don't have a DOP spec for our laser diodes. That being said, the PER should be roughly 400:1, but this is not a formal spec either, but should serve as a reasonable estimate.
Thibault Vieille  (posted 2019-11-18 01:35:10.207)
Hi, Try to set up a high power laser diode (visible betw. 500 and 700nm) with very high power stability. I see your laser driver LD3000R but it is written that it supports A, D and E pin config. However most of your most powerful laser diodes (L638P700M, L638P200, L637G1, L520G1 etc) comes with different pin config. Can you recommend me a correct fit; please?
YLohia  (posted 2019-11-18 11:10:43.0)
Hello, thank you for contacting Thorlabs. For these diodes, depending on the specific diode, we would recommend using the LDC220C driver. This provides up to +/-2 A current and is compatible with all of the diodes mentioned by you.
rawoodruff  (posted 2018-09-15 10:30:46.96)
What spectral width would you expect from your UV and visible diodes: single mode and multimode?
YLohia  (posted 2018-09-24 11:32:11.0)
Hello, thank you for contacting Thorlabs. We have linewidth test data for some of the diodes in the pigtailed laser diodes pages. Please note that these are Fabry-Perot diodes (with the exception of the DJ532) and cannot be used for single frequency applications. I have reached out to you directly to get a better sense of your application and what specific wavelengths you are interested in.
paul.janin  (posted 2018-06-05 17:36:06.44)
Hello, I've been trying to modulate an L637P5 with a square wave around threshold. However, the diode seems to respond too slowly to the modulation to follow the square wave even at frequencies as low as 10kHz. Do you know what could be the cause of this slow response ? The diode manages to follow a sine modulation even at higher frequencies, although with some attenuation. Thank you.
YLohia  (posted 2018-07-27 03:24:04.0)
Hello, thank you for contacting Thorlabs. Based on our discussion, the modulation bandwidth of the LDC201ULN driver you have is specified to be 3kHz. This bandwidth is only applicable to small signal sine wave modulation (not square wave). Another thing that can impact the bandwidth measurements is the terminating load resistance being used with your detector/oscilloscope. For fast measurements, a 50 Ohm load should be used (not 1 MOhm).
vjadrisko  (posted 2017-05-19 14:03:07.04)
Hi there, i am interested in laser diode LP660-SF20 but would like to know is it polarized and if so which polarization it is ? Thank you.
tfrisch  (posted 2017-05-19 05:05:17.0)
Hello, thank you for contacting Thorlabs. The light is polarized, but the state will be changed depending on bending and stressing of the SM fiber. We have fiber polarization management solutions in the link below. I will reach out to you to discuss these. https://www.thorlabs.com/navigation.cfm?guide_id=2089
ross.leyman  (posted 2015-05-13 17:45:00.44)
Hi there, Regarding the L520P120 - do you know what the beam diameter immediately at the diode package output window is? It looks like a clear aperture of 1.6mm but it's hard to tell of course. Also, can this module be driven in pulse-mode operation or is it strictly CW only? And if pulse is ok, can a higher (peak) output power be achieved as one might expect? Thanks in advance, Ross
besembeson  (posted 2015-08-28 10:42:41.0)
Response from Bweh at Thorlabs USA: Our UK office will provide the beam diameter estimate at the window to you. We don't have modulation specifications for this diode, which is why we specify the diode under cw conditions. We don't also recommend pulsing at high peak powers. While the diode can in theory be pulsed, we recommend applying a DC bias current to threshold and pulsing above that.
sinerkim  (posted 2014-01-24 08:37:01.07)
Could you provide a LP520-SF15 without any fiber coupling?
jacob.sendowski  (posted 2013-08-21 21:27:04.24)
I would like to know the linewidth of this laser source. Also what time of temperature controlled mount would you recommend for operating this laser? thanks Jdogg
tcohen  (posted 2013-08-22 14:49:00.0)
Response from Tim at Thorlabs: The linewidth of the LP785-SF100 is ~.5nm typical, max of 2nm. You can mount this with an LM9LP. We now show the individual tested datasheets corresponding to our current stock on our website. You can see measured spectrum by clicking the "Choose Item" link right next to the part number. In some cases, these plots will be limited to the spectral resolution of the spectrometer used. In this case, the spectrometer used has a resolution of <.6nm FWHM @633nm.
saktinst  (posted 2013-06-18 16:05:00.883)
I am going to use diode laser to mark my organic material. Do you have any idea what kind of laser can i use? Is it also this diode laser provided by scanning head to mark barcode code? Thanks
jlow  (posted 2013-06-20 10:50:00.0)
Response from Jeremy at Thorlabs: The correct laser to use would depend on the material that you are using and its absorption characteristic. I will get in contact with you directly to discuss about your application further.
cristina.martinez-g  (posted 2013-04-17 10:16:47.623)
Will be offered, in a near future, cheap lasers near 760nm ? Thank you very much, cristina
tcohen  (posted 2013-04-25 12:57:00.0)
Response from Tim at Thorlabs to Cristina: Thank you for your inquiry. We will take your feedback into consideration as we look to expand our wavelength selection and I will contact you directly to discuss your application.
werneck  (posted 2013-04-07 21:04:57.74)
1) On datasheet of LPM-660-SMA it reads slope efficiency=0,75 mW/mA, output power=22.5 mW and operating current 65 mA. However, for a current of 65 mA with a slope efficiency of .75 it would produce an output power of 48.8mW not 22.5 mW as stated. On the other hand, if I want 22 mW output power, from the slope efficiency I calculate 29 mA which is below the threshold current. What is wrong? 2) "Monitor current" is the output current of PD when LD is at maximum output power?
jlow  (posted 2013-04-09 12:11:00.0)
Response from Jeremy at Thorlabs: The slope efficiency is defined as ?P/?I and not P/I. The drive current below the threshold current of the laser diode does not contribute to light emission and therefore the slope is taken from the line in the laser power vs. current curve after the threshold current. In the characterization sheet sent with each laser diode pigtail, the monitor current is the current of the internal photodiode when the output is at 22mW.
olsonaj  (posted 2013-03-16 17:51:31.903)
Do you know if anyone has used the LD785-SH300 in an external cavity diode laser configuration? Any reason why you believe it may or may not work in such a setup?
jlow  (posted 2013-03-28 08:36:00.0)
Response from Jeremy at Thorlabs: We do not have any data on using this laser diode in an external cavity. We will get in contact with you to discuss in more details about your application.
Tyler  (posted 2012-07-31 17:52:43.0)
Hello Florian, The 1418 Euro price is based on what it cost Thorlabs to purchase the laser diodes in 2008. I am sorry that this hasn't been updated to be consistent with the current cost of laser diodes. Thank you for taking the time to point out the price of the DL3146-151 laser diode to us. I will work on getting the price of the diode fixed right away. Sincerely, Tyler
florian.kehl  (posted 2012-07-27 02:47:49.0)
Dear Sir or Madam, we're frequent customers and so far happy with your products and service. But selling a DL3146-151 for 1418€ doesn't seem to be a fair price at all, since exactly the same product is being sold for only 18€, for example if you check: http://www.roithner-laser.com/pricelist.pdf. How can this discrepancy be explained? Thanks!
tcohen  (posted 2012-04-03 10:46:00.0)
Response from Tim at Thorlabs: Laser diodes can be delicate and require precise drive electronics. Because there is a maximum current which cannot be exceeded even for a very limited amount of time, spikes in electronics will cause immediate damage. Because a tiny change in voltage can be a large change in current, as seen on a LD’s I-V curve, temperature and other fluctuations in electronics when using a voltage source can cause the maximum drive current to be exceeded and damage the LD. For this reason, current sources are typically used.
ZWJIORO  (posted 2012-03-30 02:17:48.0)
Dear Thorlabs, could a voltage source drive the LD?Thanks!
jjurado  (posted 2011-04-06 15:33:00.0)
Response from Javier at Thorlabs to last poster: Thank you very much for your feedback. We will split the presentation of the L375P020MLD laser diode into another page in order to make it more visible. The new page will go live shortly.
user  (posted 2011-04-06 08:26:24.0)
L375P020MLD would get more attention if this group were titled NUV - Visible Laser Diodes
Thorlabs  (posted 2010-08-31 13:51:26.0)
Response from Javier at Thorlabs: Most of our laser diodes operate in single transverse mode and multi-longitudinal mode. Laser diodes are highly divergent sources, with a full angle output usually in the range of 30 degrees. You can refer to the Collimation Tutorial tab for information on how to choose the most appropriate optic for collimating the output of your laser. I will contact you directly to discuss your application.
aroy25  (posted 2010-08-27 18:58:42.0)
Are the single mode lasers also single transverse mode? I am looking for a TEM00 profile..what is the beam diameter? regards
Adam  (posted 2010-05-20 21:06:36.0)
A response from Adam at Thorlabs to chenli: The laser diode controller, ITC510, has been superceded by the ITC4001. This product is a laser diode current and temperature controller, which can output of to 1A for laser diode current control and 8A for laser diode temperature control. I will contact you directly to determine the exact information that you need.
chenli_hust  (posted 2010-05-20 19:31:03.0)
I want to know some information about LASER DIODE COMBI CONTROLLER:ITC510,would you do me some help? Im looking forward to your reply.
Laurie  (posted 2010-03-29 17:37:27.0)
A response from Laurie at Thorlabs to mph: Thank you for your feedback on our website. Currently, we are in the process of giving this page a makeover of sorts, so I am unable to make the suggested change visible to the general public immediately. However, we will be sure to include your suggested change in the new version of this page, which should be available in a few weeks. Thanks again for taking the time to provide valuable feedback!
mph  (posted 2010-03-29 17:24:13.0)
In the overview, you use `discreet incorrectly. discreet:judicious in ones conduct or speech, esp. with regard to respecting privacy or maintaining silence about something of a delicate nature; prudent; circumspect. You should change this to `discrete.
klee  (posted 2009-07-17 15:33:25.0)
A response from Ken at Thorlabs to alessandro: There is no direct replacement for the HL785MG. The closest alternatives in terms of wavelength and power are HL7851G (785nm, 50mW) and DL4140-001S (785nm, 25mW).
alessandro  (posted 2009-07-17 13:26:24.0)
Dear All, What is the substitute of HL7859MG that was discontinued?
klee  (posted 2009-06-22 18:58:36.0)
Response from Ken at Thorlabs to BiryukovAA: We do not carry any green laser diodes but we do offer a few green HeNe lasers.
BiryukovAA  (posted 2009-06-22 09:15:28.0)
Our company is looking for Green Laser Diodes (543 nm). Can you offer any laser diodes operating on this wavelength. thank you, Alexey Biryukov.
j.velde  (posted 2009-03-17 06:11:13.0)
What is the mode field dia on this LD? Also do Thorlabs offer AR coated LD? Thank you! Jeroen van de Velde Applied Laser Technology
Laurie  (posted 2009-02-12 10:05:29.0)
Response from Laurie at Thorlabs to dajun.wang: The HL6548FG is AR coated for the wavelength of the diode. We are in the process of trying to obtain more specific information and will update you shortly.
dajun.wang  (posted 2009-02-09 19:06:13.0)
Hi, We bought some these HL6548FG 658 diodes from thorlabs for scientific research. One special thing is we want to put these diodes in an external cavity configuration to control the emission wavelength. Is it possible to let us know the coating material on the output facet of these diodes? We need to put additional anti-reflection coating on them by ourselves to help wavelength control. Your help is highly appreciated. With best wishes, Dajun
lsandstrom  (posted 2008-06-26 10:16:47.0)
Are the lasers lateral or longitudinal multi-mode when you state in the spec. that the lasers are multi mode?
technicalmarketing  (posted 2008-02-13 14:19:43.0)
In response to acables comments, we have added a link to an excel file that shows the compatibility between our drivers and diodes. In the future, we hope to work with our web team to provide a selection.
acable  (posted 2007-10-31 19:02:34.0)
It would be nice to have a link to the laser diode and TEC drivers from this page. It would be even better to have a linked selection guide to show all of the options for each of the lasers.
technicalmarketing  (posted 2007-10-22 08:34:05.0)
Dear rodolfls, I apologize for the delay in getting this information to you. We had to pass your inquiry to our technical support staff in Japan, who then in turn had to contact the vendor. According to the vendor, the wavelength variation/current variation is about 0.04 nm/mA and the wavelength variation/temerature variation is about 0.2 nm/K. We hope that this information is helpful to you.
rodolfls  (posted 2007-10-14 01:04:05.0)
I would like to know some characteristics of Eudyna FLD6A2TK: wavelenght variation/current variation = ? nm/mA and wavelenght variation/temperature variation = ? nm/K Thank you, Rodolfo.
melsscal  (posted 2007-09-19 06:40:08.0)
Dear Mr.Mark Struzzi, Can you please mail me the catalouge Page of the laser diode L980P200J asap. Regards for MEL SYSTEMS & SERVICES LTD. Aroop Kanti Bose Area Manager-Sales Kolkata Branch www.melssindia.com

The rows shaded green below denote single-frequency lasers.

Item #WavelengthOutput PowerOperating
Current
Operating
Voltage
Beam DivergenceLaser ModePackage
ParallelPerpendicular
L375P70MLD375 nm70 mW110 mA5.4 V22.5°Single Transverse ModeØ5.6 mm
L404P400M404 nm400 mW370 mA4.9 V13° (1/e2)42° (1/e2)MultimodeØ5.6 mm
LP405-SF10405 nm10 mW50 mA5.0 V--Single Transverse ModeØ5.6 mm, SM Pigtail
L405P20405 nm20 mW38 mA4.8 V8.5°19°Single Transverse ModeØ5.6 mm
LP405C1405 nm30 mW75 mA4.3 V1.4 mrad1.4 mradSingle Transverse ModeØ3.8 mm, SM Pigtail with Collimator
L405G2405 nm35 mW50 mA4.9 V10°21°Single Transverse ModeØ3.8 mm
DL5146-101S405 nm40 mW70 mA5.2 V19°Single Transverse ModeØ5.6 mm
L405A1405 nm175 mW (Min)150 mA5.0 V20°Single Transverse ModeØ5.6 mm
LP405-MF300405 nm300 mW350 mA4.5 V--MultimodeØ5.6 mm, MM Pigtail
L405G1405 nm1000 mW900 mA5.0 V13°45°MultimodeØ9 mm
LP450-SF25450 nm25 mW75 mA5.0 V--Single Transverse ModeØ5.6 mm, SM Pigtail
L450G3450 nm100 mW (Min)80 mA5.2 V8.4°21.5°Single Transverse ModeØ3.8 mm
L450G2450 nm100 mW (Min)80 mA5.0 V8.4°21.5°Single Transverse ModeØ5.6 mm
L450P1600MM450 nm1600 mW1200 mA4.8 V19 - 27°MultimodeØ5.6 mm
L473P100473 nm100 mW120 mA5.7 V1024Single Transverse ModeØ5.6 mm
LP488-SF20488 nm20 mW70 mA6.0 V--Single Transverse ModeØ5.6 mm, SM Pigtail
LP488-SF20G488 nm20 mW80 mA5.5 V--Single Transverse ModeØ5.6 mm, SM Pigtail
L488P60488 nm60 mW75 mA6.8 V23°Single Transverse ModeØ5.6 mm
LP515-SF3515 nm3 mW50 mA5.3 V--Single Transverse ModeØ5.6 mm, SM Pigtail
L515A1515 nm10 mW50 mA5.4 V6.5°21°Single Transverse ModeØ5.6 mm
LP520-SF15A520 nm15 mW100 mA7.0 V--Single Transverse ModeØ5.6 mm, SM Pigtail
LP520-SF15520 nm15 mW140 mA6.5 V--Single Transverse ModeØ9 mm, SM Pigtail
L520A1520 nm30 mW (Min)80 mA5.5 V22°Single Transverse ModeØ5.6 mm
PL520520 nm50 mW250 mA7.0 V22°Single Transverse ModeØ3.8 mm
L520P50520 nm45 mW150 mA7.0 V22°Single Transverse ModeØ5.6 mm
L520A2520 nm110 mW (Min)225 mA5.9 V22°Single Transverse ModeØ5.6 mm
DJ532-10532 nm10 mW220 mA1.9 V0.69°0.69°Single Transverse ModeØ9.5 mm (non-standard)
DJ532-40532 nm40 mW330 mA1.9 V0.69°0.69°Single Transverse ModeØ9.5 mm (non-standard)
LP633-SF50633 nm50 mW170 mA2.6 V--Single Transverse ModeØ5.6 mm, SM Pigtail
HL63163DG633 nm100 mW170 mA2.6 V8.5°18°Single Transverse ModeØ5.6 mm
LPS-635-FC635 nm2.5 mW70 mA2.2 V--Single Transverse ModeØ9 mm, SM Pigtail
LPS-PM635-FC635 nm2.5 mW60 mA2.2 V--Single Transverse ModeØ9.0 mm, PM Pigtail
L635P5635 nm5 mW30 mA<2.7 V32°Single Transverse ModeØ5.6 mm
HL6312G635 nm5 mW50 mA<2.7 V31°Single Transverse ModeØ9 mm
LPM-635-SMA635 nm8 mW50 mA2.2 V--MultimodeØ9 mm, MM Pigtail
LP635-SF8635 nm8 mW60 mA2.3 V--Single Transverse ModeØ5.6 mm, SM Pigtail
HL6320G635 nm10 mW60 mA2.2 V31°Single Transverse ModeØ9 mm
HL6322G635 nm15 mW75 mA2.4 V30°Single Transverse ModeØ9 mm
L637P5637 nm5 mW20 mA<2.4 V34°Single Transverse ModeØ5.6 mm
LP637-SF50637 nm50 mW140 mA2.6 V--Single Transverse ModeØ5.6 mm, SM Pigtail
LP637-SF70637 nm70 mW220 mA2.7 V--Single Transverse ModeØ5.6 mm, SM Pigtail
HL63142DG637 nm100 mW140 mA2.7 V18°Single Transverse ModeØ5.6 mm
HL63133DG637 nm170 mW250 mA2.8 V17°Single Transverse ModeØ5.6 mm
HL6388MG637 nm250 mW340 mA2.3 V10°40°MultimodeØ5.6 mm
L637G1637 nm1200 mW1100 mA2.5 V10°32°MultimodeØ9 mm (non-standard)
L638P040638 nm40 mW92 mA2.4 V10°21°Single Transverse ModeØ5.6 mm
L638P150638 nm150 mW230 mA2.7 V918Single Transverse ModeØ3.8 mm
L638P200638 nm200 mW280 mA2.9 V814Single Transverse ModeØ5.6 mm
L638P700M638 nm700 mW820 mA2.2 V35°MultimodeØ5.6 mm
HL6358MG639 nm10 mW40 mA2.4 V21°Single Transverse ModeØ5.6 mm
HL6323MG639 nm30 mW100 mA2.5 V8.5°30°Single Transverse ModeØ5.6 mm
HL6362MG640 nm40 mW90 mA2.5 V10°21°Single Transverse ModeØ5.6 mm
LP642-SF20642 nm20 mW90 mA2.5 V--Single Transverse ModeØ5.6 mm, SM Pigtail
LP642-PF20642 nm20 mW110 mA2.5 V--Single Transverse ModeØ5.6 mm, PM Pigtail
HL6364DG642 nm60 mW120 mA2.5 V10°21°Single Transverse ModeØ5.6 mm
HL6366DG642 nm80 mW150 mA2.5 V10°21°Single Transverse ModeØ5.6 mm
HL6385DG642 nm150 mW250 mA2.6 V17°Single Transverse ModeØ5.6 mm
L650P007650 nm7 mW28 mA2.2 V28°Single Transverse ModeØ5.6 mm
LPS-660-FC658 nm7.5 mW65 mA2.6 V--Single Transverse ModeØ5.6 mm, SM Pigtail
LP660-SF20658 nm20 mW80 mA2.6 V--Single Transverse ModeØ5.6 mm, SM Pigtail
LPM-660-SMA658 nm22.5 mW65 mA2.6 V--MultimodeØ5.6 mm, MM Pigtail
HL6501MG658 nm30 mW75 mA2.6 V8.5°22°Single Transverse ModeØ5.6 mm
L658P040658 nm40 mW75 mA2.2 V10°20°Single Transverse ModeØ5.6 mm
LP660-SF40658 nm40 mW135 mA2.5 V--Single Transverse ModeØ5.6 mm, SM Pigtail
LP660-SF60658 nm60 mW210 mA2.4 V--Single Transverse ModeØ5.6 mm, SM Pigtail
HL6544FM660 nm50 mW115 mA2.3 V10°17°Single Transverse ModeØ5.6 mm
LP660-SF50660 nm50 mW140 mA2.3 V--Single Transverse ModeØ5.6 mm, SM Pigtail
HL6545MG660 nm120 mW170 mA2.45 V10°17°Single Transverse ModeØ5.6 mm
L660P120660 nm120 mW175 mA2.5 V10°17°Single Transverse ModeØ5.6 mm
L670VH1670 nm1 mW2.5 mA2.6 V10°10°Single Transverse ModeTO-46
LPS-675-FC670 nm2.5 mW55 mA2.2 V--Single Transverse ModeØ9 mm, SM Pigtail
HL6748MG670 nm10 mW30 mA2.2 V25°Single Transverse ModeØ5.6 mm
HL6714G670 nm10 mW55 mA<2.7 V22°Single Transverse ModeØ9 mm
HL6756MG670 nm15 mW35 mA2.3 V24°Single Transverse ModeØ5.6 mm
LP685-SF15685 nm15 mW55 mA2.1 V--Single Transverse ModeØ5.6 mm, SM Pigtail
HL6750MG685 nm50 mW70 mA2.3 V21°Single Transverse ModeØ5.6 mm
HL6738MG690 nm30 mW85 mA2.5 V8.5°19°Single Transverse ModeØ5.6 mm
LP705-SF15705 nm15 mW55 mA2.3 V--Single Transverse ModeØ5.6 mm, SM Pigtail
HL7001MG705 nm40 mW75 mA2.5 V18°Single Transverse ModeØ5.6 mm
LP730-SF15730 nm15 mW70 mA2.5 V--Single Transverse ModeØ5.6 mm, SM Pigtail
HL7302MG730 nm40 mW75 mA2.5 V18°Single Transverse ModeØ5.6 mm
L760VH1760 nm0.5 mW3 mA (Max)2.2 V12°12°Single FrequencyTO-46
DBR760PN761 nm9 mW125 mA2.0 V--Single FrequencyButterfly, PM Pigtail
L763VH1763 nm0.5 mW3 mA (Max)2.0 V10°10°Single FrequencyTO-46
DBR767PN767 nm23 mW220 mA1.87 V--Single FrequencyButterfly, PM Pigtail
DBR770PN770 nm35 mW220 mA1.92 V--Single FrequencyButterfly, PM Pigtail
L780P010780 nm10 mW24 mA1.8 V30°Single Transverse ModeØ5.6 mm
DBR780PN780 nm45 mW250 mA1.9 V--Single FrequencyButterfly, PM Pigtail
L785P5785 nm5 mW28 mA1.9 V10°29°Single Transverse ModeØ5.6 mm
LPS-PM785-FC785 nm6.5 mW60 mA---Single Transverse ModeØ5.6 mm, PM Pigtail
LPS-785-FC785 nm10 mW65 mA1.85 V--Single Transverse ModeØ5.6 mm, SM Pigtail
LP785-SF20785 nm20 mW85 mA1.9 V--Single Transverse ModeØ5.6 mm, SM Pigtail
DBR785S785 nm25 mW230 mA2.0 V--Single FrequencyButterfly, SM Pigtail
DBR785P785 nm25 mW230 mA2.0 V--Single FrequencyButterfly, PM Pigtail
L785P25785 nm25 mW45 mA1.9 V30°Single Transverse ModeØ5.6 mm
FPV785S785 nm50 mW410 mA2.2 V--Single FrequencyButterfly, SM Pigtail
FPV785P785 nm50 mW410 mA2.1 V--Single FrequencyButterfly, PM Pigtail
LP785-SAV50785 nm50 mW500 mA2.2 V--Single FrequencyØ9 mm, SM Pigtail
L785P090785 nm90 mW125 mA2.0 V10°17°Single Transverse ModeØ5.6 mm
LP785-SF100785 nm100 mW300 mA2.0 V--Single Transverse ModeØ9 mm, SM Pigtail
FPL785P785 nm200 mW500 mA2.1 V--Single Transverse ModeButterfly, PM Pigtail
FPL785S-250785 nm250 mW (Min)500 mA2.0 V--Single Transverse ModeButterfly, SM Pigtail
LD785-SEV300785 nm300 mW500 mA (Max)2.0 V16°Single FrequencyØ9 mm
LD785-SH300785 nm300 mW400 mA2.0 V18°Single Transverse ModeØ9 mm
FPL785C785 nm300 mW400 mA2.0 V18°Single Transverse Mode3 mm x 5 mm Submount
LD785-SE400785 nm400 mW550 mA2.0 V16°Single Transverse ModeØ9 mm
FPV785M785 nm600 mW1100 mA1.9 V--MultimodeButterfly, MM Pigtail
L795VH1795 nm0.25 mW1.2 mA1.8 V20°12°Single FrequencyTO-46
DBR795PN795 nm40 mW230 mA2.0 V--Single FrequencyButterfly, PM Pigtail
DBR808PN808 nm42 mW250 mA2 V--Single FrequencyButterfly, PM Pigtail
LP808-SA60808 nm60 mW150 mA1.9 V--Single Transverse ModeØ9 mm, SM Pigtail
M9-808-0150808 nm150 mW180 mA1.9 V17°Single Transverse ModeØ9 mm
L808P200808 nm200 mW260 mA2 V10°30°MultimodeØ5.6 mm
FPL808P808 nm200 mW600 mA2.1 V--Single Transverse ModeButterfly, PM Pigtail
FPL808S808 nm200 mW750 mA2.3 V--Single Transverse ModeButterfly, SM Pigtail
L808H1808 nm300 mW400 mA2.1 V14°Single Transverse ModeØ9 mm
LD808-SE500808 nm500 mW750 mA2.2 V14°Single Transverse ModeØ9 mm
LD808-SEV500808 nm500 mW800 mA (Max)2.2 V14°Single FrequencyØ9 mm
L808P500MM808 nm500 mW650 mA1.8 V12°30°MultimodeØ5.6 mm
L808P1000MM808 nm1000 mW1100 mA2 V30°MultimodeØ9 mm
DBR816PN816 nm45 mW250 mA1.95 V--Single FrequencyButterfly, PM Pigtail
LP820-SF80820 nm80 mW230 mA2.3 V--Single Transverse ModeØ5.6 mm, SM Pigtail
L820P100820 nm100 mW145 mA2.1 V17°Single Transverse ModeØ5.6 mm
L820P200820 nm200 mW250 mA2.4 V17°Single Transverse ModeØ5.6 mm
DBR828PN828 nm24 mW250 mA2.0 V--Single FrequencyButterfly, PM Pigtail
LPS-830-FC830 nm10 mW120 mA---Single Transverse ModeØ5.6 mm, SM Pigtail
LPS-PM830-FC830 nm10 mW50 mA2.0 V--Single Transverse ModeØ5.6 mm, PM Pigtail
LP830-SF30830 nm30 mW115 mA1.9 V--Single Transverse ModeØ9 mm, SM Pigtail
HL8338MG830 nm50 mW75 mA1.9 V22°Single Transverse ModeØ5.6 mm
L830H1830 nm250 mW3 A (Max)2 V10°Single Transverse ModeØ9 mm
FPL830P830 nm300 mW900 mA2.22 V--Single Transverse ModeButterfly, PM Pigtail
FPL830S830 nm350 mW900 mA2.5 V--Single Transverse ModeButterfly, SM Pigtail
LD830-SE650830 nm650 mW900 mA2.3 V13°Single Transverse ModeØ9 mm
LD830-MA1W830 nm1 W2 A2.1 V24°MultimodeØ9 mm
LD830-ME2W830 nm2 W3 A (Max)2.0 V21°MultimodeØ9 mm
L840P200840 nm200 mW255 mA2.4 V917Single Transverse ModeØ5.6 mm
L850VH1850 nm1 mW6 mA (Max)2 V12°12°Single FrequencyTO-46
L850P010850 nm10 mW50 mA2 V10°30°Single Transverse ModeØ5.6 mm
L850P030850 nm30 mW65 mA2 V8.5°30°Single Transverse ModeØ5.6 mm
FPV852S852 nm20 mW400 mA2.2 V--Single FrequencyButterfly, SM Pigtail
FPV852P852 nm20 mW400 mA2.2 V--Single FrequencyButterfly, PM Pigtail
DBR852PN852 nm24 mW300 mA2.0 V--Single FrequencyButterfly, PM Pigtail
LP852-SF30852 nm30 mW115 mA1.9 V--Single Transverse ModeØ9 mm, SM Pigtail
L852P50852 nm50 mW75 mA1.9 V22°Single Transverse ModeØ5.6 mm
LP852-SF60852 nm60 mW150 mA2.0 V--Single Transverse ModeØ9 mm, SM Pigtail
L852P100852 nm100 mW120 mA1.9 V28°Single Transverse ModeØ9 mm
L852P150852 nm150 mW170 mA1.9 V18°Single Transverse ModeØ9 mm
L852SEV1852 nm270 mW400 mA (Max)2.0 V12°Single FrequencyØ9 mm
L852H1852 nm300 mW415 mA (Max)2 V15°Single Transverse ModeØ9 mm
FPL852P852 nm300 mW900 mA2.35 V--Single Transverse ModeButterfly, PM Pigtail
FPL852S852 nm350 mW900 mA2.5 V--Single Transverse ModeButterfly, SM Pigtail
LD852-SE600852 nm600 mW950 mA2.3 V7° (1/e2)13° (1/e2)Single Transverse ModeØ9 mm
LD852-SEV600852 nm600 mW1050 mA (Max)2.2 V13° (1/e2)Single FrequencyØ9 mm
LP880-SF3880 nm3 mW25 mA2.2 V--Single Transverse ModeØ5.6 mm, SM Pigtail
L880P010880 nm10 mW30 mA2.0 V12°37°Single Transverse ModeØ5.6 mm
L895VH1895 nm0.2 mW1.4 mA1.6 V20°13°Single FrequencyTO-46
DBR895PN895 nm12 mW300 mA2 V--Single FrequencyButterfly, PM Pigtail
LP904-SF3904 nm3 mW30 mA1.5 V--Single Transverse ModeØ5.6 mm, SM Pigtail
L904P010904 nm10 mW50 mA2.0 V10°30°Single Transverse ModeØ5.6 mm
LP915-SF40915 nm40 mW130 mA1.5 V--Single Transverse ModeØ9 mm, SM Pigtail
DBR935PN935 nm13 mW300 mA1.75 V--Single FrequencyButterfly, PM Pigtail
LP940-SF30940 nm30 mW90 mA1.5 V--Single Transverse ModeØ9 mm, SM Pigtail
M9-940-0200940 nm200 mW270 mA1.9 V28°Single Transverse ModeØ9 mm
L960H1960 nm250 mW400 mA2.1 V11°12°Single Transverse ModeØ9 mm
FPV976S976 nm30 mW400 mA (Max)2.2 V--Single FrequencyButterfly, SM Pigtail
FPV976P976 nm30 mW400 mA (Max)2.2 V--Single FrequencyButterfly, PM Pigtail
DBR976PN976 nm33 mW450 mA2.0 V--Single FrequencyButterfly, PM Pigtail
L976SEV1976 nm270 mW400 mA (Max)2.0 V12°Single FrequencyØ9 mm
BL976-SAG3976 nm300 mW470 mA2.0 V--Single Transverse ModeButterfly, SM Pigtail
BL976-PAG500976 nm500 mW830 mA2.0 V--Single Transverse ModeButterfly, PM Pigtail
BL976-PAG700976 nm700 mW1090 mA2.0 V--Single Transverse ModeButterfly, PM Pigtail
BL976-PAG900976 nm900 mW1480 mA2.5 V--Single Transverse ModeButterfly, PM Pigtail
L980P010980 nm10 mW25 mA2 V10°30°Single Transverse ModeØ5.6 mm
LP980-SF15980 nm15 mW70 mA1.5 V--Single Transverse ModeØ5.6 mm, SM Pigtail
L980P030980 nm30 mW50 mA1.5 V10°35°Single Transverse ModeØ5.6 mm
L980P100A980 nm100 mW150 mA1.6 V32°MultimodeØ5.6 mm
LP980-SA60980 nm60 mW230 mA2.0 V--Single Transverse ModeØ9.0 mm, SM Pigtail
L980H1980 nm200 mW300 mA (Max)2.0 V13°Single Transverse ModeØ9 mm
L980P200980 nm200 mW300 mA1.5 V30°MultimodeØ5.6 mm
DBR1060SN1060 nm130 mW650 mA2.0 V--Single FrequencyButterfly, SM Pigtail
DBR1060PN1060 nm130 mW650 mA1.8 V--Single FrequencyButterfly, PM Pigtail
DBR1064S1064 nm40 mW150 mA2.0 V--Single FrequencyButterfly, SM Pigtail
DBR1064P1064 nm40 mW150 mA2.0 V--Single FrequencyButterfly, PM Pigtail
DBR1064PN1064 nm110 mW550 mA2.0 V--Single FrequencyButterfly, PM Pigtail
LPS-1060-FC1064 nm50 mW220 mA1.4 V--Single Transverse ModeØ9 mm, SM Pigtail
M9-A64-02001064 nm200 mW280 mA1.7 V28°Single Transverse ModeØ9 mm
L1064H11064 nm300 mW700 mA1.92 V7.6°13.5°Single Transverse ModeØ9 mm
L1064H21064 nm450 mW1100 mA1.92 V7.6°13.5°Single Transverse ModeØ9 mm
DBR1083PN1083 nm100 mW500 mA1.75 V--Single FrequencyButterfly, PM Pigtail
L1270P5DFB1270 nm5 mW15 mA1.1 VSingle FrequencyØ5.6 mm
L1290P5DFB1290 nm5 mW16 mA1.0 VSingle FrequencyØ5.6 mm
LP1310-SAD21310 nm2.0 mW40 mA1.1 V--Single FrequencyØ5.6 mm, SM Pigtail
LP1310-PAD21310 nm2.0 mW40 mA1.0 V--Single FrequencyØ5.6 mm, PM Pigtail
LPS-PM1310-FC1310 nm2.5 mW20 mA1.1 V--Single Transverse ModeØ5.6 mm, PM Pigtail
L1310P5DFB1310 nm5 mW16 mA1.0 VSingle FrequencyØ5.6 mm
LPSC-1310-FC1310 nm50 mW350 mA2 V--Single Transverse ModeØ5.6 mm, SM Pigtail
FPL1053S1310 nm130 mW400 mA1.7 V--Single Transverse ModeButterfly, SM Pigtail
FPL1053P1310 nm130 mW400 mA1.7 V--Single Transverse ModeButterfly, PM Pigtail
FPL1053T1310 nm300 mW (Pulsed)750 mA2 V15°28°Single Transverse ModeØ5.6 mm
FPL1053C1310 nm300 mW (Pulsed)750 mA2 V15°27°Single Transverse ModeChip on Submount
L1310G11310 nm2000 mW5 A1.5 V24°MultimodeØ9 mm
L1330P5DFB1330 nm5 mW14 mA1.0 VSingle FrequencyØ5.6 mm
L1370G11370 nm2000 mW5 A1.4 V22°MultimodeØ9 mm
BL1425-PAG5001425 nm500 mW1600 mA2.0 V--Single Transverse ModeButterfly, PM Pigtail
BL1436-PAG5001436 nm500 mW1600 mA2.0 V--Single Transverse ModeButterfly, PM Pigtail
L1450G11450 nm2000 mW5 A1.4 V22°MultimodeØ9 mm
BL1456-PAG5001456 nm500 mW1600 mA2.0 V--Single Transverse ModeButterfly, PM Pigtail
L1470P5DFB1470 nm5 mW19 mA1.0 VSingle FrequencyØ5.6 mm
L1480G11480 nm2000 mW5 A1.6 V20°MultimodeØ9 mm
L1490P5DFB1490 nm5 mW24 mA1.0 VSingle FrequencyØ5.6 mm
L1510P5DFB1510 nm5 mW20 mA1.0 VSingle FrequencyØ5.6 mm
L1530P5DFB1530 nm5 mW21 mA1.0 VSingle FrequencyØ5.6 mm
LPS-1550-FC1550 nm1.5 mW30 mA1.0 V--Single Transverse ModeØ5.6 mm, SM Pigtail
LPS-PM1550-FC1550 nm1.5 mW30 mA1.1 V--Single Transverse ModeØ5.6 mm, SM Pigtail
LP1550-SAD21550 nm2.0 mW40 mA1.0 V--Single FrequencyØ5.6 mm, SM Pigtail
LP1550-PAD21550 nm2.0 mW40 mA1.0 V--Single FrequencyØ5.6 mm, PM Pigtail
L1550P5DFB1550 nm5 mW20 mA1.0 V10°Single FrequencyØ5.6 mm
ML925B45F1550 nm5 mW30 mA1.1 V25°30°Single Transverse ModeØ5.6 mm
SFL1550S1550 nm40 mW300 mA1.5 V--Single FrequencyButterfly, SM Pigtail
SFL1550P1550 nm40 mW300 mA1.5 V--Single FrequencyButterfly, PM Pigtail
LPSC-1550-FC1550 nm50 mW250 mA2 V--Single Transverse ModeØ5.6 mm, SM Pigtail
FPL1009S1550 nm100 mW400 mA1.4 V--Single Transverse ModeButterfly, SM Pigtail
FPL1009P1550 nm100 mW400 mA1.4 V--Single Transverse ModeButterfly, PM Pigtail
ULN15PC1550 nm140 mW650 mA3.0 V--Single FrequencyExtended Butterfly, PM Pigtail
ULN15PT1550 nm140 mW650 mA3.0 V--Single FrequencyExtended Butterfly, PM Pigtail
FPL1001C1550 nm150 mW400 mA1.4 V18°31°Single Transverse ModeChip on Submount
FPL1055T1550 nm300 mW (Pulsed)750 mA2 V15°28°Single Transverse ModeØ5.6 mm
FPL1055C1550 nm300 mW (Pulsed)750 mA2 V15°28°Single Transverse ModeChip on Submount
L1550G11550 nm1700 mW5 A1.5 V28°MultimodeØ9 mm
DFB15501555 nm100 mW (Min)1000 mA (Max)3.0 V--Single FrequencyButterfly, SM Pigtail
DFB1550N1555 nm130 mW (Min)1800 mA (Max)3.0 V--Single FrequencyButterfly, SM Pigtail
DFB1550P1555 nm100 mW (Min)1000 mA (Max)3.0 V--Single FrequencyButterfly, PM Pigtail
DFB1550PN1555 nm130 mW (Min)1800 mA (Max)3.0 V--Single FrequencyButterfly, PM Pigtail
L1570P5DFB1570 nm5 mW25 mA1.0 VSingle FrequencyØ5.6 mm
L1575G11575 nm1700 mW5 A1.5 V28°MultimodeØ9 mm
LPSC-1625-FC1625 nm50 mW350 mA1.5 V--Single Transverse ModeØ5.6 mm, SM Pigtail
FPL1054S1625 nm80 mW400 mA1.7 V--Single Transverse ModeButterfly, SM Pigtail
FPL1054P1625 nm80 mW400 mA1.7 V--Single Transverse ModeButterfly, PM Pigtail
FPL1054C1625 nm250 mW (Pulsed)750 mA2 V15°28°Single Transverse ModeChip on Submount
FPL1054T1625 nm200 mW (Pulsed)750 mA2 V15°28°Single Transverse ModeØ5.6 mm
DFB16421642 nm80 mW900 mA (Max)3.0 V--Single FrequencyButterfly, SM Pigtail
DFB1642P1642 nm80 mW900 mA (Max)3.0 V--Single FrequencyButterfly, PM Pigtail
DFB16461646 nm80 mW900 mA (Max)3.0 V--Single FrequencyButterfly, SM Pigtail
DFB1646P1646 nm80 mW900 mA (Max)3.0 V--Single FrequencyButterfly, PM Pigtail
FPL1059S1650 nm80 mW400 mA1.7 V--Single Transverse ModeButterfly, SM Pigtail
FPL1059P1650 nm80 mW400 mA1.7 V--Single Transverse ModeButterfly, PM Pigtail
DFB16501650 nm80 mW900 mA (Max)3.0 V--Single FrequencyButterfly, SM Pigtail
DFB1650P1650 nm80 mW900 mA (Max)3.0 V--Single FrequencyButterfly, PM Pigtail
FPL1059C1650 nm225 mW (Pulsed)750 mA2 V15°28°Single Transverse ModeChip on Submount
FPL1059T1650 nm225 mW (Pulsed)750 mA2 V15°28°Single Transverse ModeØ5.6 mm
DFB16541654 nm80 mW900 mA (Max)3.0 V--Single FrequencyButterfly, SM Pigtail
DFB1654P1654 nm80 mW900 mA (Max)3.0 V--Single FrequencyButterfly, PM Pigtail
FPL1940S1940 nm15 mW400 mA2 V--Single Transverse ModeButterfly, SM Pigtail
FPL2000S2 µm15 mW400 mA2 V--Single Transverse ModeButterfly, SM Pigtail
FPL2000C2 µm30 mW400 mA5.2 V19°Single Transverse ModeChip on Submount
ID3250HHLH3.00 - 3.50 µm (DFB)5 mW400 mA (Max)5 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
IF3400T13.40 µm (FP)30 mW300 mA4 V40°70°Single Transverse ModeØ9 mm
ID3750HHLH3.50 - 4.00 µm (DFB)5 mW300 mA (Max)5 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QF3850T13.85 µm (FP)200 mW600 mA (Max)13.5 V30°40°Single Transverse ModeØ9 mm
QF3850HHLH3.85 µm (FP)320 mW (Min)1100 mA (Max)13 V6 mrad (0.34°)6 mrad (0.34°)Single Transverse ModeHorizontal HHL
QF4040HHLH4.05 µm (FP)320 mW (Min)1100 mA (Max)13 V6 mrad (0.34°)6 mrad (0.34°)Single Transverse ModeHorizontal HHL
QD4500CM14.00 - 5.00 µm (DFB)40 mW500 mA (Max)10.5 V30°40°Single FrequencyTwo-Tab C-Mount
QD4500HHLH4.00 - 5.00 µm (DFB)80 mW500 mA (Max)11 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QF4050T24.05 µm (FP)70 mW250 mA12 V30°40°Single Transverse ModeØ9 mm
QF4050C24.05 µm (FP)300 mW400 mA12 V3042Single Transverse ModeTwo-Tab C-Mount
QF4050T14.05 µm (FP)300 mW600 mA (Max)12.0 V30°40°Single Transverse ModeØ9 mm
QF4050D24.05 µm (FP)800 mW750 mA13 V30°40°Single Transverse ModeD-Mount
QF4050D34.05 µm (FP)1200 mW1000 mA13 V30°40°Single Transverse ModeD-Mount
QD4472HH4.472 µm (DFB)85 mW500 mA (Max)11 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QF4600T24.60 µm (FP)200 mW500 mA (Max)13.0 V30°40°Single Transverse ModeØ9 mm
QF4600T14.60 µm (FP)400 mW800 mA (Max)12.0 V30°40°Single Transverse ModeØ9 mm
QF4600C24.60 µm (FP)600 mW600 mA12 V30°42°Single Transverse ModeTwo-Tab C-Mount
QF4600T34.60 µm (FP)1000 mW800 mA (Max)13 V30°40°Single Transverse ModeØ9 mm
QF4600D44.60 µm (FP)2500 mW1800 mA12.5 V40°30°Single Transverse ModeD-Mount
QF4600D34.60 µm (FP)3000 mW1700 mA12.5 V30°40°Single Transverse ModeD-Mount
QD4602HH4.602 µm (DFB)150 mW1000 mA (Max)12 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QF4650HHLH4.65 µm (FP)1500 mW (Min)1100 mA12 V6 mrad (0.34°)6 mrad (0.34°)Single Transverse ModeHorizontal HHL
QD5500CM15.00 - 6.00 µm (DFB)40 mW700 mA (Max)9.5 V30°45°Single FrequencyTwo-Tab C-Mount
QD5500HHLH5.00 - 6.00 µm (DFB)150 mW500 mA (Max)11 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QD5250C25.20 - 5.30 µm (DFB)60 mW700 mA (Max)9.5 V30°45°Single FrequencyTwo-Tab C-Mount
QD5263HH5.263 µm (DFB)130 mW1000 mA (Max)12 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QD6500CM16.00 - 7.00 µm (DFB)40 mW650 mA (Max)10 V35°50°Single FrequencyTwo-Tab C-Mount
QD6500HHLH6.00 - 7.00 µm (DFB)80 mW600 mA (Max)11 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QD6134HH6.134 µm (DFB)50 mW1000 mA (Max)12 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QD7500CM17.00 - 8.00 µm (DFB)40 mW600 mA (Max)10 V40°50°Single FrequencyTwo-Tab C-Mount
QD7500HHLH7.00 - 8.00 µm (DFB)50 mW700 mA (Max)12 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QD7500DM17.00 - 8.00 µm (DFB)100 mW600 mA (Max)11.5 V40°55°Single FrequencyD-Mount
QD7416HH7.416 µm (DFB)100 mW1000 mA (Max)12 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QD7716HH7.716 µm (DFB)30 mW1000 mA (Max)12 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QF7900HB7.9 µm (FP)700 mW1600 mA (Max)9 V6 mrad (0.34°)6 mrad (0.34°)Single Transverse ModeHorizontal HHL
QD7901HH7.901 µm (DFB)50 mW700 mA (Max)10 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QD8050CM18.00 - 8.10 µm (DFB)100 mW1000 mA (Max)9.5 V55°70°Single FrequencyTwo-Tab C-Mount
QD8500CM18.00 - 9.00 µm (DFB)100 mW900 mA (Max)9.5 V40°55°Single FrequencyTwo-Tab C-Mount
QD8500HHLH8.00 - 9.00 µm (DFB)100 mW600 mA (Max)10.2 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QF8450C28.45 µm (FP)300 mW750 mA9 V40°60°Single Transverse ModeTwo-Tab C-Mount
QF8500HB8.5 µm (FP)500 mW2000 mA (Max)9 V6 mrad (0.34°)6 mrad (0.34°)Single Transverse ModeHorizontal HHL
QD8650CM18.60 - 8.70 µm (DFB)50 mW900 mA (Max)9.5 V55°70°Single FrequencyTwo-Tab C-Mount
QD8912HH8.912 µm (DFB)150 mW1000 mA (Max)12 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QD9500CM19.00 - 10.00 µm (DFB)60 mW800 mA (Max)9.5 V40°55°Single FrequencyTwo-Tab C-Mount
QD9500HHLH9.00 - 10.00 µm (DFB)100 mW600 mA (Max)10.2 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QD9062HH9.062 µm (DFB)130 mW1000 mA (Max)12 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QF9150C29.15 µm (FP)200 mW850 mA11 V40°60°Single Transverse ModeTwo-Tab C-Mount
QF9200HB9.2 µm (FP)250 mW2000 mA (Max)9 V6 mrad (0.34°)6 mrad (0.34°)Single Transverse ModeHorizontal HHL
QF9500T19.5 µm (FP)300 mW550 mA12 V40°55°Single Transverse ModeØ9 mm
QD9550C29.50 - 9.60 µm (DFB)60 mW800 mA (Max)9.5 V40°55°Single FrequencyTwo-Tab C-Mount
QF9550CM19.55 µm (FP)80 mW1500 mA7.8 V35°60°Single Transverse ModeTwo-Tab C-Mount
QD9697HH9.697 µm (DFB)80 mW1000 mA (Max)12 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QD10500CM110.00 - 11.00 µm (DFB)40 mW600 mA (Max)10 V40°55°Single FrequencyTwo-Tab C-Mount
QD10500HHLH10.00 - 11.00 µm (DFB)50 mW700 mA (Max)12 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QD10530HH10.530 µm (DFB)50 mW1000 mA (Max)12 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QD10549HH10.549 µm (DFB)60 mW1000 mA (Max)12 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL
QD10622HH10.622 µm (DFB)60 mW1000 mA (Max)12 V6 mrad (0.34°)6 mrad (0.34°)Single FrequencyHorizontal HHL

The rows shaded green above denote single-frequency lasers.
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404 - 405 nm

Item # Info Wavelength
(nm)
Power
(mW)a,b
Typical/Max
Drive Currenta
Package Pin Code Monitor
Photodiodec
Compatible
Socket
Wavelength
Tested
Laser Mode
L404P400M info 404 400 370 mA / 410 mA Ø5.6 mm G No S7060R No Multimode
LP405-SF10 info 405 10 50 mA / 60 mA Ø5.6 mm, SM Pigtail B Yes S7060Rd Yes Single Transverse Mode
L405P20 info 405 20 38 mA / 55 mA Ø5.6 mm B Yes S7060R No Single Transverse Mode
LP405C1 info 405 30 75 mA / 110 mA Ø3.8 mm, SM Pigtail,
Collimator Output
G No S038Sd Yes Single Transverse Mode
L405G2e info 405 35 50 mA / 75 mA Ø3.8 mm G No S038S Yes Single Transverse Mode
DL5146-101S info 405 40 70 mA / 100 mA Ø5.6 mm B Yes S7060R No Single Transverse Mode
L405A1 info 405 175 (Min) 150 mA / 200 mA Ø5.6 mm A Yes S7060R No Single Transverse Mode
LP405-MF300 info 405 300 350 mA / 410 mA Ø5.6 mm, MM Pigtail G No S7060Rd Yes Multimode
L405G1 info 405 1000 900 mA / 1200 mA Ø9 mm G No S8060 No Multimode
  • Do not exceed the maximum optical power or maximum drive current, whichever occurs first.
  • Typical value unless otherwise noted.
  • Laser diodes with a built-in monitor photodiode can operate at constant power.
  • This socket is included with the purchase of the corresponding laser diode.
  • The L405G2 is tested to ensure a center wavelength tolerance of ±1 nm.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
L404P400M Support Documentation
L404P400M404 nm, 400 mW, Ø5.6 mm, G Pin Code, MM Laser Diode
$753.14
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Choose ItemLP405-SF10 Support Documentation
LP405-SF10405 nm, 10 mW, B Pin Code, SM Fiber-Pigtailed Laser Diode, FC/PC
$721.06
Today
L405P20 Support Documentation
L405P20405 nm, 20 mW, Ø5.6 mm, B Pin Code, Laser Diode
$58.21
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Choose ItemLP405C1 Support Documentation
LP405C1405 nm, 30 mW, G Pin Code, SM Fiber-Pigtailed Laser Diode, Collimator Output
$1,229.51
Today
L405G2 Support Documentation
L405G2405 nm, 35 mW, Ø3.8 mm, G Pin Code, Laser Diode
$104.93
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DL5146-101S Support Documentation
DL5146-101S405 nm, 40 mW, Ø5.6 mm, B Pin Code Laser Diode
$95.93
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L405A1 Support Documentation
L405A1405 nm, 175 mW, Ø5.6 mm, A Pin Code, Laser Diode
$805.23
Today
Choose ItemLP405-MF300 Support Documentation
LP405-MF300405 nm, 300 mW, G Pin Code, Ø50 µm MM Fiber-Pigtailed Laser Diode, FC/PC
$943.21
Today
L405G1 Support Documentation
L405G1405 nm, 1000 mW, Ø9 mm, G Pin Code, MM Laser Diode
$780.30
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450 - 488 nm

Item # Info Wavelength
(nm)
Power
(mW)a,b
Typical/Max
Drive Currenta
Package Pin
Code
Monitor
Photodiodec
Compatible
Socket
Wavelength
Tested
Laser Mode
LP450-SF25 info 450 25 75 mA / 140 mA Ø5.6 mm, SM Pigtail G No S7060Rd Yes Single Transverse Mode
L450G3 info 450 100 (Min) 80 mA / 110 mA Ø3.8 mm G No S038S No Single Transverse Mode
L450G2 info 450 100 (Min) 80 mA / 110 mA Ø5.6 mm G No S7060R No Single Transverse Mode
L450P1600MM info 450 1600 1200 mA / 1500 mA Ø5.6 mm G No S7060R No Multimode
L473P100 info 473 100 120 mA / 150 mA Ø5.6 mm F+e Yes - No Single Transverse Mode
LP488-SF20 info 488 20 85 mA / 110 mA Ø5.6 mm, SM Pigtail B Yes S7060Rd Yes Single Transverse Mode
LP488-SF20G info 488 20 80 mA / 120 mA Ø5.6 mm, SM Pigtail G No S7060Rd Yes Single Transverse Mode
L488P60 info 488 60 75 mA / 110 mA Ø5.6 mm B Yes S7060R No Single Transverse Mode
  • Do not exceed the maximum optical power or maximum drive current, whichever occurs first.
  • Typical value unless otherwise noted.
  • Laser diodes with a built-in monitor photodiode can operate at constant power.
  • This socket is included with the purchase of the corresponding laser diode.
  • This laser diode has a built in Zener diode to help protect against damage from small levels of electrostatic discharge and reverse potential on the laser diode. A temperature-controlled mount such as our LDM56F(/M) or LDM90(/M) is recommended for general use.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
Choose ItemLP450-SF25 Support Documentation
LP450-SF25Customer Inspired! 450 nm, 25 mW, G Pin Code, SM Fiber-Pigtailed Laser Diode, FC/PC
$795.60
Today
L450G3 Support Documentation
L450G3450 nm, 100 mW, Ø3.8 mm, G Pin Code, Laser Diode
$138.57
Today
L450G2 Support Documentation
L450G2450 nm, 100 mW, Ø5.6 mm, G Pin Code, Laser Diode
$126.90
Today
L450P1600MM Support Documentation
L450P1600MM450 nm, 1600 mW, Ø5.6 mm, G Pin Code, MM, Laser Diode
$94.74
Today
L473P100 Support Documentation
L473P100473 nm, 100 mW, Ø5.6 mm, F+ Pin Code, Laser Diode
$3,032.68
Today
Choose ItemLP488-SF20 Support Documentation
LP488-SF20488 nm, 20 mW, B Pin Code, SM Fiber-Pigtailed Laser Diode, FC/PC
$3,401.03
Today
Choose ItemLP488-SF20G Support Documentation
LP488-SF20G488 nm, 20 mW, G Pin Code, SM Fiber-Pigtailed Laser Diode, FC/PC
$916.64
Today
L488P60 Support Documentation
L488P60488 nm, 60 mW, Ø5.6 mm, B Pin Code, Laser Diode
$2,793.99
Today
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515 - 520 nm

Item # Info Wavelength
(nm)
Power
(mW)a,b
Typical/Max
Drive Currenta
Package Pin Code Monitor
Photodiodec
Compatible
Socket
Wavelength
Tested
Laser Mode
LP515-SF3 info 515 3 50 mA / 100 mA Ø5.6 mm, SM Pigtail A Yes S7060Rd Yes Single Transverse Mode
L515A1 info 515 10 50 mA / 100 mA Ø5.6 mm A Yes S7060R No Single Transverse Mode
LP520-SF15A info 520 15 100 mA / 160 mA Ø5.6 mm, SM Pigtail A Yes S7060Rd Yes Single Transverse Mode
L520A1 info 520 30 (Min) 80 mA / 100 mA Ø5.6 mm A No S7060R No Single Transverse Mode
PL520 info 520 50 150 mA / 160 mA Ø3.8 mm G No S038S No Single Transverse Mode
L520P50 info 520 50 150 mA / 160 mA Ø5.6 mm A Yes S7060R No Single Transverse Mode
L520A2 info 520 110 (Min) 225 mA / 330 mA Ø5.6 mm A No S7060R No Single Transverse Mode
  • Do not exceed the maximum optical power or maximum drive current, whichever occurs first.
  • Typical value unless otherwise noted.
  • Laser diodes with a built-in monitor photodiode can operate at constant power.
  • This socket is included with the purchase of the corresponding laser diode.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
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Choose ItemLP515-SF3 Support Documentation
LP515-SF3515 nm, 3 mW, A Pin Code, SM Fiber-Pigtailed Laser Diode, FC/PC
$474.90
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L515A1 Support Documentation
L515A1515 nm, 10 mW, Ø5.6 mm, A Pin Code, Laser Diode
$30.68
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Choose ItemLP520-SF15A Support Documentation
LP520-SF15A520 nm, 15 mW, A Pin Code, SM Fiber-Pigtailed Laser Diode, FC/PC
$811.26
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L520A1 Support Documentation
L520A1520 nm, 30 mW, Ø5.6 mm, A Pin Code, Laser Diode
$76.29
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PL520 Support Documentation
PL520520 nm, 50 mW, Ø3.8 mm, G Pin Code Laser Diode
$89.69
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L520P50 Support Documentation
L520P50520 nm, 50 mW, Ø5.6 mm, A Pin Code, Laser Diode
$76.61
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L520A2 Support Documentation
L520A2520 nm, 110 mW, Ø5.6 mm, A Pin Code, Laser Diode
$155.40
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532 nm

Item # Info Wavelength
(nm)
Power
(mW)a
Typical/Max
Drive Currenta
Package Pin Code Monitor
Photodiode
Compatible
Socket
Wavelength
Tested
Laser Mode
DJ532-10b info 532 10 220 mA / 250 mA Ø9.5 mm (non-standard)c A Yesd - No Single Transverse Mode
DJ532-40b info 532 40 330 mA / 400 mA Ø9.5 mm (non-standard)c E No - No Single Transverse Mode
  • Do not exceed the maximum optical power or maximum drive current, whichever occurs first.
  • Click here for more information on our 532 nm Diode Pumped Solid State Lasers.
  • These lasers have the same pin spacing as our Ø5.6 mm laser diodes. They are compatible with the LDM56 Laser Diode Mount using the LDM56DJ DPSS Laser Mounting Flange.
  • The monitor photodiode of the DJ532-10 measures the power of the pump source, not the 532 nm output. Therefore, we recommend operating these diodes in constant current mode.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
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DJ532-10 Support Documentation
DJ532-10532 nm, 10 mW, A Pin Code, DPSS Laser
$175.81
Today
DJ532-40 Support Documentation
DJ532-40532 nm, 40 mW, E Pin Code, DPSS Laser
$212.64
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633 - 635 nm

Item # Info Wavelength
(nm)
Power
(mW)a
Typical/Max
Drive Currenta
Package Pin
Code
Monitor
Photodiodeb
Compatible
Socket
Wavelength
Tested
Laser Mode
LP633-SF50 info 633 50 170 mA / 210 mA Ø5.6 mm SM Pigtail, FC/PC G No S7060Rc Yes Single Transverse Mode
HL63163DG info 633 100 170 mA / 230 mA Ø5.6 mm G No S7060R No Single Transverse Mode
LPS-635-FC info 635 2.5 70 mA / 95 mA Ø9 mm, SM Pigtail A Yes S8060 or S8060-4 Yes Single Transverse Mode
LPS-PM635-FC info 635 2.5 60 mA / 95 mA Ø9.0 mm, PM Pigtaild A Yes S8060 or S8060-4 Yes Single Transverse Mode
L635P5 info 635 5 30 mA / 45 mA Ø5.6 mm A Yes S7060R No Single Transverse Mode
HL6312G info 635 5 50 mA / 85 mA Ø9 mm A Yes S8060 or S8060-4 No Single Transverse Mode
LPM-635-SMA info 635 7.5 70 mA / 95 mA Ø9 mm, MM Pigtail A Yes S8060 or S8060-4 Yes Multimodee
LP635-SF8 info 635 8 85 mA / 100 mA Ø5.6 mm, SM Pigtail A Yes S7060Rc Yes Single Transverse Mode
HL6320G info 635 10 60 mA / 95 mA Ø9 mm A Yes S8060 or S8060-4 No Single Transverse Mode
HL6322G info 635 15 75 mA / 100 mA Ø9 mm A Yes S8060 or S8060-4 No Single Transverse Mode
  • Do not exceed the maximum optical power or maximum drive current, whichever occurs first.
  • Laser diodes with a built-in monitor photodiode can operate at constant power.
  • This socket is included with the purchase of the corresponding laser diode.
  • The slow axis of the polarization-maintaining fiber is aligned to the connector key.
  • This pigtail has a single mode laser diode and multimode fiber pigtail, which together produce a multimode output.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
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Choose ItemLP633-SF50 Support Documentation
LP633-SF50633 nm, 50 mW, G Pin Code, SM Fiber-Pigtailed Laser Diode, FC/PC
$960.82
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HL63163DG Support Documentation
HL63163DG633 nm, 100 mW, Ø5.6 mm, G Pin Code, Laser Diode
$337.37
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Choose ItemLPS-635-FC Support Documentation
LPS-635-FC635 nm, 2.5 mW, A Pin Code, SM Fiber-Pigtailed Laser Diode, FC/PC
$432.41
Today
Choose ItemLPS-PM635-FC Support Documentation
LPS-PM635-FC635 nm, 2.5 mW, A Pin Code, PM Fiber-Pigtailed Laser Diode, FC/PC
$1,076.26
Today
L635P5 Support Documentation
L635P5635 nm, 5 mW, Ø5.6 mm, A Pin Code, Laser Diode
$27.67
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HL6312G Support Documentation
HL6312G635 nm, 5 mW, Ø9 mm, A Pin Code, Laser Diode
$24.94
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Choose ItemLPM-635-SMA Support Documentation
LPM-635-SMA635 nm, 7.5 mW, A Pin Code, Ø62.5 µm MM Fiber-Pigtailed Laser Diode, SMA905
$477.54
Today
Choose ItemLP635-SF8 Support Documentation
LP635-SF8635 nm, 8.0 mW, A Pin Code, SM Fiber-Pigtailed Laser Diode, FC/PC
$711.56
Today
HL6320G Support Documentation
HL6320G635 nm, 10 mW, Ø9 mm, A Pin Code, Laser Diode
$47.24
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HL6322G Support Documentation
HL6322G635 nm, 15 mW, Ø9 mm, A Pin Code, Laser Diode
$79.00
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637 - 639 nm

Item # Info Wavelength
(nm)
Power
(mW)a
Typical/Max
Drive Currenta
Package Pin Code Monitor
Photodiodeb
Compatible
Socket
Wavelength
Tested
Laser Mode
L637P5 info 637 5 20 mA / 25 mA Ø5.6 mm C Yes S7060R No Single Transverse Mode
LP637-SF50 info 637 50 140 mA / 180 mA Ø5.6 mm, SM Pigtail A Yes S7060Rc Yes Single Transverse Mode
LP637-SF70 info 637 70 220 mA / 300 mA Ø5.6 mm, SM Pigtail G No S7060Rc Yes Single Transverse Mode
HL63142DG info 637 100 140 mA / 180 mA Ø5.6 mm A Yes S7060R No Single Transverse Mode
HL63133DG info 637 170 250 mA / 320 mA Ø5.6 mm G No S7060R No Single Transverse Mode
HL6388MG info 637 250 340 mA / 430 mA Ø5.6 mm H No S7060R No Multimode
L637G1 info 637 1200 1100 mA / 1500 mA Ø9 mmd G No Customd No Multimode
L638P040 info 638 40 92 mA / 115 mA Ø5.6 mm A Yes S7060R No Single Transverse Mode
L638P150 info 638 150 230 mA / 300 mA Ø3.8 mm G No S038S No Single Transverse Mode
L638P200 info 638 200 280 mA / 330 mA Ø5.6 mm G No S7060R No Single Transverse Mode
L638P700M info 638 700 820 mA / 1000 mA Ø5.6 mm G No S7060R No Multimode
HL6358MG info 639 10 40 mA / 50 mA Ø5.6 mm A Yes S7060R No Single Transverse Mode
HL6323MG info 639 30 100 mA / 130 mA Ø5.6 mm A Yes S7060R No Single Transverse Mode
  • Do not exceed the maximum optical power or maximum drive current, whichever occurs first.
  • Laser diodes with a built-in monitor photodiode can operate at constant power.
  • This socket is included with the purchase of the corresponding laser diode.
  • A socket is included to assist with soldering. The leads on this diode have a larger 0.6 mm diameter than the typical 0.45 mm diameter for a Ø9 mm package. This makes it incompatible with mounts and sockets that are designed to fit a standard Ø9 mm TO can package.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
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L637P5 Support Documentation
L637P5Customer Inspired! 637 nm, 5 mW, Ø5.6 mm, C Pin Code, Laser Diode
$15.68
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Choose ItemLP637-SF50 Support Documentation
LP637-SF50637 nm, 50 mW, A Pin Code, SM Fiber-Pigtailed Laser Diode, FC/PC
$890.94
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Choose ItemLP637-SF70 Support Documentation
LP637-SF70637 nm, 70 mW, G Pin Code, SM Fiber-Pigtailed Laser Diode, FC/PC
$866.00
Today
HL63142DG Support Documentation
HL63142DG637 nm, 100 mW, Ø5.6 mm, A Pin Code, Laser Diode
$321.92
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HL63133DG Support Documentation
HL63133DG637 nm, 170 mW, Ø5.6 mm, G Pin Code, Laser Diode
$190.07
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HL6388MG Support Documentation
HL6388MG637 nm, 250 mW, Ø5.6 mm, H Pin Code, MM, Laser Diode
$65.93
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L637G1 Support Documentation
L637G1637 nm, 1200 mW, Ø9 mm, G Pin Code, MM, Laser Diode
$178.09
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L638P040 Support Documentation
L638P040638 nm, 40 mW, Ø5.6 mm, A Pin Code, Laser Diode
$112.85
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L638P150 Support Documentation
L638P150638 nm, 150 mW, Ø3.8 mm, G Pin Code, Laser Diode
$54.74
Today
L638P200 Support Documentation
L638P200638 nm, 200 mW, Ø5.6 mm, G Pin Code, Laser Diode
$153.73
Today
L638P700M Support Documentation
L638P700M638 nm, 700 mW, Ø5.6 mm, G Pin Code, MM, Laser Diode
$72.17
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HL6358MG Support Documentation
HL6358MG639 nm, 10 mW, Ø5.6 mm, A Pin Code, Laser Diode
$17.94
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HL6323MG Support Documentation
HL6323MG639 nm, 30 mW, Ø5.6 mm, A Pin Code, Laser Diode
$150.87
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640 - 642 nm

Item # Info Wavelength
(nm)
Power
(mW)a
Typical/Max
Drive Currenta
Package Pin Code Monitor
Photodiodeb
Compatible
Socket
Wavelength
Tested
Laser Mode
HL6362MG info 640 40 90 mA / 110 mA Ø5.6 mm A Yes S7060R No Single Transverse Mode
LP642-SF20 info 642 20 90 mA / 140 mA Ø5.6 mm, SM Pigtail A Yes S7060Rc Yes Single Transverse Mode
LP642-PF20 info 642 20 110 mA / 150 mA Ø5.6 mm, PM Pigtaild A Yes S7060Rc Yes Single Transverse Mode
HL6364DG info 642 60 120 mA / 155 mA Ø5.6 mm A Yes S7060R No Single Transverse Mode
HL6366DG info 642 80 150 mA / 175 mA Ø5.6 mm A Yes S7060R No Single Transverse Mode
HL6385DG info 642 150 250 mA / 350 mA Ø5.6 mm H No S7060R No Single Transverse Mode
  • Do not exceed the maximum optical power or maximum drive current, whichever occurs first.
  • Laser diodes with a built-in monitor photodiode can operate at constant power.
  • This socket is included with the purchase of the corresponding laser diode.
  • The slow axis of the polarization-maintaining fiber is aligned to the connector key.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
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HL6362MG Support Documentation
HL6362MG640 nm, 40 mW, Ø5.6 mm, A Pin Code, Laser Diode
$136.61
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Choose ItemLP642-SF20 Support Documentation
LP642-SF20642 nm, 20 mW, A Pin Code, SM Fiber-Pigtailed Laser Diode, FC/PC
$669.03
Today
Choose ItemLP642-PF20 Support Documentation
LP642-PF20642 nm, 20 mW, A Pin Code, PM Fiber-Pigtailed Laser Diode, FC/PC
$1,028.74
Today
HL6364DG Support Documentation
HL6364DG642 nm, 60 mW, Ø5.6 mm, A Pin Code, Laser Diode
$180.56
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HL6366DG Support Documentation
HL6366DG642 nm, 80 mW, Ø5.6 mm, A Pin Code, Laser Diode
$229.27
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HL6385DG Support Documentation
HL6385DG642 nm, 150 mW, Ø5.6 mm, H Pin Code, Laser Diode
$356.39
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650 - 658 nm

Item # Info Wavelength
(nm)
Power
(mW)a
Typical/Max
Drive Currenta
Package Pin Code Monitor
Photodiodeb
Compatible
Socket
Wavelength
Tested
Laser Mode
L650P007 info 650 7 28 mA / 35 mA Ø5.6 mm A Yes S7060R No Single Transverse Mode
LPS-660-FC info 658 7.5 65 mA / 95 mA Ø5.6 mm, SM Pigtail C Yes S7060Rc Yes Single Transverse Mode
LP660-SF20 info 658 20 80 mA / 110 mA Ø5.6 mm, SM Pigtail A Yes S7060Rc Yes Single Transverse Mode
LPM-660-SMA info 658 22.5 65 mA / 95 mA Ø5.6 mm, MM Pigtail C Yes S7060Rc Yes Multimoded
HL6501MG info 658 30 75 mA / 120 mA Ø5.6 mm C Yes S7060R No Single Transverse Mode
L658P040 info 658 40 75 mA / 110 mA Ø5.6 mm A Yes S7060R No Single Transverse Mode
LP660-SF40 info 658 40 135 mA / 170 mA Ø5.6 mm, SM Pigtail H No S7060Rc Yes Single Transverse Mode
LP660-SF60 info 658 60 210 mA / 250 mA Ø5.6 mm, SM Pigtail H No S7060Rc Yes Single Transverse Mode
  • Do not exceed the maximum optical power or maximum drive current, whichever occurs first.
  • Laser diodes with a built-in monitor photodiode can operate at constant power.
  • This socket is included with the purchase of the corresponding laser diode.
  • This pigtail has a single mode laser diode and multimode fiber pigtail, which together produce a multimode output.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
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L650P007 Support Documentation
L650P007650 nm, 7 mW, Ø5.6 mm, A Pin Code, Laser Diode
$15.08
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Choose ItemLPS-660-FC Support Documentation
LPS-660-FC658 nm, 7.5 mW, C Pin Code, SM Fiber-Pigtailed Laser Diode, FC/PC
$459.43
Today
Choose ItemLP660-SF20 Support Documentation
LP660-SF20658 nm, 20 mW, A Pin Code, SM Fiber-Pigtailed Laser Diode, FC/PC
$509.39
Today
Choose ItemLPM-660-SMA Support Documentation
LPM-660-SMA658 nm, 22.5 mW, C Pin Code, Ø62.5 µm MM Fiber-Pigtailed Laser Diode, SMA905
$435.97
Today
HL6501MG Support Documentation
HL6501MG658 nm, 30 mW, Ø5.6 mm, C Pin Code, Laser Diode
$28.63
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L658P040 Support Documentation
L658P040658 nm, 40 mW, Ø5.6 mm, A Pin Code, Laser Diode
$31.77
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Choose ItemLP660-SF40 Support Documentation
LP660-SF40658 nm, 40 mW, H Pin Code, SM Fiber-Pigtailed Laser Diode, FC/PC
$721.06
Today
Choose ItemLP660-SF60 Support Documentation
LP660-SF60658 nm, 60 mW, H Pin Code, SM Fiber-Pigtailed Laser Diode, FC/PC
$781.65
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660 nm

Item # Info Wavelength
(nm)
Power
(mW)a
Typical/Max
Drive Currenta
Package Pin Code Monitor
Photodiodeb
Compatible
Socket
Wavelength
Tested
Laser Mode
HL6544FM info 660 50 115 mA / 135 mA Ø5.6 mm G No S7060R No Single Transverse Mode
LP660-SF50 info 660 50 140 mA / 200 mA Ø5.6 mm SM Pigtail, FC/PC C Yes S7060Rc Yes Single Transverse Mode
HL6545MG info 660 120 170 mA / 210 mA Ø5.6 mm H No S7060R No Single Transverse Mode
L660P120 info 660 120 175 mA / 210 mA Ø5.6 mm C Yes S7060R No Single Transverse Mode
  • Do not exceed the maximum optical power or maximum drive current, whichever occurs first.
  • Laser diodes with a built-in photodiode can operate at constant power.
  • This socket is included with the purchase of the corresponding laser diode.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
HL6544FM Support Documentation
HL6544FM660 nm, 50 mW, Ø5.6 mm, G Pin Code, Laser Diode
$38.91
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Choose ItemLP660-SF50 Support Documentation
LP660-SF50660 nm, 50 mW, C Pin Code, SM Fiber-Pigtailed Laser Diode, FC/PC
$797.77
Today
HL6545MG Support Documentation
HL6545MG660 nm, 120 mW, Ø5.6 mm, H Pin Code, Laser Diode
$51.09
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L660P120 Support Documentation
L660P120660 nm, 120 mW, Ø5.6 mm, C Pin Code, Laser Diode
$116.73
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670 nm

Item # Info Wavelength
(nm)
Power
(mW)a
Typical/Max
Drive Currenta
Package Pin Code Monitor
Photodiodeb
Compatible
Socket
Wavelength
Tested
Laser Mode
L670VH1 info 670 1 2.5 mA / 2.8 mA TO-46 H No S8060 Yesc Single Transverse Mode
LPS-675-FC info 670 2.5 55 mA / 90 mA Ø9 mm, SM Pigtail A Yes S8060 or S8060-4 Yes Single Transverse Mode
HL6748MG info 670 10 30 mA / 45 mA Ø5.6 mm A Yes S7060R No Single Transverse Mode
HL6714G info 670 10 55 mA / 90 mA Ø9 mm A Yes S8060 or S8060-4 No Single Transverse Mode
HL6756MG info 670 15 35 mA / 45 mA Ø5.6 mm A Yes S7060R No Single Transverse Mode
  • Do not exceed the maximum optical power or maximum drive current, whichever occurs first.
  • Laser diodes with a built-in photodiode can operate at constant power.
  • The L670VH1 is tested to ensure a center wavelength tolerance of ±10 nm.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
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L670VH1 Support Documentation
L670VH1670 nm, 1 mW, TO-46, H Pin Code, VCSEL Diode
$164.67
Today
Choose ItemLPS-675-FC Support Documentation
LPS-675-FC670 nm, 2.5 mW, A Pin Code, SM Fiber-Pigtailed Laser Diode, FC/PC
$540.50
Today
HL6748MG Support Documentation
HL6748MG670 nm, 10 mW, Ø5.6 mm, A Pin Code, Laser Diode
$31.19
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HL6714G Support Documentation
HL6714G670 nm, 10 mW, Ø9 mm, A Pin Code, Laser Diode
$59.11
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HL6756MG Support Documentation
HL6756MG670 nm, 15 mW, Ø5.6 mm, A Pin Code, Laser Diode
$70.69
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685 nm

Item # Info Wavelength
(nm)
Power
(mW)a
Typical/Max
Drive Currenta
Package Pin Code Monitor
Photodiodeb
Compatible
Socket
Wavelength
Tested
Laser Mode
LP685-SF15 info 685 15 55 mA / 80 mA Ø5.6 mm, SM Pigtail C Yes S7060Rc Yes Single Transverse Mode
HL6750MG info 685 50 70 mA / 120 mA Ø5.6 mm C Yes S7060R No Single Transverse Mode
  • Do not exceed the maximum optical power or maximum drive current, whichever occurs first.
  • Laser diodes with a built-in monitor photodiode can operate at constant power.
  • This socket is included with the purchase of the corresponding laser diode.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
Choose ItemLP685-SF15 Support Documentation
LP685-SF15685 nm, 15 mW, C Pin Code, SM Fiber-Pigtailed Laser Diode, FC/PC
$622.48
Today
HL6750MG Support Documentation
HL6750MG685 nm, 50 mW, Ø5.6 mm, C Pin Code, Laser Diode
$93.24
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690 nm

Item # Info Wavelength
(nm)
Power
(mW)a
Typical/Max
Drive Currenta
Package Pin Code Monitor
Photodiodeb
Compatible
Socket
Wavelength
Tested
Laser Mode
HL6738MG info 690 30 85 mA / 115 mA Ø5.6 mm C Yes S7060R No Single Transverse Mode
  • Do not exceed the maximum optical power or maximum drive current, whichever occurs first.
  • Laser diodes with a built-in photodiode can operate at constant power.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
HL6738MG Support Documentation
HL6738MG690 nm, 30 mW, Ø5.6 mm, C Pin Code, Laser Diode
$56.43
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