Volume-Holographic-Grating- (VHG) Stabilized SF Lasers, TO Cans


  • 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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info icon Clicking this icon opens a window that contains specifications and mechanical drawings.
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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

  • 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 (info icon) 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
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
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:

DBR Equation

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
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
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
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 #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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785 nm VHG-Stabilized Laser Diode, Ø9 mm TO Can Package

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
LD785-SEV300c info 785 nm 300 mW 500 mA E Ø9 mm TO Cand No S8060 or
S8060-4
Yes Single
Frequencye
LDM90(/M) LDC205Cf
  • Do not exceed the maximum optical power or maximum drive current, whichever occurs first.
  • The power can be tuned across the operating current range, given in the serial-number-specific documentation, while maintaining wavelength-stabilized, single-frequency performance within a stabilized temperature range.
  • In order to achieve the specified performance, we recommend using the LDM90(/M) Laser Diode Mount and, when collimated, an NIR Optical Isolator; single frequency performance when collimated is only guaranteed with >35 dB isolation of back reflections.
  • The Ø9 mm package for the LD785-SEV300 is 4.30 mm (0.17") thick, which is more than the standard Ø9 mm package thickness of 1.50 mm (0.06"). The diode will still function with all Ø9 mm laser diode mounts; please see the Drawing tab in the blue info icon (info) above for full package specifications. Mounting this diode in the LDM90(/M) mount requires two 2-56 screws, included with this diode.
  • Single Longitudinal Mode and Single Transverse Mode
  • We recommend using the LDC205C current controller in conjunction with one of Thorlabs' temperature controllers, such as the TED200C.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
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Choose ItemLD785-SEV300 Support Documentation
LD785-SEV300Customer Inspired! 785 nm, 300 mW, Ø9 mm TO Can, E Pin Code, VHG Wavelength-Stabilized Single-Frequency Laser Diode
$1,640.53
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808 nm VHG-Stabilized Laser Diode, Ø9 mm TO Can Package

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
LD808-SEV500c info 808 nm 500 mW 800 mA E Ø9 mm TO Cand No S8060 or
S8060-4
Yes Single
Frequencye
LDM90(/M) ITC4001f
  • Do not exceed the maximum optical power or maximum drive current, whichever occurs first.
  • Within the stabilized temperature range, the laser can be tuned across the operating current range while maintaining wavelength-stabilized, single-frequency performance. The stabilized temperature and operating current range are provided for each unit in the serial-number-specific documentation.
  • In order to achieve the specified performance, we recommend using the LDM90(/M) Laser Diode Mount and, when collimated, an NIR Optical Isolator; single frequency performance when collimated is only guaranteed with >35 dB isolation of back reflections.
  • The Ø9 mm package for the LD808-SEV500 is 4.30 mm (0.17") thick, which is more than the standard Ø9 mm package thickness of 1.50 mm (0.06"). The diode will still function with all Ø9 mm laser diode mounts; please see the Drawing tab in the blue info icon (info) above for full package specifications. Mounting this diode in the LDM90(/M) mount requires two 2-56 screws, included with this diode.
  • Single Longitudinal Mode and Single Transverse Mode
  • We recommend using the ITC4001 current and temperature controller with the noise reduction filter enabled.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
Choose ItemLD808-SEV500 Support Documentation
LD808-SEV500808 nm, 500 mW, Ø9 mm TO Can, E Pin Code, VHG Wavelength-Stabilized Single-Frequency Laser Diode
$1,761.69
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852 nm VHG-Stabilized Laser Diode, Ø9 mm TO Can Package

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 info 852 nm 270 mW 400 mA E Ø9 mm TO Cand No S8060 or
S8060-4
Yes Single
Frequencye
LDM90(/M) ITC4001f
LD852-SEV600c info 852 nm 600 mW 1050 mA E Ø9 mm TO Cand No S8060 or
S8060-4
Yes Single
Frequencye
LDM90(/M) ITC4001f
  • Do not exceed the maximum optical power or maximum drive current, whichever occurs first.
  • Within the stabilized temperature range, the laser can be tuned across the operating current range while maintaining wavelength-stabilized, single-frequency performance. The stabilized temperature and operating current range are provided for each unit in the serial-number-specific documentation.
  • In order to achieve the specified performance, we recommend using the LDM90(/M) Laser Diode Mount and, when collimated, an NIR Optical Isolator; single frequency performance when collimated is only guaranteed with >35 dB isolation of back reflections.
  • The Ø9 mm package for the L852SEV1 and LD852-SEV600 is 4.30 mm (0.17") thick, which is more than the standard Ø9 mm package thickness of 1.50 mm (0.06"). The diodes will still function with all Ø9 mm laser diode mounts; please see the Drawing tab in the blue info icons (info) above for full package specifications. Mounting these diodes in the LDM90(/M) mount requires two 2-56 screws, included with each diode.
  • Single Longitudinal Mode and Single Transverse Mode
  • We recommend using the ITC4001 current and temperature controller with the noise reduction filter enabled.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
Choose ItemL852SEV1 Support Documentation
L852SEV1852 nm, 270 mW, Ø9 mm TO Can, E Pin Code, VHG Wavelength-Stabilized Single-Frequency Laser Diode
$1,000.00
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Choose ItemLD852-SEV600 Support Documentation
LD852-SEV600852 nm, 600 mW, Ø9 mm TO Can, E Pin Code, VHG Wavelength-Stabilized Single-Frequency Laser Diode
$1,761.69
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976 nm VHG-Stabilized Laser Diode, Ø9 mm TO Can Package

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
L976SEV1c info 976 nm 270 mW 400 mA E Ø9 mm TO Cand No S8060 or
S8060-4
Yes Single
Frequencye
LDM90(/M) ITC4001f
  • Do not exceed the maximum optical power or maximum drive current, whichever occurs first.
  • Within the stabilized temperature range, the laser can be tuned across the operating current range while maintaining wavelength-stabilized, single-frequency performance. The stabilized temperature and operating current range are provided for each unit in the serial-number-specific documentation.
  • In order to achieve the specified performance, we recommend using the LDM90(/M) Laser Diode Mount and, when collimated, an NIR Optical Isolator; single frequency performance when collimated is only guaranteed with >35 dB isolation of back reflections.
  • The Ø9 mm package for the L976SEV1 is 4.30 mm (0.17") thick, which is more than the standard Ø9 mm package thickness of 1.50 mm (0.06"). The diode will still function with all Ø9 mm laser diode mounts; please see the Drawing tab in the blue info icon (info) above for full package specifications. Mounting this diode in the LDM90(/M) mount requires two 2-56 screws, included with this diode.
  • Single Longitudinal Mode and Single Transverse Mode
  • We recommend using the ITC4001 current and temperature controller with the noise reduction filter enabled.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
Choose ItemL976SEV1 Support Documentation
L976SEV1976 nm, 270 mW, Ø9 mm TO Can, E Pin Code, VHG Wavelength-Stabilized Single-Frequency Laser Diode
$1,530.00
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