Volume-Holographic-Grating- (VHG) Stabilized SF Lasers, TO Can Pigtail
- 785 nm VHG-Stabilized Laser Diode
- Wavelength-Stabilized Output Over Operating Temperature Range
- SM Fiber Pigtail Package with FC/APC Connector
785 nm, 50 mW, SM Pigtail
This high-resolution optical spectrum was obtained using one of Thorlabs’ Optical Spectrum Analyzers (OSA201C), which provides 8 pm resolution at 785 nm.
|Clicking this icon opens a window that contains specifications and mechanical drawings.|
|Clicking this icon allows you to download our standard support documentation.|
|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.|
- 785 nm Center Wavelength
- Wavelength-Stabilized Output
- Narrow 10 MHz Typical Linewidth (CW)
- Pigtailed Single Mode Optical Fiber with FC/APC Connector (2.0 mm Narrow Key)
- Integrated Optical Isolator to Protect Against Back Reflections
- Raman Spectroscopy
Thorlabs' Volume-Holographic-Grating- (VHG) Stabilized Laser is a laser diode that uses feedback from a volume holographic grating to provide narrow-linewidth, single-frequency operation. This allows this laser to achieve 10 MHz typical linewidths with an excellent side mode suppression ratio (40 dB typical). Typical performance graphs can be viewed by clicking on the blue icon () in the table below. More information on the stabilized temperature range can be found on the individualized data sheet for each laser diode.
The LP785-SAV50 VHG-stabilized laser incorporates an E-pin code and is pigtailed to an FC/APC-terminated fiber. It has an internal optical isolator and FC/APC connector which provide protection against back reflections that could de-stabilize the laser performance. We also offer VHG-stabilized lasers in pigtailed butterfly and unmounted Ø9 mm TO can packages.
While the center wavelength is listed for the laser diodes 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 a pigtailed distributed feedback (DFB) single-frequency laser and external cavity and distributed bragg reflector (DBR) butterfly-packaged single-frequency lasers. The DFB lasers provide similar linewidths to the VHG-stablized lasers, but provide a mode-hop-free tuning of several nanometers while maintaining single-frequency operation. The butterfly-packaged external cavity lasers offer a narrower linewidth and more center wavelength options than our VHG-stabilized lasers. 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.
We recommend cleaning the fiber connector of the pigtail package 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 connector on this pigtailed laser diode is cleaned and capped before shipping, we cannot guarantee that they will remain free of contamination after it is removed from the package. We also recommend that the laser is turned off when connecting or disconnecting the device from other fibers.
ECL, DFB, VHG-Stabilized, DBR, and Hybrid Single-Frequency Lasers
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. In addition, these methods can be combine to form hybrid laser designs. 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). In addition, these methods can be combine to form hybrid laser designs. We discuss below some of the main differences between 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 (<1 MHz). 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.
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 and MIR) incorporates the grating within the laser diode structure itself (see Figure 2). This corrugated periodic structure coupled closely to the active region acts as a Bragg reflector, selecting a single longitudinal mode as the lasing mode. If the active region has enough gain at frequencies near the Bragg frequency, an end reflector is unnecessary, relying instead upon the Bragg reflector for all optical feedback and mode selection. Due to this “built-in” selection, a DFB can achieve single-frequency operation over broad temperature and current ranges. To aid in mode selection and improve manufacturing yield, DFB lasers often utilize a phase shift section within the diode structure as well.
The lasing wavelength for a DFB is approximately equal to the Bragg wavelength:
where λ is the wavelength, neff is the effective refractive index, and Λ is the grating period. By changing the effective index, the lasing wavelength can be tuned. This is accomplished through temperature and current tuning of the DFB.
The DFB has a relatively narrow tuning range: about 2 nm at 850 nm, about 4 nm at 1550 nm, or at least 1 cm-1 in the mid-IR (4.00 - 11.00 µm). However, over this tuning range, the DFB can achieve single-frequency operation, which means that this is a continuous tuning range without mode hops. Because of this feature, DFBs have become a popular and majority choice for real-world applications such as telecom and sensors. Since the cavity length of a DFB is rather short, the linewidths are typically in the 1 MHz to 10 MHz range. Additionally, the close coupling between the grating structure and the active region results in lower maximum output power compared to ECL and DBR lasers.
Click to Enlarge
Figure 3: VHG Lasers have a Volume Holographic Grating Outside of the Active Gain Medium
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.
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.
Thorlabs Ultralow Noise (ULN) Hybrid Lasers 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. As with the ECL, this 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 fiber is embedded with an FBG, which is a region of varry refractive index. This acts as a Bragg reflector with the added benefit of being thermally isolated from the gain medium. The grating period, or frequency to which the refractive index changes, can be changed by introducing thermal stress to the fiber, allowing users to temperature tune the laser output without affecting the gain medium's temperature. While this configuration provides both excellent low-noise performance and accurate tuning capabilities, the length of the fiber required causes the hermetically sealed case to be extended beyond a typical 14-pin package requiring custom mounting.
Click to Enlarge
Figure 5: Thorlabs Hybrid Lasers have a Fiber Bragg Gratting Coupled to the Active Gain Medium
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 (<1 MHz) 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 has the lowest output power due to inherent properties of the continuous grating feedback structure.
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.
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.
Use grounded anti-static wrist straps whenever handling diodes.
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.
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.
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.
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.
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.
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.
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:
|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.|
|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.|
|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).|
|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.|
|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.|
|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.|
|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.|
|All class 2 lasers (and higher) must display, in addition to the corresponding sign above, this triangular warning sign.|
|The rows shaded green below denote single-frequency lasers.|
|L375P70MLD||375 nm||70 mW||110 mA||5.4 V||9°||22.5°||Single Mode||Ø5.6 mm|
|L404P400M||404 nm||400 mW||370 mA||4.9 V||13° (1/e2)||42° (1/e2)||Multimode||Ø5.6 mm|
|LP405-SF10||405 nm||10 mW||50 mA||5.0 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|L405P20||405 nm||20 mW||38 mA||4.8 V||8.5°||19°||Single Mode||Ø5.6 mm|
|LP405C1||405 nm||30 mW||75 mA||4.3 V||1.4 mrad||1.4 mrad||Single Mode||Ø3.8 mm, SM Pigtail with Collimator|
|L405G2||405 nm||35 mW||50 mA||4.9 V||10°||21°||Single Mode||Ø3.8 mm|
|DL5146-101S||405 nm||40 mW||70 mA||5.2 V||8°||19°||Single Mode||Ø5.6 mm|
|L405P150||405 nm||150 mW||138 mA||4.9 V||6°||6°||Single Mode||Ø3.8 mm|
|LP405-MF300||405 nm||300 mW||350 mA||4.5 V||-||-||Multimode||Ø5.6 mm, MM Pigtail|
|L405G1||405 nm||1000 mW||900 mA||5.0 V||13°||45°||Multimode||Ø9 mm|
|L450G1||447 nm||3000 mW||2000 mA||5.2 V||6°||30°||Multimode||Ø9 mm|
|LP450-SF15||450 nm||15 mW||85 mA||5.5 V||-||-||Single Mode||Ø9 mm, SM Pigtail|
|PL450B||450 nm||80 mW||75 mA||5.2 V||4 - 7.5°||18 - 25°||Single Mode||Ø3.8 mm|
|L450P1600MM||450 nm||1600 mW||1200 mA||4.8 V||7°||19 - 27°||Multimode||Ø5.6 mm|
|L473P100||473 nm||100 mW||120 mA||5.7 V||10||24||Single Mode||Ø5.6 mm|
|LP488-SF20||488 nm||20 mW||70 mA||6.0 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|L488P60||488 nm||60 mW||75 mA||6.8 V||7°||23°||Single Mode||Ø5.6 mm|
|LP515-SF3||515 nm||3 mW||50 mA||5.3 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|L515A1||515 nm||10 mW||50 mA||5.4 V||6.5°||21°||Single Mode||Ø5.6 mm|
|LP520-SF15||520 nm||15 mW||140 mA||6.5 V||-||-||Single Mode||Ø9 mm, SM Pigtail|
|PL520||520 nm||50 mW||250 mA||7.0 V||7°||22°||Single Mode||Ø3.8 mm|
|L520P50||520 nm||45 mW||150 mA||7.0 V||7°||22°||Single Mode||Ø5.6 mm|
|L520G1||520 nm||900 mW||1600 mA||4.8 V||7.5°||25°||Multimode||Ø9 mm (non-standard)|
|DJ532-10||532 nm||10 mW||220 mA||1.9 V||0.69°||0.69°||Single Mode||Ø9.5 mm (non-standard)|
|DJ532-40||532 nm||40 mW||330 mA||1.9 V||0.69°||0.69°||Single Mode||Ø9.5 mm (non-standard)|
|LP633-SF50||633 nm||50 mW||170 mA||2.6 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|HL63163DG||633 nm||100 mW||170 mA||2.6 V||8.5°||18°||Single Mode||Ø5.6 mm|
|LPS-635-FC||635 nm||2.5 mW||70 mA||2.2 V||-||-||Single Mode||Ø9.5 mm, SM Pigtail|
|LPS-PM635-FC||635 nm||2.5 mW||70 mA||2.2 V||-||-||Single Mode||Ø9.5 mm, PM Pigtail|
|L635P5||635 nm||5 mW||30 mA||<2.7 V||8°||32°||Single Mode||Ø5.6 mm|
|HL6312G||635 nm||5 mW||55 mA||<2.7 V||8°||31°||Single Mode||Ø9 mm|
|LPM-635-SMA||635 nm||8 mW||50 mA||2.2 V||-||-||Multimode||Ø9 mm, MM Pigtail|
|LP635-SF8||635 nm||8 mW||60 mA||2.3 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|HL6320G||635 nm||10 mW||70 mA||<2.7 V||8°||31°||Single Mode||Ø9 mm|
|HL6322G||635 nm||15 mW||85 mA||<2.7 V||8°||30°||Single Mode||Ø9 mm|
|L637P5||637 nm||5 mW||20 mA||<2.4 V||8°||34°||Single Mode||Ø5.6 mm|
|LP637-SF50||637 nm||50 mW||140 mA||2.6 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|LP637-SF70||637 nm||70 mW||220 mA||2.7 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|HL63142DG||637 nm||100 mW||140 mA||2.7 V||8°||18°||Single Mode||Ø5.6 mm|
|HL63133DG||637 nm||170 mW||250 mA||2.8 V||9°||17°||Single Mode||Ø5.6 mm|
|HL6388MG||637 nm||250 mW||340 mA||2.3 V||10°||40°||Multimode||Ø5.6 mm|
|L637G1||637 nm||1200 mW||1100 mA||2.5 V||10°||32°||Multimode||Ø9 mm (non-standard)|
|L638P040||638 nm||40 mW||92 mA||2.4 V||10°||21°||Single Mode||Ø5.6 mm|
|L638P150||638 nm||150 mW||230 mA||2.7 V||9||18||Single Mode||Ø3.8 mm|
|L638P200||638 nm||200 mW||280 mA||2.9 V||8||14||Single Mode||Ø5.6 mm|
|L638P700M||638 nm||700 mW||820 mA||2.2 V||9°||35°||Multimode||Ø5.6 mm|
|HL6358MG||639 nm||10 mW||40 mA||2.3 V||8°||21°||Single Mode||Ø5.6 mm|
|HL6323MG||639 nm||30 mW||95 mA||2.3 V||8.5°||30°||Single Mode||Ø5.6 mm|
|HL6362MG||640 nm||40 mW||90 mA||2.4 V||10°||21°||Single Mode||Ø5.6 mm|
|LP642-SF20||642 nm||20 mW||90 mA||2.5 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|LP642-PF20||642 nm||20 mW||90 mA||2.5 V||-||-||Single Mode||Ø5.6 mm, PM Pigtail|
|HL6364DG||642 nm||60 mW||125 mA||2.5 V||10°||21°||Single Mode||Ø5.6 mm|
|HL6366DG||642 nm||80 mW||155 mA||2.5 V||10°||21°||Single Mode||Ø5.6 mm|
|HL6385DG||642 nm||150 mW||280 mA||2.6 V||9°||17°||Single Mode||Ø5.6 mm|
|L650P007||650 nm||7 mW||28 mA||2.2 V||9°||28°||Single Mode||Ø5.6 mm|
|LPS-660-FC||658 nm||7.5 mW||65 mA||2.6 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|LP660-SF20||658 nm||20 mW||80 mA||2.6 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|LPM-660-SMA||658 nm||22.5 mW||65 mA||2.6 V||-||-||Multimode||Ø5.6 mm, MM Pigtail|
|HL6501MG||658 nm||30 mW||65 mA||2.6 V||8.5°||22°||Single Mode||Ø5.6 mm|
|L658P040||658 nm||40 mW||75 mA||2.2 V||10°||20°||Single Mode||Ø5.6 mm|
|LP660-SF40||658 nm||40 mW||135 mA||2.5 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|LP660-SF60||658 nm||60 mW||210 mA||2.4 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|HL6544FM||660 nm||50 mW||115 mA||2.3 V||10°||17°||Single Mode||Ø5.6 mm|
|LP660-SF50||660 nm||50 mW||140 mA||2.3 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|HL6545MG||660 nm||120 mW||170 mA||2.45 V||10°||17°||Single Mode||Ø5.6 mm|
|L660P120||660 nm||120 mW||175 mA||2.5 V||10°||17°||Single Mode||Ø5.6 mm|
|L670VH1||670 nm||1 mW||2.5 mA||2.6 V||10°||10°||Single Mode||TO-46|
|LPS-675-FC||670 nm||2.5 mW||55 mA||2.2 V||-||-||Single Mode||Ø9 mm, SM Pigtail|
|HL6748MG||670 nm||10 mW||30 mA||2.2 V||8°||25°||Single Mode||Ø5.6 mm|
|HL6714G||670 nm||10 mW||55 mA||<2.7 V||8°||22°||Single Mode||Ø9 mm|
|HL6756MG||670 nm||15 mW||35 mA||2.3 V||8°||24°||Single Mode||Ø5.6 mm|
|LP685-SF15||685 nm||15 mW||55 mA||2.1 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|HL6750MG||685 nm||50 mW||75 mA||2.3 V||9°||21°||Single Mode||Ø5.6 mm|
|HL6738MG||690 nm||30 mW||90 mA||2.5 V||8.5°||19°||Single Mode||Ø5.6 mm|
|LP705-SF15||705 nm||15 mW||55 mA||2.3 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|HL7001MG||705 nm||40 mW||75 mA||2.5 V||9°||18°||Single Mode||Ø5.6 mm|
|HL7302MG||730 nm||40 mW||75 mA||2.5 V||9°||18°||Single Mode||Ø5.6 mm|
|DBR760PN||761 nm||9 mW||125 mA||2.0 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|DBR767PN||767 nm||23 mW||220 mA||1.87 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|DBR770PN||770 nm||35 mW||220 mA||1.92 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|L780P010||780 nm||10 mW||24 mA||1.8 V||8°||30°||Single Mode||Ø5.6 mm|
|LP780-SAD15||780 nm||15 mW||180 mA||2.2 V||-||-||Single Frequency||Ø9 mm, SM Pigtail|
|DBR780PN||780 nm||45 mW||250 mA||1.9 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|L785P5||785 nm||5 mW||28 mA||1.9 V||10°||29°||Single Mode||Ø5.6 mm|
|LPS-PM785-FC||785 nm||6.25 mW||65 mA||-||-||-||Single Mode||Ø5.6 mm, PM Pigtail|
|LPS-785-FC||785 nm||10 mW||65 mA||1.85 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|LP785-SF20||785 nm||20 mW||85 mA||1.9 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|DBR785S||785 nm||25 mW||230 mA||2.0 V||-||-||Single Frequency||Butterfly, SM Pigtail|
|DBR785P||785 nm||25 mW||230 mA||2.0 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|L785P25||785 nm||25 mW||45 mA||1.9 V||8°||30°||Single Mode||Ø5.6 mm|
|FPV785S||785 nm||50 mW||410 mA||2.2 V||-||-||Single Frequency||Butterfly, SM Pigtail|
|FPV785P||785 nm||50 mW||410 mA||2.1 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|LP785-SAV50||785 nm||50 mW||500 mA||2.2 V||-||-||Single Frequency||Ø9 mm, SM Pigtail|
|L785P090||785 nm||90 mW||120 mA||2.0 V||9°||16°||Single Mode||Ø5.6 mm|
|LP785-SF100||785 nm||100 mW||300 mA||2.0 V||-||-||Single Mode||Ø9 mm, SM Pigtail|
|L785H1||785 nm||200 mW||220 mA||2.5 V||8.5°||16°||Single Mode||Ø5.6 mm|
|FPL785P||785 nm||200 mW||500 mA||2.1 V||-||-||Single Mode||Butterfly, PM Pigtail|
|FPL785S-250||785 nm||250 mW (Min)||500 mA||2.0 V||-||-||Single Mode||Butterfly, SM Pigtail|
|LD785-SEV300||785 nm||300 mW||500 mA (Max)||2.0 V||8°||16°||Single Frequency||Ø9 mm|
|LD785-SH300||785 nm||300 mW||400 mA||2.0 V||7°||18°||Single Mode||Ø9 mm|
|FPL785C||785 nm||300 mW||400 mA||2.0 V||7°||18°||Single Mode||3 mm x 5 mm Submount|
|LD785-SE400||785 nm||400 mW||550 mA||2.0 V||7°||16°||Single Mode||Ø9 mm|
|FPV785M||785 nm||600 mW||1100 mA||1.9 V||-||-||Multimode||Butterfly, MM Pigtail|
|L795VH1||795 nm||0.25 mW||1.2 mA||1.8 V||20°||12°||Single Frequency||TO-46|
|DBR795PN||795 nm||40 mW||230 mA||2.0 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|ML620G40||805 nm||500 mW||650 mA||1.9 V||3°||34°||Multimode||Ø5.6 mm|
|L808P010||808 nm||10 mW||50 mA||2 V||10°||30°||Single Mode||Ø5.6 mm|
|L808P030||808 nm||30 mW||65 mA||2 V||10°||30°||Single Mode||Ø5.6 mm|
|DBR808PN||808 nm||42 mW||250 mA||2 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|M9-808-0150||808 nm||150 mW||180 mA||1.9 V||8°||17°||Single Mode||Ø9 mm|
|L808P200||808 nm||200 mW||260 mA||2 V||10°||30°||Multimode||Ø5.6 mm|
|FPL808P||808 nm||200 mW||600 mA||2.1 V||-||-||Single Mode||Butterfly, PM Pigtail|
|FPL808S||808 nm||200 mW||750 mA||2.3 V||-||-||Single Mode||Butterfly, SM Pigtail|
|LD808-SE500||808 nm||500 mW||750 mA||2.2 V||7°||14°||Single Mode||Ø9 mm|
|LD808-SEV500||808 nm||500 mW||800 mA (Max)||2.2 V||8°||14°||Single Frequency||Ø9 mm|
|L808P500MM||808 nm||500 mW||650 mA||1.8 V||12°||30°||Multimode||Ø5.6 mm|
|L808P1000MM||808 nm||1000 mW||1100 mA||2 V||9°||30°||Multimode||Ø9 mm|
|DBR816PN||816 nm||45 mW||250 mA||1.95 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|LP820-SF80||820 nm||80 mW||230 mA||2.3 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|L820P100||820 nm||100 mW||145 mA||2.1 V||9°||17°||Single Mode||Ø5.6 mm|
|L820P200||820 nm||200 mW||250 mA||2.4 V||9°||17°||Single Mode||Ø5.6 mm|
|DBR828PN||828 nm||24 mW||250 mA||2.0 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|LPS-830-FC||830 nm||10 mW||120 mA||-||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|LPS-PM830-FC||830 nm||10 mW||120 mA||-||-||-||Single Mode||Ø5.6 mm, PM Pigtail|
|LP830-SF30||830 nm||30 mW||115 mA||1.9 V||-||-||Single Mode||Ø9 mm, SM Pigtail|
|HL8338MG||830 nm||50 mW||75 mA||1.9 V||9°||22°||Single Mode||Ø5.6 mm|
|L830H1||830 nm||250 mW||3 A (Max)||2 V||8°||10°||Single Mode||Ø9 mm|
|FPL830P||830 nm||300 mW||900 mA||2.22 V||-||-||Single Mode||Butterfly, PM Pigtail|
|FPL830S||830 nm||350 mW||900 mA||2.5 V||-||-||Single Mode||Butterfly, SM Pigtail|
|LD830-SE650||830 nm||650 mW||900 mA||2.3 V||7°||13°||Single Mode||Ø9 mm|
|LD830-MA1W||830 nm||1 W||1.330 A||2.1 V||7°||24°||Multimode||Ø9 mm|
|LD830-ME2W||830 nm||2 W||3 A (Max)||2.0 V||8°||21°||Multimode||Ø9 mm|
|L840P200||840 nm||200 mW||255 mA||2.4 V||9||17||Single Mode||Ø5.6 mm|
|L850VH1||850 nm||1 mW||2 mA||2 V||12°||12°||Single Frequency||TO-46|
|L850P010||850 nm||10 mW||50 mA||2 V||10°||30°||Single Mode||Ø5.6 mm|
|L850P030||850 nm||30 mW||65 mA||2 V||8.5°||30°||Single Mode||Ø5.6 mm|
|LP850-SF80||850 nm||80 mW||230 mA||2.3 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|FPV852S||852 nm||20 mW||400 mA||2.2 V||-||-||Single Frequency||Butterfly, SM Pigtail|
|FPV852P||852 nm||20 mW||400 mA||2.2 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|DBR852PN||852 nm||24 mW||300 mA||2.0 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|LP852-SF30||852 nm||30 mW||115 mA||1.9 V||-||-||Single Mode||Ø9 mm, SM Pigtail|
|L852P50||852 nm||50 mW||75 mA||1.9 V||9°||22°||Single Mode||Ø5.6 mm|
|L852P100||852 nm||100 mW||120 mA||1.9 V||8°||28°||Single Mode||Ø9 mm|
|L852P150||852 nm||150 mW||170 mA||1.9 V||8°||18°||Single Mode||Ø9 mm|
|L852H1||852 nm||300 mW||415 mA (Max)||2 V||7°||15°||Single Mode||Ø9 mm|
|FPL852P||852 nm||300 mW||900 mA||2.35 V||-||-||Single Mode||Butterfly, PM Pigtail|
|FPL852S||852 nm||350 mW||900 mA||2.5 V||-||-||Single Mode||Butterfly, SM Pigtail|
|LD852-SE600||852 nm||600 mW||950 mA||2.3 V||7° (1/e2)||13° (1/e2)||Single Mode||Ø9 mm|
|LD852-SEV600||852 nm||600 mW||1050 mA (Max)||2.2 V||8°||13° (1/e2)||Single Frequency||Ø9 mm|
|LP880-SF3||880 nm||3 mW||25 mA||2.2 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|L880P010||880 nm||10 mW||30 mA||2.0 V||12°||37°||Single Mode||Ø5.6 mm|
|L895VH1||895 nm||0.2 mW||1.4 mA||1.6 V||20°||13°||Single Frequency||TO-46|
|DBR895PN||895 nm||12 mW||300 mA||2 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|L904P010||904 nm||10 mW||50 mA||2 V||10°||30°||Single Mode||Ø5.6 mm|
|LP915-SF40||915 nm||40 mW||130 mA||1.5 V||-||-||Single Mode||Ø9 mm, SM Pigtail|
|M9-915-0300||915 nm||300 mW||370 mA||1.9 V||8°||28°||Single Mode||Ø9 mm|
|LP940-SF30||940 nm||30 mW||90 mA||1.5 V||-||-||Single Mode||Ø9 mm, SM Pigtail|
|M9-940-0200||940 nm||200 mW||270 mA||1.9 V||8°||28°||Single Mode||Ø9 mm|
|L960H1||960 nm||250 mW||400 mA||2.1 V||11°||12°||Single Mode||Ø9 mm|
|FPV976S||976 nm||30 mW||400 mA (Max)||2.2 V||-||-||Single Frequency||Butterfly, SM Pigtail|
|FPV976P||976 nm||30 mW||400 mA (Max)||2.2 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|DBR976PN||976 nm||33 mW||450 mA||2.0 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|BL976-SAG300||976 nm||300 mW||470 mA||2.0 V||-||-||Single Mode||Butterfly, SM Pigtail|
|BL976-PAG500||976 nm||500 mW||830 mA||2.0 V||-||-||Single Mode||Butterfly, PM Pigtail|
|BL976-PAG700||976 nm||700 mW||1090 mA||2.0 V||-||-||Single Mode||Butterfly, PM Pigtail|
|BL976-PAG900||976 nm||900 mW||1480 mA||2.5 V||-||-||Single Mode||Butterfly, PM Pigtail|
|L980P010||980 nm||10 mW||25 mA||2 V||10°||30°||Single Mode||Ø5.6 mm|
|LP980-SF15||980 nm||15 mW||70 mA||1.5 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|L980P030||980 nm||30 mW||50 mA||1.5 V||10°||35°||Single Mode||Ø5.6 mm|
|L9805E2P5||980 nm||50 mW||95 mA||1.5 V||8°||33°||Single Mode||Ø5.6 mm|
|L980P100A||980 nm||100 mW||150 mA||1.6 V||6°||32°||Multimode||Ø5.6 mm|
|L980H1||980 nm||200 mW||300 mA (Max)||2.0 V||8°||13°||Single Mode||Ø9 mm|
|L980P200||980 nm||200 mW||300 mA||1.5 V||6°||30°||Multimode||Ø5.6 mm|
|DBR1060SN||1060 nm||130 mW||650 mA||2.0 V||-||-||Single Frequency||Butterfly, SM Pigtail|
|DBR1060PN||1060 nm||130 mW||650 mA||1.8 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|DBR1064S||1064 nm||40 mW||150 mA||2.0 V||-||-||Single Frequency||Butterfly, SM Pigtail|
|DBR1064P||1064 nm||40 mW||150 mA||2.0 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|DBR1064PN||1064 nm||110 mW||550 mA||2.0 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|LPS-1060-FC||1064 nm||50 mW||220 mA||1.4 V||-||-||Single Mode||Ø9 mm, SM Pigtail|
|M9-A64-0200||1064 nm||200 mW||280 mA||1.7 V||8°||28°||Single Mode||Ø9 mm|
|M9-A64-0300||1064 nm||300 mW||390 mA||1.7 V||8°||28°||Single Mode||Ø9 mm|
|L1064H1||1064 nm||300 mw||700 mA||1.92 V||7.6°||13.5°||Single Mode||Ø9 mm|
|DBR1083PN||1083 nm||100 mW||500 mA||1.75 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|LP1310-SAD2||1310 nm||2.0 mW||40 mA||1.1 V||-||-||Single Frequency||Ø5.6 mm, SM Pigtail|
|LPS-1310-FC||1310 nm||2.5 mW||20 mA||1.1 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|LPS-PM1310-FC||1310 nm||2.5 mW||20 mA||1.1 V||-||-||Single Mode||Ø5.6 mm, PM Pigtail|
|L1310P5DFB||1310 nm||5 mW||20 mA||1.1 V||7°||9°||Single Frequency||Ø5.6 mm|
|ML725B8F||1310 nm||5 mW||20 mA||1.1 V||25°||30°||Single Mode||Ø5.6 mm|
|LPSC-1310-FC||1310 nm||50 mW||350 mA||2 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|FPL1053S||1310 nm||130 mW||400 mA||1.7 V||-||-||Single Mode||Butterfly, SM Pigtail|
|FPL1053P||1310 nm||130 mW||400 mA||1.7 V||-||-||Single Mode||Butterfly, PM Pigtail|
|FPL1053T||1310 nm||300 mW (Pulsed)||750 mA||2 V||15°||28°||Single Mode||Ø5.6 mm|
|FPL1053C||1310 nm||300 mW (Pulsed)||750 mA||2 V||15°||27°||Single Mode||Chip on Submount|
|L1310G1||1310 nm||2000 mW||5 A||1.5 V||7°||24°||Multimode||Ø9 mm|
|L1370G1||1370 nm||2000 mW||5 A||1.4 V||6°||22°||Multimode||Ø9 mm|
|BL1425-PAG500||1425 nm||500 mW||1600 mA||2.0 V||-||-||Single Mode||Butterfly, PM Pigtail|
|BL1436-PAG500||1436 nm||500 mW||1600 mA||2.0 V||-||-||Single Mode||Butterfly, PM Pigtail|
|L1450G1||1450 nm||2000 mW||5 A||1.4 V||7°||22°||Multimode||Ø9 mm|
|BL1456-PAG500||1456 nm||500 mW||1600 mA||2.0 V||-||-||Single Mode||Butterfly, PM Pigtail|
|L1480G1||1480 nm||2000 mW||5 A||1.6 V||6°||20°||Multimode||Ø9 mm|
|LPS-1550-FC||1550 nm||1.5 mW||30 mA||1.0 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|LPS-PM1550-FC||1550 nm||1.5 mW||30 mA||1.1 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|LP1550-SAD2||1550 nm||2.0 mW||40 mA||1.0 V||-||-||Single Frequency||Ø5.6 mm, SM Pigtail|
|LP1550-PAD2||1550 nm||2.0 mW||40 mA||1.0 V||-||-||Single Frequency||Ø5.6 mm, PM Pigtail|
|L1550P5DFB||1550 nm||5 mW||20 mA||1.1 V||8°||10°||Single Frequency||Ø5.6 mm|
|ML925B45F||1550 nm||5 mW||30 mA||1.1 V||25°||30°||Single Mode||Ø5.6 mm|
|SFL1550S||1550 nm||40 mW||300 mA||1.5 V||-||-||Single Frequency||Butterfly, SM Pigtail|
|SFL1550P||1550 nm||40 mW||300 mA||1.5 V||-||-||Single Frequency||Butterfly, PM Pigtail|
|LPSC-1550-FC||1550 nm||50 mW||250 mA||2 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|FPL1009S||1550 nm||100 mW||400 mA||1.4 V||-||-||Single Mode||Butterfly, SM Pigtail|
|FPL1009P||1550 nm||100 mW||400 mA||1.4 V||-||-||Single Mode||Butterfly, PM Pigtail|
|FPL1001C||1550 nm||150 mW||400 mA||1.4 V||18°||31°||Single Mode||Chip on Submount|
|FPL1055T||1550 nm||300 mW (Pulsed)||750 mA||2 V||15°||28°||Single Mode||Ø5.6 mm|
|FPL1055C||1550 nm||300 mW (Pulsed)||750 mA||2 V||15°||28°||Single Mode||Chip on Submount|
|L1550G1||1550 nm||1700 mW||5 A||1.5 V||7°||28°||Multimode||Ø9 mm|
|L1575G1||1575 nm||1700 mW||5 A||1.5 V||6°||28°||Multimode||Ø9 mm|
|LPSC-1625-FC||1625 nm||50 mW||350 mA||1.5 V||-||-||Single Mode||Ø5.6 mm, SM Pigtail|
|FPL1054S||1625 nm||80 mW||400 mA||1.7 V||-||-||Single Mode||Butterfly, SM Pigtail|
|FPL1054P||1625 nm||80 mW||400 mA||1.7 V||-||-||Single Mode||Butterfly, PM Pigtail|
|FPL1054C||1625 nm||250 mW (Pulsed)||750 mA||2 V||15°||28°||Single Mode||Chip on Submount|
|FPL1054T||1625 nm||200 mW (Pulsed)||750 mA||2 V||15°||28°||Single Mode||Ø5.6 mm|
|FPL1059S||1650 nm||80 mW||400 mA||1.7 V||-||-||Single Mode||Butterfly, SM Pigtail|
|FPL1059P||1650 nm||80 mW||400 mA||1.7 V||-||-||Single Mode||Butterfly, PM Pigtail|
|FPL1059C||1650 nm||225 mW (Pulsed)||750 mA||2 V||15°||28°||Single Mode||Chip on Submount|
|FPL1059T||1650 nm||225 mW (Pulsed)||750 mA||2 V||15°||28°||Single Mode||Ø5.6 mm|
|FPL1940S||1940 nm||15 mW||400 mA||2 V||-||-||Single Mode||Butterfly, SM Pigtail|
|FPL2000S||2 µm||15 mW||400 mA||2 V||-||-||Single Mode||Butterfly, SM Pigtail|
|FPL2000C||2 µm||30 mW||400 mA||5.2 V||8°||19°||Single Mode||Chip on Submount|
|ID3250HHLH||3.00 - 3.50 µm (DFB)||5 mW||400 mA||5 V||6 mrad (0.34°)||6 mrad (0.34°)||Single Frequency||Two-Tab C-Mount|
|QF3850T1||3.85 µm (FP)||200 mW||600 mA (Max)||13.5 V||30°||40°||Single Mode||Ø9 mm|
|QF3850HHLH||3.85 µm (FP)||320 mW (Min)||1100 mA||13 V||6 mrad (0.34°)||6 mrad (0.34°)||Single Mode||Horizontal HHL|
|QF4040HHLH||4.05 µm (FP)||320 mW (Min)||1100 mA||13 V||6 mrad (0.34°)||6 mrad (0.34°)||Single Mode||Horizontal HHL|
|QD4500CM1||4.00 - 5.00 µm (DFB)||40 mW||<500 mA||10.5 V||30°||40°||Single Frequency||Two-Tab C-Mount|
|QF4050C2||4.05 µm (FP)||300 mW||400 mA||12 V||30||42||Single Mode||Two-Tab C-Mount|
|QF4050T1||4.05 µm (FP)||300 mW||600 mA (Max)||12.0 V||30°||40°||Single Mode||Ø9 mm|
|QF4050D2||4.05 µm (FP)||800 mW||750 mA||13 V||30°||40°||Single Mode||D-Mount|
|QF4050D3||4.05 µm (FP)||1200 mW||1000 mA||13 V||30°||40°||Single Mode||D-Mount|
|QF4550CM1||4.55 µm (FP)||450 mW||900 mA||10.5 V||30°||55°||Single Mode||Two-Tab C-Mount|
|QF4600T2||4.60 µm (FP)||200 mW||500 mA (Max)||13.0 V||30°||40°||Single Mode||Ø9 mm|
|QF4600T1||4.60 µm (FP)||400 mW||800 mA (Max)||12.0 V||30°||40°||Single Mode||Ø9 mm|
|QF4600D4||4.60 µm (FP)||2500 mW||1800 mA||12.5 V||40°||30°||Single Mode||D-Mount|
|QF4650HHLH||4.65 µm (FP)||1500 mW (Min)||1100 mA||12 V||6 mrad (0.34°)||6 mrad (0.34°)||Single Mode||Horizontal HHL|
|QD5500CM1||5.00 - 8.00 µm (DFB)||40 mW||<700 mA||9.5 V||30 °||45 °||Single Frequency||Two-Tab C-Mount|
|QD5250CM1||5.20 - 5.30 µm (DFB)||120 mW||<660 mA||10.2 V||41°||52°||Single Frequency||Two-Tab C-Mount|
|QF5300CM1||5.30 µm (FP)||150 mW||1200 mA||9.0 V||30°||55°||Single Mode||Two-Tab C-Mount|
|QD6500CM1||6.00 - 7.00 µm (DFB)||40 mW||<650 mA||10 V||35 °||50 °||Single Frequency||Two-Tab C-Mount|
|QD7500CM1||7.00 - 8.00 µm (DFB)||40 mW||<600 mA||10 V||40°||50°||Single Frequency||Two-Tab C-Mount|
|QD7500HHLH||7.00 - 8.00 µm (DFB)||50 mW||700 mA||12 V||6 mrad (0.34°)||6 mrad (0.34°)||Single Frequency||Horizontal HHL|
|QD7500DM1||7.00 - 8.00 µm (DFB)||100 mW||<600 mA||11.5 V||40°||55°||Single Frequency||D-Mount|
|QD8050CM1||8.00 - 8.10 µm (DFB)||100 mW||<1000 mA||9.5 V||55°||70°||Single Frequency||Two-Tab C-Mount|
|QD8500CM1||8.00 - 9.00 µm (DFB)||100 mW||<900 mA||9.5 V||40 °||55 °||Single Frequency||Two-Tab C-Mount|
|QD8500HHLH||8.00 - 9.00 µm (DFB)||100 mW||<600 mA||10.2 V||6 mrad (0.34°)||6 mrad (0.34°)||Single Frequency||Horizontal HHL|
|QD8650CM1||8.60 - 8.70 µm (DFB)||50 mW||<900 mA||9.5 V||55°||70°||Single Frequency||Two-Tab C-Mount|
|QD9500CM1||9.00 - 10.00 µm (DFB)||60 mW||<800 mA||9.5 V||40°||55°||Single Frequency||Two-Tab C-Mount|
|QD9500HHLH||9.00 - 10.00 µm (DFB)||100 mW||<600 mA||10.2 V||6 mrad (0.34°)||6 mrad (0.34°)||Single Frequency||Horizontal HHL|
|QF9150C2||9.15 µm (FP)||200 mW||850 mA||11 V||40°||60°||Single Mode||Two-Tab C-Mount|
|QF9550CM1||9.55 µm (FP)||80 mW||1500 mA||7.8 V||35°||60°||Single Mode||Two-Tab C-Mount|
|QD10500CM1||10.00 - 11.00 µm (DFB)||40 mW||<600 mA||10 V||40°||55°||Single Frequency||Two-Tab C-Mount|
|QD10500HHLH||10.00 - 11.00 µm (DFB)||50 mW||700 mA||12 V||6 mrad (0.34°)||6 mrad (0.34°)||Single Frequency||Horizontal HHL|
|The rows shaded green above denote single-frequency lasers.|