Server-rendered product directory

Lasers model catalog

Browse 3,778 canonical product destinations across 12 product families. Page 26 lists models 3,001–3,120.

Laser modelsOEM-I-793-BG793 nm CW LasersThe OEM-I-793-BG is a 793 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Tuning changes the selected output wavelength so spectral features can be scanned with the same source. The tuning band specifies which lines can be reached; linewidth describes the width of the selected line. The specified fiber connection delivers the generated light to the experiment; its core size, numerical aperture and connector need to match the receiving optics.View product →
Laser modelsOEM-IR-20962096 nm Pulsed LasersThe OEM-IR-2096 is a 2096 nm pulsed diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy.View product →
Laser modelsOEM-IR-21202120 nm Pulsed LasersThe OEM-IR-2120 is a 2120 nm pulsed diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy.View product →
Laser modelsOEM-IR-21302130 nm CW LasersThe OEM-IR-2130 is a 2130 nm continuous-wave diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsOEM-JD-520520 nm CW LasersThe OEM-JD-520 is a 520 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
Laser modelsOEM-JD-635635 nm CW LasersThe OEM-JD-635 is a 635 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
Laser modelsOEM-MFOEM-MF high-power line laserThe OEM-MF is a CW line laser with 375–1550 nm wavelength options and output up to 15 W, depending on wavelength. TTL or analog up to 30 kHz. Select a listed wavelength, fan angle and power configuration for the required working distance.View product →
Laser modelsOEM-N-532532 nm Multi-wavelength LasersThe OEM-N-532 is a 532 nm continuous-wave diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
Laser modelsOEM-S-545-MD545 nm CW LasersThe OEM-S-545-MD is a 545 nm continuous-wave diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. The specified fiber connection delivers the generated light to the experiment; its core size, numerical aperture and connector need to match the receiving optics.View product →
Laser modelsOEM-S-561-MD561 nm CW LasersThe OEM-S-561-MD is a 561 nm continuous-wave diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. The specified fiber connection delivers the generated light to the experiment; its core size, numerical aperture and connector need to match the receiving optics.View product →
Laser modelsOEM-S-577-MD577 nm CW LasersThe OEM-S-577-MD is a 577 nm continuous-wave diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. The specified fiber connection delivers the generated light to the experiment; its core size, numerical aperture and connector need to match the receiving optics.View product →
Laser modelsOEM-S-588-MD588 nm CW LasersThe OEM-S-588-MD is a 588 nm continuous-wave diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. The specified fiber connection delivers the generated light to the experiment; its core size, numerical aperture and connector need to match the receiving optics.View product →
Laser modelsOEM-S-589-MD589 nm CW LasersThe OEM-S-589-MD is a 589 nm continuous-wave diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. The specified fiber connection delivers the generated light to the experiment; its core size, numerical aperture and connector need to match the receiving optics.View product →
Laser modelsOEM-TD-635635 nm Multi-wavelength LasersThe OEM-TD-635 is a 635 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
Laser modelsOEM-W-532532 nm Multi-wavelength LasersThe OEM-W-532 is a 532 nm continuous-wave diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
Laser modelsOptical Communication Series ExperimentComponents & AccessoriesExperiment of laser propagation in waveguide; B asic experiment of fiber technology; Laser fiber coupling experiment; Fiber sensing series experiments; Fiber stimulated Raman scattering experimentView product →
Laser modelsPGL Series637 nm CW LasersThe PGL Series is a 637 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-D12405 nm CW LasersThe PGL-D12 is a 405 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-D12-405405 nm CW LasersThe PGL-D12-405 is a 405 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-D12-445445 nm CW LasersThe PGL-D12-445 is a 445 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-D12-447447 nm CW LasersThe PGL-D12-447 is a 447 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-D12-450450 nm CW LasersThe PGL-D12-450 is a 450 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-D12-520520 nm CW LasersThe PGL-D12-520 is a 520 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-D12-635635 nm CW LasersThe PGL-D12-635 is a 635 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-D12-640640 nm CW LasersThe PGL-D12-640 is a 640 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-D12-655656 nm Pulsed LasersThe PGL-D12-655 is a 656 nm pulsed direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy.View product →
Laser modelsPGL-D12-655655 nm Pulsed LasersThe PGL-D12-655 is a 655 nm pulsed direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample.View product →
Laser modelsPGL-D12-808808 nm CW LasersThe PGL-D12-808 is a 808 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Tuning changes the selected output wavelength so spectral features can be scanned with the same source. The tuning band specifies which lines can be reached; linewidth describes the width of the selected line.View product →
Laser modelsPGL-D8405 nm CW LasersThe PGL-D8 is a 405 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-D8-405405 nm CW LasersThe PGL-D8-405 is a 405 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-D8-445445 nm CW LasersThe PGL-D8-445 is a 445 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-D8-447447 nm CW LasersThe PGL-D8-447 is a 447 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-D8-450450 nm CW LasersThe PGL-D8-450 is a 450 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-D8-520520 nm CW LasersThe PGL-D8-520 is a 520 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-D8-635635 nm CW LasersThe PGL-D8-635 is a 635 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-D8-640640 nm CW LasersThe PGL-D8-640 is a 640 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-D8-655656 nm Pulsed LasersThe PGL-D8-655 is a 656 nm pulsed direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy.View product →
Laser modelsPGL-D8-655655 nm Pulsed LasersThe PGL-D8-655 is a 655 nm pulsed direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample.View product →
Laser modelsPGL-F-405405 nm CW LasersThe PGL-F-405 is a 405 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. PC control allows the operating state to be set from software, so illumination can be coordinated with the experiment.View product →
Laser modelsPGL-F-445445 nm CW LasersThe PGL-F-445 is a 445 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. PC control allows the operating state to be set from software, so illumination can be coordinated with the experiment.View product →
Laser modelsPGL-F-450450 nm CW LasersThe PGL-F-450 is a 450 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. PC control allows the operating state to be set from software, so illumination can be coordinated with the experiment.View product →
Laser modelsPGL-F-488488 nm CW LasersThe PGL-F-488 is a 488 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. PC control allows the operating state to be set from software, so illumination can be coordinated with the experiment.View product →
Laser modelsPGL-F-520520 nm CW LasersThe PGL-F-520 is a 520 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. PC control allows the operating state to be set from software, so illumination can be coordinated with the experiment.View product →
Laser modelsPGL-F-660660 nm CW LasersThe PGL-F-660 is a 660 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. PC control allows the operating state to be set from software, so illumination can be coordinated with the experiment.View product →
Laser modelsPGL-F-685685 nm Pulsed LasersThe PGL-F-685 is a 685 nm pulsed laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. PC control allows the operating state to be set from software, so illumination can be coordinated with the experiment.View product →
Laser modelsPGL-F-785785 nm CW LasersThe PGL-F-785 is a 785 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. PC control allows the operating state to be set from software, so illumination can be coordinated with the experiment.View product →
Laser modelsPGL-F-830830 nm CW LasersThe PGL-F-830 is a 830 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. PC control allows the operating state to be set from software, so illumination can be coordinated with the experiment.View product →
Laser modelsPGL-F-940940 nm CW LasersThe PGL-F-940 is a 940 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. PC control allows the operating state to be set from software, so illumination can be coordinated with the experiment.View product →
Laser modelsPGL-FP-10641064 nm CW LasersThe PGL-FP-1064 is a 1064 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-FP-13101310 nm CW LasersThe PGL-FP-1310 is a 1310 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-FP-15501550 nm CW LasersThe PGL-FP-1550 is a 1550 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-FP-405405 nm CW LasersThe PGL-FP-405 is a 405 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. PC control allows the operating state to be set from software, so illumination can be coordinated with the experiment.View product →
Laser modelsPGL-FP-445445 nm CW LasersThe PGL-FP-445 is a 445 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. PC control allows the operating state to be set from software, so illumination can be coordinated with the experiment.View product →
Laser modelsPGL-FP-460460 nm Fiber LasersThe PGL-FP-460 is a 460 nm laser source. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-FP-480480 nm CW LasersThe PGL-FP-480 is a 480 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-FP-488488 nm CW LasersThe PGL-FP-488 is a 488 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. PC control allows the operating state to be set from software, so illumination can be coordinated with the experiment.View product →
Laser modelsPGL-FP-495495 nm CW LasersThe PGL-FP-495 is a 495 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-FP-520520 nm CW LasersThe PGL-FP-520 is a 520 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. PC control allows the operating state to be set from software, so illumination can be coordinated with the experiment.View product →
Laser modelsPGL-FP-633633 nm CW LasersThe PGL-FP-633 is a 633 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-FP-635635 nm CW LasersThe PGL-FP-635 is a 635 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-FP-670670 nm CW LasersThe PGL-FP-670 is a 670 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-FP-685685 nm Pulsed LasersThe PGL-FP-685 is a 685 nm pulsed laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. PC control allows the operating state to be set from software, so illumination can be coordinated with the experiment.View product →
Laser modelsPGL-FP-808808 nm CW LasersThe PGL-FP-808 is a 808 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-FP-830830 nm CW LasersThe PGL-FP-830 is a 830 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. PC control allows the operating state to be set from software, so illumination can be coordinated with the experiment.View product →
Laser modelsPGL-FP-880880 nm Fiber LasersThe PGL-FP-880 is a 880 nm laser source. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-FP-905905 nm CW LasersThe PGL-FP-905 is a 905 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-FP-940940 nm CW LasersThe PGL-FP-940 is a 940 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. PC control allows the operating state to be set from software, so illumination can be coordinated with the experiment.View product →
Laser modelsPGL-FP-980980 nm Pulsed LasersThe PGL-FP-980 is a 980 nm pulsed fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample.View product →
Laser modelsPGL-FS-10641064 nm CW LasersThe PGL-FS-1064 is a 1064 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-FS-405405 nm CW LasersThe PGL-FS-405 is a 405 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-FS-445445 nm CW LasersThe PGL-FS-445 is a 445 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-FS-447447 nm CW LasersThe PGL-FS-447 is a 447 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-FS-450450 nm CW LasersThe PGL-FS-450 is a 450 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-FS-520520 nm CW LasersThe PGL-FS-520 is a 520 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-FS-635635 nm CW LasersThe PGL-FS-635 is a 635 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-FS-640640 nm CW LasersThe PGL-FS-640 is a 640 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-FS-655656 nm Pulsed LasersThe PGL-FS-655 is a 656 nm pulsed direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy.View product →
Laser modelsPGL-FS-655655 nm Pulsed LasersThe PGL-FS-655 is a 655 nm pulsed direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample.View product →
Laser modelsPGL-FS-808808 nm CW LasersThe PGL-FS-808 is a 808 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Tuning changes the selected output wavelength so spectral features can be scanned with the same source. The tuning band specifies which lines can be reached; linewidth describes the width of the selected line.View product →
Laser modelsPGL-FS-980980 nm Pulsed LasersThe PGL-FS-980 is a 980 nm pulsed direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample.View product →
Laser modelsPGL-H-10601060 nm CW LasersThe PGL-H-1060 is a 1060 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-H-405405 nm CW LasersThe PGL-H-405 is a 405 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-H-445445 nm CW LasersThe PGL-H-445 is a 445 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-H-447447 nm CW LasersThe PGL-H-447 is a 447 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-H-450450 nm CW LasersThe PGL-H-450 is a 450 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-H-520520 nm CW LasersThe PGL-H-520 is a 520 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-H-635635 nm CW LasersThe PGL-H-635 is a 635 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-H-640640 nm CW LasersThe PGL-H-640 is a 640 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-H-655656 nm Pulsed LasersThe PGL-H-655 is a 656 nm pulsed direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy.View product →
Laser modelsPGL-H-655655 nm Pulsed LasersThe PGL-H-655 is a 655 nm pulsed direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample.View product →
Laser modelsPGL-H-808808 nm CW LasersThe PGL-H-808 is a 808 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Tuning changes the selected output wavelength so spectral features can be scanned with the same source. The tuning band specifies which lines can be reached; linewidth describes the width of the selected line.View product →
Laser modelsPGL-H-980980 nm Pulsed LasersThe PGL-H-980 is a 980 nm pulsed direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample.View product →
Laser modelsPGL-H1473 nm CW LasersThe PGL-H1 is a 473 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-H1-10641064 nm CW LasersThe PGL-H1-1064 is a 1064 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-H1-473473 nm CW LasersThe PGL-H1-473 is a 473 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-H1-561561 nm CW LasersThe PGL-H1-561 is a 561 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-H1-589589 nm CW LasersThe PGL-H1-589 is a 589 nm continuous-wave solid-state laser. Light is amplified in a solid gain medium inside an optical resonator. The resonator feeds light back through that medium to build the laser beam. The pump arrangement and cooling determine how energy is supplied and waste heat is removed. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-H1-594594 nm CW LasersThe PGL-H1-594 is a 594 nm continuous-wave laser module. The optical head packages the light source for integration into an instrument. Its specified driver and cooling arrangement determine how the module is powered and stabilized. Waste heat is removed through the specified mounting or cooling interface. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsPGL-LF-10601060 nm CW LasersThe PGL-LF-1060 is a 1060 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
Laser modelsPGL-LF-10641064 nm CW LasersThe PGL-LF-1064 is a 1064 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-LF-13101310 nm CW LasersThe PGL-LF-1310 is a 1310 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
Laser modelsPGL-LF-14501450 nm Fiber LasersThe PGL-LF-1450 is a 1450 nm direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength.View product →
Laser modelsPGL-LF-14801480 nm CW LasersThe PGL-LF-1480 is a 1480 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Tuning changes the selected output wavelength so spectral features can be scanned with the same source. The tuning band specifies which lines can be reached; linewidth describes the width of the selected line.View product →
Laser modelsPGL-LF-15501550 nm CW LasersThe PGL-LF-1550 is a 1550 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
Laser modelsPGL-LF-405405 nm CW LasersThe PGL-LF-405 is a 405 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
Laser modelsPGL-LF-450450 nm CW LasersThe PGL-LF-450 is a 450 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
Laser modelsPGL-LF-520520 nm CW LasersThe PGL-LF-520 is a 520 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
Laser modelsPGL-LF-635635 nm CW LasersThe PGL-LF-635 is a 635 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-LF-637637 nm CW LasersThe PGL-LF-637 is a 637 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
Laser modelsPGL-LF-638638 nm CW LasersThe PGL-LF-638 is a 638 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
Laser modelsPGL-LF-639639 nm CW LasersThe PGL-LF-639 is a 639 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
Laser modelsPGL-LF-640640 nm CW LasersThe PGL-LF-640 is a 640 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-LF-642642 nm CW LasersThe PGL-LF-642 is a 642 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
Laser modelsPGL-LF-650650 nm CW LasersThe PGL-LF-650 is a 650 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
Laser modelsPGL-LF-655656 nm Pulsed LasersThe PGL-LF-655 is a 656 nm pulsed direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy.View product →
Laser modelsPGL-LF-655655 nm Pulsed LasersThe PGL-LF-655 is a 655 nm pulsed direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample.View product →
Laser modelsPGL-LF-660660 nm CW LasersThe PGL-LF-660 is a 660 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsPGL-LF-808808 nm CW LasersThe PGL-LF-808 is a 808 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Tuning changes the selected output wavelength so spectral features can be scanned with the same source. The tuning band specifies which lines can be reached; linewidth describes the width of the selected line.View product →
Laser modelsPGL-LF-830830 nm CW LasersThe PGL-LF-830 is a 830 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
Laser modelsPGL-LF-845845 nm CW LasersThe PGL-LF-845 is a 845 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →

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