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Lasers model catalog

Browse 3,778 canonical product destinations across 12 product families. Page 8 lists models 841–960.

Laser modelsFC-W-375C375 nm Fiber LasersThe FC-W-375C is a 375 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. 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 modelsFC-W-375H-II375 nm Fiber LasersThe FC-W-375H-II is a 375 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. 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 modelsFC-W-405H-II405 nm Fiber LasersThe FC-W-405H-II 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. 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 modelsFC-W-444C444 nm Application SystemsThe FC-W-444C is a 444 nm 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.View product →
Laser modelsFC-W-445C445 nm Fiber LasersThe FC-W-445C 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. 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. 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 modelsFC-W-445H-II445 nm Fiber LasersThe FC-W-445H-II 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. 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. 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 modelsFC-W-447C447 nm Fiber LasersThe FC-W-447C 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. 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. 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 modelsFC-W-447H-II447 nm Fiber LasersThe FC-W-447H-II 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. 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. 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 modelsFC-W-450C450 nm Fiber LasersThe FC-W-450C 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. 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 modelsFC-W-450H-II-100W450 nm Fiber LasersThe FC-W-450H-II-100W is a 450 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 modelsFC-W-450H-II-200W450 nm Fiber LasersThe FC-W-450H-II-200W is a 450 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 modelsFC-W-450H-II-500W450 nm Fiber LasersThe FC-W-450H-II-500W is a 450 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 modelsFC-W-450H-II-50W450 nm Fiber LasersThe FC-W-450H-II-50W 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. 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 modelsFC-W-455C455 nm Application SystemsThe FC-W-455C is a 455 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 modelsFC-W-460C460 nm Fiber LasersThe FC-W-460C is a 460 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 modelsFC-W-460H-II460 nm Fiber LasersThe FC-W-460H-II is a 460 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 modelsFC-W-462C462 nm Fiber LasersThe FC-W-462C is a 462 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 modelsFC-W-462H-II462 nm Fiber LasersThe FC-W-462H-II is a 462 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 modelsFC-W-520520 nm Fiber LasersThe FC-W-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. 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 modelsFC-W-635635 nm Fiber LasersThe FC-W-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. 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 modelsFC-W-637637 nm Fiber LasersThe FC-W-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. 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 modelsFC-W-638/450C638 nm Application SystemsThe FC-W-638/450C is a 638 nm 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.View product →
Laser modelsFC-W-638/525/450/1064/1470C638 nm Application SystemsThe FC-W-638/525/450/1064/1470C is a 638 nm 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.View product →
Laser modelsFC-W-638/525/450/808/1064C638 nm Application SystemsThe FC-W-638/525/450/808/1064C is a 638 nm 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.View product →
Laser modelsFC-W-638/525/450/808/1550C638 nm Application SystemsThe FC-W-638/525/450/808/1550C is a 638 nm 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.View product →
Laser modelsFC-W-638/525/450/940/980C638 nm Fiber LasersThe FC-W-638/525/450/940/980C 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. 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 modelsFC-W-638/525/450/980/808C638 nm Application SystemsThe FC-W-638/525/450/980/808C is a 638 nm 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.View product →
Laser modelsFC-W-638/525/450C638 nm Application SystemsThe FC-W-638/525/450C is a 638 nm 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.View product →
Laser modelsFC-W-638/525C638 nm Application SystemsThe FC-W-638/525C is a 638 nm 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.View product →
Laser modelsFC-W-638/808/980/1064C638 nm Application SystemsThe FC-W-638/808/980/1064C is a 638 nm 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.View product →
Laser modelsFC-W-638/808/980/1470C638 nm Application SystemsThe FC-W-638/808/980/1470C is a 638 nm 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.View product →
Laser modelsFC-W-638/808/980C638 nm Application SystemsThe FC-W-638/808/980C is a 638 nm 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.View product →
Laser modelsFC-W-638/980/1064C638 nm Application SystemsThe FC-W-638/980/1064C is a 638 nm 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.View product →
Laser modelsFC-W-638/980/1550C638 nm Application SystemsThe FC-W-638/980/1550C is a 638 nm 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.View product →
Laser modelsFC-W-640640 nm Fiber LasersThe FC-W-640 is a 640 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. 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 modelsFC-W-655655 nm Fiber LasersThe FC-W-655 is a 655 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. 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 modelsFC-W-793793 nm Fiber LasersThe FC-W-793 is a 793 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 modelsFC-W-793H793 nm Fiber LasersThe FC-W-793H is a 793 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 modelsFC-W-808/810808 nm Fiber LasersThe FC-W-808/810 is a 808 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. 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 modelsFC-W-808H808 nm Fiber LasersThe FC-W-808H is a 808 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. 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 modelsFC-W-880880 nm Application SystemsThe FC-W-880 is a 880 nm 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.View product →
Laser modelsFC-W-880/885A880 nm Application SystemsThe FC-W-880/885A is a 880 nm 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.View product →
Laser modelsFC-W-880H880 nm Application SystemsThe FC-W-880H is a 880 nm 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.View product →
Laser modelsFC-W-915915 nm Fiber LasersThe FC-W-915 is a 915 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. 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 modelsFC-W-915H915 nm Application SystemsThe FC-W-915H is a 915 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. 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 modelsFC-W-938/940938 nm Application SystemsThe FC-W-938/940 is a 938 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. 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 modelsFC-W-940H940 nm Application SystemsThe FC-W-940H is a 940 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. 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 modelsFC-W-976976 nm Fiber LasersThe FC-W-976 is a 976 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. 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 modelsFC-W-976/980A976 nm Application SystemsThe FC-W-976/980A is a 976 nm 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.View product →
Laser modelsFC-W-976/980H-110-150W976 nm Application SystemsThe FC-W-976/980H-110-150W is a 976 nm 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.View product →
Laser modelsFC-W-976/980H-50~100W976 nm Application SystemsThe FC-W-976/980H-50~100W is a 976 nm 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.View product →
Laser modelsFC-W-976H976 nm Fiber LasersThe FC-W-976H is a 976 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. 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 modelsFC-W-980980 nm Application SystemsThe FC-W-980 is a 980 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. 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 modelsFC-W-980H980 nm Application SystemsThe FC-W-980H is a 980 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. 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 modelsFiber Optic SpectrometerSpectrum AnalysisIt can be used to measure wavelength and line width of laser, LED and common light source, can accurately obtain the spectral characteristics of the light source which is being tested.View product →
Laser modelsFL-1014-LN-L1014 nm Fiber LasersThe FL-1014-LN-L is a 1014 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1014-SLM1014 nm Fiber LasersThe FL-1014-SLM is a 1014 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1018-CW1018 nm Fiber LasersThe FL-1018-CW is a 1018 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-1018-LN-L1018 nm Fiber LasersThe FL-1018-LN-L is a 1018 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1018-SLM1018 nm Fiber LasersThe FL-1018-SLM is a 1018 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1027-LN-L1027 nm Fiber LasersThe FL-1027-LN-L is a 1027 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1027-SLM1027 nm Fiber LasersThe FL-1027-SLM is a 1027 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1030-CW1030 nm Fiber LasersThe FL-1030-CW is a 1030 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-1030-LN-L1030 nm Fiber LasersThe FL-1030-LN-L is a 1030 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1030-Nano1030 nm Fiber LasersThe FL-1030-Nano is a 1030 nm pulsed fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-1030-Pico1030 nm Fiber LasersThe FL-1030-Pico is a 1030 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-1030-PS1030 nm Fiber LasersThe FL-1030-PS is a 1030 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. A semiconductor saturable absorber mirror (SESAM) becomes less absorbing at higher intensity, helping short pulses build through passive mode locking. Pulses shorter than 10 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsFL-1030-PS-Seed1030 nm Fiber LasersThe FL-1030-PS-Seed is a 1030 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. A semiconductor saturable absorber mirror (SESAM) becomes less absorbing at higher intensity, helping short pulses build through passive mode locking. Pulses shorter than 10 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsFL-1030-S1030 nm Fiber LasersThe FL-1030-S is a 1030 nm nanosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-1030-SLM1030 nm Fiber LasersThe FL-1030-SLM is a 1030 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1040-CW1040 nm Fiber LasersThe FL-1040-CW is a 1040 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-1040-LN-L1040 nm Fiber LasersThe FL-1040-LN-L is a 1040 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1040-SLM1040 nm Fiber LasersThe FL-1040-SLM is a 1040 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1050-CW1050 nm Fiber LasersThe FL-1050-CW is a 1050 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-1050-LN-L1050 nm Fiber LasersThe FL-1050-LN-L is a 1050 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1050-SLM1050 nm Fiber LasersThe FL-1050-SLM is a 1050 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1053-CW1053 nm Fiber LasersThe FL-1053-CW is a 1053 nm pulsed fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-1053-LN-H1053 nm Fiber LasersThe FL-1053-LN-H is a 1053 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1053-LN-L1053 nm Fiber LasersThe FL-1053-LN-L is a 1053 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1053-SLM1053 nm Fiber LasersThe FL-1053-SLM is a 1053 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1060-CW1060 nm Fiber LasersThe FL-1060-CW is a 1060 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-10641064 nm Application SystemsThe FL-1064 is a 1064 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. A semiconductor saturable absorber mirror (SESAM) becomes less absorbing at higher intensity, helping short pulses build through passive mode locking. Pulses shorter than 10 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsFL-1064-AO1064 nm Fiber LasersThe FL-1064-AO is a 1064 nm nanosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-1064-LN-H1064 nm Fiber LasersThe FL-1064-LN-H is a 1064 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1064-LN-L1064 nm Fiber LasersThe FL-1064-LN-L is a 1064 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1064-Nano1064 nm Fiber LasersThe FL-1064-Nano is a 1064 nm nanosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-1064-Pico1064 nm Fiber LasersThe FL-1064-Pico is a 1064 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-1064-PS1064 nm Fiber LasersThe FL-1064-PS is a 1064 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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. Pulses shorter than 10 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsFL-1064-PS-Seed1064 nm Fiber LasersThe FL-1064-PS-Seed is a 1064 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. A semiconductor saturable absorber mirror (SESAM) becomes less absorbing at higher intensity, helping short pulses build through passive mode locking. Pulses shorter than 10 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsFL-1064-S1064 nm Fiber LasersThe FL-1064-S is a 1064 nm nanosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-1064-SLM1064 nm Fiber LasersThe FL-1064-SLM is a 1064 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1064-SLM-H1064 nm Fiber LasersThe FL-1064-SLM-H is a 1064 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1070-CW1070 nm Fiber LasersThe FL-1070-CW is a 1070 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-1070-Pico1070 nm Fiber LasersThe FL-1070-Pico is a 1070 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-1080-CW1080 nm Fiber LasersThe FL-1080-CW is a 1080 nm fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment.View product →
Laser modelsFL-1080-LN-L1080 nm Fiber LasersThe FL-1080-LN-L is a 1080 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1080-Nano1080 nm Fiber LasersThe FL-1080-Nano is a 1080 nm nanosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-1080-Pico1080 nm Fiber LasersThe FL-1080-Pico is a 1080 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-1080-SLM1080 nm Fiber LasersThe FL-1080-SLM is a 1080 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1090-CW1090 nm Fiber LasersThe FL-1090-CW is a 1090 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-1100-CW1100 nm Fiber LasersThe FL-1100-CW is a 1100 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-1100-LN-L1100 nm Fiber LasersThe FL-1100-LN-L is a 1100 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1100-SLM1100 nm Fiber LasersThe FL-1100-SLM is a 1100 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1120-CW1120 nm Fiber LasersThe FL-1120-CW is a 1120 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-1120-LN-L1120 nm Fiber LasersThe FL-1120-LN-L is a 1120 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1120-SLM1120 nm Fiber LasersThe FL-1120-SLM is a 1120 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1178-CW1178 nm Fiber LasersThe FL-1178-CW is a 1178 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-1240-CW1240 nm Fiber LasersThe FL-1240-CW is a 1240 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-1270-CW1270 nm Fiber LasersThe FL-1270-CW is a 1270 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-1310-CW1310 nm Fiber LasersThe FL-1310-CW is a 1310 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-1484-CW1484 nm Fiber LasersThe FL-1484-CW is a 1484 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-1530-SLM1530 nm Fiber LasersThe FL-1530-SLM is a 1530 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1540-SLM1540 nm Fiber LasersThe FL-1540-SLM is a 1540 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1550-AO1550 nm Fiber LasersThe FL-1550-AO is a 1550 nm nanosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-1550-CW1550 nm Fiber LasersThe FL-1550-CW is a 1550 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-1550-LN-L1550 nm Fiber LasersThe FL-1550-LN-L is a 1550 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1550-Nano1550 nm Fiber LasersThe FL-1550-Nano is a 1550 nm nanosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-1550-Pico1550 nm Fiber LasersThe FL-1550-Pico is a 1550 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-1550-PS1550 nm Fiber LasersThe FL-1550-PS is a 1550 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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. Pulses shorter than 10 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsFL-1550-S1550 nm Fiber LasersThe FL-1550-S is a 1550 nm nanosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 →

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