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Lasers model catalog

Browse 3,778 canonical product destinations across 12 product families. Page 23 lists models 2,641–2,760.

Laser modelsMLL-U-532532 nm Single-Frequency LasersThe MLL-U-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. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsMLL-U-532-SM532 nm Fiber LasersThe MLL-U-532-SM is a 532 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 modelsMLL-U-550550 nm Fiber LasersThe MLL-U-550 is a 550 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 modelsMLL-U-561561 nm CW LasersThe MLL-U-561 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.View product →
Laser modelsMLL-U-561-SM561 nm CW LasersThe MLL-U-561-SM is a 561 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 modelsMLL-U-577577 nm CW LasersThe MLL-U-577 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.View product →
Laser modelsMLL-U-588588 nm CW LasersThe MLL-U-588 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.View product →
Laser modelsMLL-U-588-SM588 nm CW LasersThe MLL-U-588-SM is a 588 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 modelsMLL-U-589589 nm CW LasersThe MLL-U-589 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.View product →
Laser modelsMLL-U-589-SM589 nm CW LasersThe MLL-U-589-SM is a 589 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 modelsMLL-U-671671 nm CW LasersThe MLL-U-671 is a 671 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 modelsMLL-U-671-SM671 nm CW LasersThe MLL-U-671-SM is a 671 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 modelsMLL-U-914-SU914 nm CW LasersThe MLL-U-914-SU is a 914 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 modelsMLL-U-946-SU946 nm CW LasersThe MLL-U-946-SU is a 946 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 modelsMLL-V-532532 nm CW LasersThe MLL-V-532 is a 532 nm continuous-wave laser source. 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 modelsMLL-V-532-SM532 nm Fiber LasersThe MLL-V-532-SM is a 532 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. 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 modelsMLL-V-671671 nm CW LasersThe MLL-V-671 is a 671 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 modelsMLL-V-671-SM671 nm CW LasersThe MLL-V-671-SM is a 671 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. 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 modelsMLL-W-473473 nm CW LasersThe MLL-W-473 is a 473 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 modelsMLL-W-473-SM473 nm CW LasersThe MLL-W-473-SM is a 473 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. 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 modelsMLL-XF-808808 nm CW LasersThe MLL-XF-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. 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 modelsMLL-XS-561561 nm CW LasersThe MLL-XS-561 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.View product →
Laser modelsMPL-355355 nm CW LasersThe MPL-355 is a 355 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 modelsMPL-355 (FC)355 nm Pulsed LasersThe MPL-355 (FC) is a 355 nm nanosecond 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. 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 lasting approximately 0.6 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-E-15351535 nm Pulsed LasersThe MPL-E-1535 is a 1535 nm pulsed laser source. 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 modelsMPL-F-10301030 nm Pulsed LasersThe MPL-F-1030 is a 1030 nm nanosecond 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. Pulses lasting approximately 6 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-F-349349 nm Pulsed LasersThe MPL-F-349 is a 349 nm nanosecond 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. 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 modelsMPL-F-351351 nm Pulsed LasersThe MPL-F-351 is a 351 nm nanosecond 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. At the nominal 1 kHz repetition rate, pulses lasting approximately 4 ns arrive about 1 ms apart.View product →
Laser modelsMPL-F-355355 nm Pulsed LasersThe MPL-F-355 is a 355 nm nanosecond 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. 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 lasting approximately 5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-FL-355355 nm Fiber LasersThe MPL-FL-355 is a 355 nm nanosecond 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. Pulses lasting approximately 5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-FN-236236 nm Pulsed LasersThe MPL-FN-236 is a 236 nm nanosecond 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. Pulses lasting approximately 1.4 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-FN-266266 nm Pulsed LasersThe MPL-FN-266 is a 266 nm nanosecond 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. 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 lasting approximately 0.6 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-FN-278-L/1uJ278 nm Pulsed LasersThe MPL-FN-278-L/1uJ is a 278 nm pulsed laser source. 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 modelsMPL-FN-315315 nm Pulsed LasersThe MPL-FN-315 is a 315 nm nanosecond 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. Pulses lasting approximately 1.6 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-FN-355355 nm Pulsed LasersThe MPL-FN-355 is a 355 nm nanosecond 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. 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 lasting approximately 0.6 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-FN-556556 nm Pulsed LasersThe MPL-FN-556 is a 556 nm nanosecond 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. Pulses lasting approximately 35 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-H-10471047 nm Pulsed LasersThe MPL-H-1047 is a 1047 nm nanosecond 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. Pulses lasting approximately 6 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-H-10531053 nm Pulsed LasersThe MPL-H-1053 is a 1053 nm nanosecond 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. Pulses lasting approximately 10 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-H-10641064 nm Pulsed LasersThe MPL-H-1064 is a 1064 nm nanosecond 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. 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 modelsMPL-H-1064A1064 nm Pulsed LasersThe MPL-H-1064A is a 1064 nm nanosecond 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. 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 lasting approximately 1.5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-H-13131313 nm Pulsed LasersThe MPL-H-1313 is a 1313 nm nanosecond 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. Pulses lasting approximately 18 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-H-13191319 nm Pulsed LasersThe MPL-H-1319 is a 1319 nm nanosecond 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. Pulses lasting approximately 15 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-H-15731573 nm Pulsed LasersThe MPL-H-1573 is a 1573 nm nanosecond 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 modelsMPL-H-523.5523.5 nm Pulsed LasersThe MPL-H-523.5 is a 523.5 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 modelsMPL-H-526.5526.5 nm Pulsed LasersThe MPL-H-526.5 is a 526.5 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. 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 modelsMPL-H-532532 nm Pulsed LasersThe MPL-H-532 is a 532 nm nanosecond 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. 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 modelsMPL-H-532A532 nm Pulsed LasersThe MPL-H-532A is a 532 nm nanosecond 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. 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 lasting approximately 1.3 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-H-656.5656.5 nm Pulsed LasersThe MPL-H-656.5 is a 656.5 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 modelsMPL-III-10641064 nm Pulsed LasersThe MPL-III-1064 is a 1064 nm nanosecond 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. 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 modelsMPL-III-1064A1064 nm Pulsed LasersThe MPL-III-1064A is a 1064 nm nanosecond 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. 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 lasting approximately 1.5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-III-532532 nm Pulsed LasersThe MPL-III-532 is a 532 nm nanosecond 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. 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 modelsMPL-III-532A532 nm Pulsed LasersThe MPL-III-532A is a 532 nm nanosecond 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. 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 lasting approximately 1.3 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-N-257257 nm Pulsed LasersThe MPL-N-257 is a 257 nm nanosecond 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. Pulses lasting approximately 5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-N-343343 nm Pulsed LasersThe MPL-N-343 is a 343 nm nanosecond 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. Pulses lasting approximately 7 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-N-515515 nm Pulsed LasersThe MPL-N-515 is a 515 nm nanosecond 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. Pulses lasting approximately 10 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-N-532532 nm Pulsed LasersThe MPL-N-532 is a 532 nm nanosecond 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 modelsMPL-Q-266266 nm Pulsed LasersThe MPL-Q-266 is a 266 nm nanosecond 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. 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 lasting approximately 1.3 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-Q-355355 nm Pulsed LasersThe MPL-Q-355 is a 355 nm nanosecond 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. 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 lasting approximately 1.3 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-Q1-266266 nm Pulsed LasersThe MPL-Q1-266 is a 266 nm nanosecond 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. 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. At the nominal 1 kHz repetition rate, pulses lasting approximately 1 ns arrive about 1 ms apart.View product →
Laser modelsMPL-Q1-266/10uJ266 nm Pulsed LasersThe MPL-Q1-266/10uJ is a 266 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.View product →
Laser modelsMPL-S-10301030 nm Pulsed LasersThe MPL-S-1030 is a 1030 nm nanosecond 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. Pulses lasting approximately 0.6 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-S-10641064 nm Pulsed LasersThe MPL-S-1064 is a 1064 nm nanosecond 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. 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 modelsMPL-S-1064-HF1064 nm Pulsed LasersThe MPL-S-1064-HF is a 1064 nm nanosecond 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 modelsMPL-S-1064-HP1064 nm Pulsed LasersThe MPL-S-1064-HP is a 1064 nm nanosecond 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. 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 modelsMPL-S-1064-LP1064 nm Pulsed LasersThe MPL-S-1064-LP is a 1064 nm nanosecond 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. 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 lasting 0.5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-S-1064A-HF1064 nm Pulsed LasersThe MPL-S-1064A-HF is a 1064 nm nanosecond 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. Pulses lasting approximately 0.5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-S-1064A-HP1064 nm Pulsed LasersThe MPL-S-1064A-HP is a 1064 nm nanosecond 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. 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 lasting approximately 0.5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-S-1064B-HP1064 nm Pulsed LasersThe MPL-S-1064B-HP is a 1064 nm nanosecond 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. 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 lasting approximately 0.7 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-S-213-HP213 nm Pulsed LasersThe MPL-S-213-HP is a 213 nm picosecond 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. Pulses lasting approximately 500 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-S-266-HP266 nm Pulsed LasersThe MPL-S-266-HP is a 266 nm nanosecond 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. 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 lasting approximately 0.4 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-S-266-LP266 nm Pulsed LasersThe MPL-S-266-LP is a 266 nm nanosecond 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. 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 lasting approximately 0.4 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-S-355-HP355 nm Pulsed LasersThe MPL-S-355-HP is a 355 nm nanosecond 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. 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 lasting approximately 0.4 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-S-355-LP355 nm Pulsed LasersThe MPL-S-355-LP is a 355 nm nanosecond 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. 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 lasting approximately 0.4 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-S-532-HF532 nm Pulsed LasersThe MPL-S-532-HF is a 532 nm nanosecond 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. Pulses lasting approximately 0.5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-S-532-HP532 nm Pulsed LasersThe MPL-S-532-HP is a 532 nm nanosecond 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. 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 modelsMPL-S-532-LP532 nm Pulsed LasersThe MPL-S-532-LP is a 532 nm nanosecond 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. 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 lasting approximately 0.5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-S-532A-HP532 nm Pulsed LasersThe MPL-S-532A-HP is a 532 nm nanosecond 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. 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 lasting approximately 0.5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-S-532B-HP532 nm Pulsed LasersThe MPL-S-532B-HP is a 532 nm nanosecond 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. 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 lasting approximately 0.7 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-S-946946 nm Pulsed LasersThe MPL-S-946 is a 946 nm nanosecond 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. Pulses lasting approximately 2.6 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-T-10641064 nm Pulsed LasersThe MPL-T-1064 is a 1064 nm nanosecond 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. 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 modelsMPL-T-1064A1064 nm Pulsed LasersThe MPL-T-1064A is a 1064 nm nanosecond 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. 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 lasting approximately 1.5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-T-1064B1064 nm Pulsed LasersThe MPL-T-1064B is a 1064 nm nanosecond 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. 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 lasting 0.5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-T-15351535 nm Pulsed LasersThe MPL-T-1535 is a 1535 nm nanosecond 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 modelsMPL-T-532532 nm Pulsed LasersThe MPL-T-532 is a 532 nm nanosecond 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. 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 modelsMPL-T-532A532 nm Pulsed LasersThe MPL-T-532A is a 532 nm nanosecond 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. 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 lasting approximately 1.3 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-T-532B532 nm Pulsed LasersThe MPL-T-532B is a 532 nm nanosecond 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. 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 lasting approximately 0.5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-U-1047-SU1047 nm Pulsed LasersThe MPL-U-1047-SU is a 1047 nm nanosecond 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. Pulses lasting approximately 10 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-U-1053-SU1053 nm Pulsed LasersThe MPL-U-1053-SU is a 1053 nm nanosecond 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. 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 lasting approximately 10 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-U-1064-SU1064 nm Pulsed LasersThe MPL-U-1064-SU is a 1064 nm nanosecond 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. 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 lasting approximately 5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-U-1064A-SU1064 nm Pulsed LasersThe MPL-U-1064A-SU is a 1064 nm nanosecond 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. 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 lasting approximately 1.5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-U-1313-SU1313 nm Pulsed LasersThe MPL-U-1313-SU is a 1313 nm nanosecond 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. 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 lasting approximately 15 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-U-1319-SU1319 nm Pulsed LasersThe MPL-U-1319-SU is a 1319 nm nanosecond 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. Pulses lasting approximately 15 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-U-1444-SU1444 nm Pulsed LasersThe MPL-U-1444-SU is a 1444 nm nanosecond 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. Pulses lasting approximately 24 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-U-473473 nm Pulsed LasersThe MPL-U-473 is a 473 nm nanosecond 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. 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 lasting approximately 2.2 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-U-523.5523.5 nm Pulsed LasersThe MPL-U-523.5 is a 523.5 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 modelsMPL-U-526.5526.5 nm Pulsed LasersThe MPL-U-526.5 is a 526.5 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. 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 modelsMPL-U-532532 nm Pulsed LasersThe MPL-U-532 is a 532 nm nanosecond 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. 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 modelsMPL-U-532A532 nm Pulsed LasersThe MPL-U-532A is a 532 nm nanosecond 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. 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 lasting approximately 1.3 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-U-532B532 nm Pulsed LasersThe MPL-U-532B is a 532 nm nanosecond 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. 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 modelsMPL-U-532C532 nm Pulsed LasersThe MPL-U-532C is a 532 nm nanosecond 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. 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 lasting approximately 0.5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-U-656.5656.5 nm Pulsed LasersThe MPL-U-656.5 is a 656.5 nm nanosecond 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. Pulses lasting approximately 15 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMPL-U-946-SU946 nm Pulsed LasersThe MPL-U-946-SU is a 946 nm nanosecond 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. Pulses lasting approximately 5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsMRL-604(FC)604 nm CW LasersThe MRL-604(FC) is a 604 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 modelsMRL-607(FC)607 nm CW LasersThe MRL-607(FC) is a 607 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 modelsMRL-622(FC)622 nm CW LasersThe MRL-622(FC) is a 622 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 modelsMRL-627(FC)627 nm CW LasersThe MRL-627(FC) is a 627 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 modelsMRL-631(FC)631 nm CW LasersThe MRL-631(FC) is a 631 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 modelsMRL-633(FC)633 nm CW LasersThe MRL-633(FC) is a 633 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 modelsMRL-635(FC)635 nm CW LasersThe MRL-635(FC) 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 modelsMRL-637(FC)637 nm CW LasersThe MRL-637(FC) 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 modelsMRL-637(Line)637 nm CW LasersThe MRL-637(Line) 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 modelsMRL-639(FC)639 nm CW LasersThe MRL-639(FC) is a 639 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 modelsMRL-639(Line)639 nm CW LasersThe MRL-639(Line) is a 639 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 modelsMRL-640(FC)640 nm CW LasersThe MRL-640(FC) is a 640 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 modelsMRL-640(Line)640 nm CW LasersThe MRL-640(Line) is a 640 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 modelsMRL-642(FC)642 nm CW LasersThe MRL-642(FC) is a 642 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 modelsMRL-655(FC)655 nm CW LasersThe MRL-655(FC) is a 655 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 modelsMRL-656.5(FC)656.5 nm CW LasersThe MRL-656.5(FC) is a 656.5 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 modelsMRL-660(FC)660 nm CW LasersThe MRL-660(FC) 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 modelsMRL-666(FC)666 nm CW LasersThe MRL-666(FC) is a 666 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 →

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Lasers model catalog