Server-rendered product directory
Lasers model catalog
Browse 3,778 canonical product destinations across 12 product families. Page 19 lists models 2,161–2,280.
- Laser modelsMGL-W-589A589 nm CW LasersThe MGL-W-589A 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. 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 modelsMGL-W-594A594 nm CW LasersThe MGL-W-594A is a 594 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 modelsMGL-Z-532532 nm CW LasersThe MGL-Z-532 is a 532 nm continuous-wave diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
- Laser modelsMicro Raman Spectrum Measurement SystemSpectrum AnalysisIt combines micro system and Raman system which facilitates the Raman micro area detection.View product →
- Laser modelsMicro Raman Spectrum Measurement SystemSpectrum AnalysisIt combines micro system and Raman system which facilitates the Raman micro area detection.View product →
- Laser modelsMicroscopic Imaging LaserMulti-wavelength LasersThe Microscopic Imaging Laser is a 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 modelsMIL-1020(FC)1020 nm Application SystemsThe MIL-1020(FC) is a 1020 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 modelsMIL-1030(FC)1030 nm Application SystemsThe MIL-1030(FC) is a 1030 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 modelsMIL-1035(FC)1035 nm Application SystemsThe MIL-1035(FC) is a 1035 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 modelsMIL-1040(FC)1040 nm Application SystemsThe MIL-1040(FC) is a 1040 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 modelsMIL-1047(FC)1047 nm Application SystemsThe MIL-1047(FC) is a 1047 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 modelsMIL-1053(FC)1053 nm Application SystemsThe MIL-1053(FC) is a 1053 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 modelsMIL-1073(FC)1073 nm Application SystemsThe MIL-1073(FC) is a 1073 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 modelsMIL-1085(FC)1085 nm Application SystemsThe MIL-1085(FC) is a 1085 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 modelsMIL-1105(FC)1105 nm Application SystemsThe MIL-1105(FC) is a 1105 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 modelsMIL-1112(FC)1112 nm Application SystemsThe MIL-1112(FC) is a 1112 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 modelsMIL-1122(FC)1122 nm Application SystemsThe MIL-1122(FC) is a 1122 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 modelsMIL-1177(FC)1177 nm Application SystemsThe MIL-1177(FC) is a 1177 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 modelsMIL-1190(FC)1190 nm Application SystemsThe MIL-1190(FC) is a 1190 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 modelsMIL-1313(FC)1313 nm Application SystemsThe MIL-1313(FC) is a 1313 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 modelsMIL-1319(FC)1319 nm Application SystemsThe MIL-1319(FC) is a 1319 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 modelsMIL-1335(FC)1335 nm Application SystemsThe MIL-1335(FC) is a 1335 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 modelsMIL-1338(FC)1338 nm Application SystemsThe MIL-1338(FC) is a 1338 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 modelsMIL-1342(FC)1342 nm Application SystemsThe MIL-1342(FC) is a 1342 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 modelsMIL-1357(FC)1357 nm Application SystemsThe MIL-1357(FC) is a 1357 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 modelsMIL-1413(FC)1413 nm Application SystemsThe MIL-1413(FC) is a 1413 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 modelsMIL-1444(FC)1444 nm Application SystemsThe MIL-1444(FC) is a 1444 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 modelsMIL-1580(FC)1580 nm CW LasersThe MIL-1580(FC) is a 1580 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 modelsMIL-1720(FC)1720 nm Application SystemsThe MIL-1720(FC) is a 1720 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 modelsMIL-1910(FC)1910 nm Application SystemsThe MIL-1910(FC) is a 1910 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 modelsMIL-1990(FC)1990 nm Application SystemsThe MIL-1990(FC) is a 1990 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 modelsMIL-2096(FC)2096 nm Application SystemsThe MIL-2096(FC) is a 2096 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 modelsMIL-2117(FC)2117 nm Application SystemsThe MIL-2117(FC) is a 2117 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 modelsMIL-2120(FC)2120 nm Application SystemsThe MIL-2120(FC) is a 2120 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 modelsMIL-2124(FC)2124 nm Application SystemsThe MIL-2124(FC) is a 2124 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 modelsMIL-2128(FC)2128 nm Application SystemsThe MIL-2128(FC) is a 2128 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 modelsMIL-2130(FC)2130 nm Application SystemsThe MIL-2130(FC) is a 2130 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 modelsMIL-678(FC)678 nm Application SystemsThe MIL-678(FC) is a 678 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 modelsMIL-912(FC)912 nm Application SystemsThe MIL-912(FC) is a 912 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 modelsMIL-914(FC)914 nm Application SystemsThe MIL-914(FC) is a 914 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 modelsMIL-946(FC)946 nm Application SystemsThe MIL-946(FC) is a 946 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 modelsMIL-D-10641064 nm CW LasersThe MIL-D-1064 is a 1064 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 modelsMIL-F-10301030 nm CW LasersThe MIL-F-1030 is a 1030 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 modelsMIL-F-10731073 nm Single-Frequency LasersThe MIL-F-1073 is a 1073 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 modelsMIL-F-11051105 nm CW LasersThe MIL-F-1105 is a 1105 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 modelsMIL-FN-13571357 nm CW LasersThe MIL-FN-1357 is a 1357 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 modelsMIL-FN-912912 nm CW LasersThe MIL-FN-912 is a 912 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 modelsMIL-H-10401040 nm Fiber LasersThe MIL-H-1040 is a 1040 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 modelsMIL-H-10471047 nm CW LasersThe MIL-H-1047 is a 1047 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 modelsMIL-H-10531053 nm Pulsed LasersThe MIL-H-1053 is a 1053 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 modelsMIL-H-10641064 nm CW LasersThe MIL-H-1064 is a 1064 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 modelsMIL-H-11121112 nm CW LasersThe MIL-H-1112 is a 1112 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 modelsMIL-H-11221122 nm CW LasersThe MIL-H-1122 is a 1122 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 modelsMIL-H-11771177 nm CW LasersThe MIL-H-1177 is a 1177 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 modelsMIL-H-13131313 nm CW LasersThe MIL-H-1313 is a 1313 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 modelsMIL-H-13351335 nm CW LasersThe MIL-H-1335 is a 1335 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 modelsMIL-H-13381338 nm CW LasersThe MIL-H-1338 is a 1338 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 modelsMIL-H-13421342 nm CW LasersThe MIL-H-1342 is a 1342 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 modelsMIL-H-14131413 nm CW LasersThe MIL-H-1413 is a 1413 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 modelsMIL-H-912912 nm CW LasersThe MIL-H-912 is a 912 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 modelsMIL-H-914914 nm CW LasersThe MIL-H-914 is a 914 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 modelsMIL-H-946946 nm CW LasersThe MIL-H-946 is a 946 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 modelsMIL-N-10641064 nm CW LasersThe MIL-N-1064 is a 1064 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 modelsMIL-N-13421342 nm CW LasersThe MIL-N-1342 is a 1342 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 modelsMIL-N-16451645 nm CW LasersThe MIL-N-1645 is a 1645 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 modelsMIL-N-19101910 nm CW LasersThe MIL-N-1910 is a 1910 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 modelsMIL-N-19401940 nm CW LasersThe MIL-N-1940 is a 1940 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 modelsMIL-N-19901985 nm CW LasersThe MIL-N-1990 is a 1985 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 modelsMIL-PS-29102910 nm Pulsed LasersThe MIL-PS-2910 is a 2910 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 modelsMIL-PS-2910-42352910 nm Pulsed LasersThe MIL-PS-2910-4235 is a 2910 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. 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 15 MHz repetition rate, pulses shorter than 700 ps arrive about 66.67 ns apart.View product →
- Laser modelsMIL-PS-32053200 nm Pulsed LasersThe MIL-PS-3205 is a 3200 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 modelsMIL-PS-34403440 nm Pulsed LasersThe MIL-PS-3440 is a 3440 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. 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 15 MHz repetition rate, pulses shorter than 700 ps arrive about 66.67 ns apart.View product →
- Laser modelsMIL-PS-36403640 nm Pulsed LasersThe MIL-PS-3640 is a 3640 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. 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 15 MHz repetition rate, pulses shorter than 700 ps arrive about 66.67 ns apart.View product →
- Laser modelsMIL-PS-38103800 nm Pulsed LasersThe MIL-PS-3810 is a 3800 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 modelsMIL-PS-39673967 nm Pulsed LasersThe MIL-PS-3967 is a 3967 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. 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 15 MHz repetition rate, pulses shorter than 700 ps arrive about 66.67 ns apart.View product →
- Laser modelsMIL-PS-40004000 nm Pulsed LasersThe MIL-PS-4000 is a 4000 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. 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 15 MHz repetition rate, pulses shorter than 700 ps arrive about 66.67 ns apart.View product →
- Laser modelsMIL-PS-42354235 nm Pulsed LasersThe MIL-PS-4235 is a 4235 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. 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 15 MHz repetition rate, pulses shorter than 700 ps arrive about 66.67 ns apart.View product →
- Laser modelsMIL-S-10641064 nm CW LasersThe MIL-S-1064 is a 1064 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 modelsMIL-S-1064-OEM1064 nm CW LasersThe MIL-S-1064-OEM is a 1064 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
- Laser modelsMIL-S-1064-SM1064 nm Fiber LasersThe MIL-S-1064-SM is a 1064 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 modelsMIL-T-10641064 nm CW LasersThe MIL-T-1064 is a 1064 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 modelsMIL-T-1064-SM1064 nm Fiber LasersThe MIL-T-1064-SM is a 1064 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 modelsMIL-T-11121112 nm CW LasersThe MIL-T-1112 is a 1112 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 modelsMIL-U-1047-SU1047 nm CW LasersThe MIL-U-1047-SU is a 1047 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 modelsMIL-U-1053-SU1053 nm Pulsed LasersThe MIL-U-1053-SU is a 1053 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 modelsMIL-U-1064-SU1064 nm CW LasersThe MIL-U-1064-SU is a 1064 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 modelsMIL-U-1085-SU1085 nm CW LasersThe MIL-U-1085-SU is a 1085 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 modelsMIL-U-1112-SU1112 nm CW LasersThe MIL-U-1112-SU is a 1112 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 modelsMIL-U-1122-SU1122 nm CW LasersThe MIL-U-1122-SU is a 1122 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 modelsMIL-U-1313-SU1313 nm CW LasersThe MIL-U-1313-SU is a 1313 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 modelsMIL-U-1319-FL1319 nm CW LasersThe MIL-U-1319-FL is a 1319 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 modelsMIL-U-1342-SU1342 nm CW LasersThe MIL-U-1342-SU is a 1342 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 modelsMIL-U-1444-SU1444 nm CW LasersThe MIL-U-1444-SU is a 1444 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 modelsMIL-U-914-SU914 nm CW LasersThe MIL-U-914-SU is a 914 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 modelsMIL-U-946-SU946 nm CW LasersThe MIL-U-946-SU is a 946 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 modelsMIL-V-10471047 nm CW LasersThe MIL-V-1047 is a 1047 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 modelsMIL-V-13191319 nm CW LasersThe MIL-V-1319 is a 1319 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 modelsMIL-V-13421342 nm CW LasersThe MIL-V-1342 is a 1342 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 modelsMIL-V-30003000 nm CW LasersThe MIL-V-3000 is a 3000 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 modelsMIL-V-31003100 nm CW LasersThe MIL-V-3100 is a 3100 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 modelsMIL-V-32003200 nm CW LasersThe MIL-V-3200 is a 3200 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 modelsMIL-V-33003300 nm CW LasersThe MIL-V-3300 is a 3300 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 modelsMIL-V-33903390 nm CW LasersThe MIL-V-3390 is a 3390 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 modelsMIL-V-36003600 nm CW LasersThe MIL-V-3600 is a 3600 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 modelsMIL-V-37003700 nm CW LasersThe MIL-V-3700 is a 3700 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 modelsMIL-V-38003800 nm CW LasersThe MIL-V-3800 is a 3800 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 modelsMIL-V-39003900 nm CW LasersThe MIL-V-3900 is a 3900 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 modelsMIL-V-41004100 nm CW LasersThe MIL-V-4100 is a 4100 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 modelsMIL-W-11051105 nm CW LasersThe MIL-W-1105 is a 1105 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 modelsMIL-W-1319A1319 nm CW LasersThe MIL-W-1319A is a 1319 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 modelsMIL-W-15501550 nm CW LasersThe MIL-W-1550 is a 1550 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
- Laser modelsMIL-W-15731573 nm CW LasersThe MIL-W-1573 is a 1573 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 modelsMIL-W-16001600 nm CW LasersThe MIL-W-1600 is a 1600 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 modelsMIL-W-17001700 nm CW LasersThe MIL-W-1700 is a 1700 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 modelsMIL-W-18341834 nm CW LasersThe MIL-W-1834 is a 1834 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 modelsMIL-W-19101910 nm CW LasersThe MIL-W-1910 is a 1910 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 modelsMIL-W-19401940 nm CW LasersThe MIL-W-1940 is a 1940 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 modelsMIL-W-19901985 nm CW LasersThe MIL-W-1990 is a 1985 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 modelsMIL-W-20962096 nm CW LasersThe MIL-W-2096 is a 2096 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 modelsMIL-W-21172117 nm CW LasersThe MIL-W-2117 is a 2117 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 →