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Lasers model catalog

Browse 3,778 canonical product destinations across 12 product families. Page 10 lists models 1,081–1,200.

Laser modelsHPL-1064A-PB1064 nm Pulsed LasersThe HPL-1064A-PB is a 1064 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. At the nominal 0.5 kHz repetition rate, pulses lasting approximately 10 ns arrive about 2 ms apart.View product →
Laser modelsHPL-1064B-PA1064 nm Pulsed LasersThe HPL-1064B-PA is a 1064 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. At the nominal 0.2 kHz repetition rate, pulses lasting approximately 10 ns arrive about 5 ms apart.View product →
Laser modelsHPL-1064B-PB1064 nm Pulsed LasersThe HPL-1064B-PB is a 1064 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. At the nominal 0.5 kHz repetition rate, pulses lasting approximately 10 ns arrive about 2 ms apart.View product →
Laser modelsHPL-1319-CW1319 nm CW LasersThe HPL-1319-CW 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. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsHPL-1319-Q1319 nm Pulsed LasersThe HPL-1319-Q 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 250 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsHPL-1319-QM1319 nm Pulsed LasersThe HPL-1319-QM 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 250 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsHPL-240-T240 nm Pulsed LasersThe HPL-240-T is a 240 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 modelsHPL-244-T244 nm Pulsed LasersThe HPL-244-T is a 244 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 modelsHPL-248-T248 nm Pulsed LasersThe HPL-248-T is a 248 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 modelsHPL-330-P330 nm Pulsed LasersThe HPL-330-P is a 330 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 80 ns arrive about 1 ms apart.View product →
Laser modelsHPL-360-T360 nm Pulsed LasersThe HPL-360-T is a 360 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 shorter than 25 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsHPL-375-T375 nm Pulsed LasersThe HPL-375-T is a 375 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 modelsHPL-405-T405 nm Pulsed LasersThe HPL-405-T is a 405 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 shorter than 15 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsHPL-440-Q440 nm Pulsed LasersThe HPL-440-Q is a 440 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 5 kHz repetition rate, pulses lasting approximately 200 ns arrive about 200 µs apart.View product →
Laser modelsHPL-440-QM440 nm Pulsed LasersThe HPL-440-QM is a 440 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 5 kHz repetition rate, pulses lasting approximately 100 ns arrive about 200 µs apart.View product →
Laser modelsHPL-532-PA532 nm Pulsed LasersThe HPL-532-PA is a 532 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–50 mJ. Select energy, timing and cooling for the same configuration. 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 200 Hz repetition rate, pulses lasting approximately 10 ns arrive about 5 ms apart. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
Laser modelsHPL-532-PB532 nm Pulsed LasersThe HPL-532-PB is a 532 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–50 mJ. Select energy, timing and cooling for the same configuration. 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 500 Hz repetition rate, pulses lasting approximately 10 ns arrive about 2 ms apart. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
Laser modelsHPL-532-Q532 nm Pulsed LasersThe HPL-532-Q 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 100 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsHPL-532-QL532 nm Pulsed LasersThe HPL-532-QL 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. At the nominal 15 kHz repetition rate, pulses lasting approximately 100 ns arrive about 66.67 µs apart.View product →
Laser modelsHPL-532-QM532 nm Pulsed LasersThe HPL-532-QM 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 100 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsHPL-556-Q556 nm Pulsed LasersThe HPL-556-Q 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 100 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsHPL-589-Q589 nm Pulsed LasersThe HPL-589-Q is a 589 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 modelsHPL-589.159-Q589.159 nm Pulsed LasersThe HPL-589.159-Q is a 589.159 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 5 kHz repetition rate, successive pulses arrive about 200 µs apart.View product →
Laser modelsHPL-660-Q660 nm Pulsed LasersThe HPL-660-Q is a 660 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 5 kHz repetition rate, pulses lasting approximately 150 ns arrive about 200 µs apart.View product →
Laser modelsHPL-660-QM660 nm Pulsed LasersThe HPL-660-QM is a 660 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 150 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsHPL-720-T720 nm Pulsed LasersThe HPL-720-T is a 720 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 modelsHPL-785-T785 nm Pulsed LasersThe HPL-785-T is a 785 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 shorter than 15 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsHPL-808-T808 nm Pulsed LasersThe HPL-808-T is a 808 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 shorter than 15 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsHPL-MIR-39003900 nm Pulsed LasersThe HPL-MIR-3900 is a 3900 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 10 kHz repetition rate, pulses shorter than 50 ns arrive about 100 µs apart.View product →
Laser modelsHPL-MIR-40004000 nm Pulsed LasersThe HPL-MIR-4000 is a 4000 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 10 kHz repetition rate, pulses shorter than 50 ns arrive about 100 µs apart.View product →
Laser modelsHPL-MIR-41004100 nm Pulsed LasersThe HPL-MIR-4100 is a 4100 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 modelsHPL-MIR-42004200 nm Pulsed LasersThe HPL-MIR-4200 is a 4200 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 10 kHz repetition rate, pulses shorter than 50 ns arrive about 100 µs apart.View product →
Laser modelsHPL-MIR-43004300 nm Pulsed LasersThe HPL-MIR-4300 is a 4300 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 modelsHPL-MIR-44004400 nm Pulsed LasersThe HPL-MIR-4400 is a 4400 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 10 kHz repetition rate, pulses shorter than 50 ns arrive about 100 µs apart.View product →
Laser modelsHPL-MIR-45004500 nm Pulsed LasersThe HPL-MIR-4500 is a 4500 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 modelsHPL-MIR-46004600 nm Pulsed LasersThe HPL-MIR-4600 is a 4600 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 10 kHz repetition rate, pulses shorter than 50 ns arrive about 100 µs apart.View product →
Laser modelsHPL-MIR-48004800 nm Pulsed LasersThe HPL-MIR-4800 is a 4800 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 10 kHz repetition rate, pulses shorter than 50 ns arrive about 100 µs apart.View product →
Laser modelsIII-505L505 nm CW LasersThe III-505L is a 505 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 modelsIII-510510 nm CW LasersThe III-510 is a 510 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 modelsInfrared L aser Display CardMeasurement & SafetyInfared laser display card is used to display UV/ infrared laser spot, able to convert invisible UV/ infrared light to a visible light image...View product →
Laser modelsIntegrated OEM Laser Power MeterMeasurement & SafetySuitable for integration into laser processing equipment or laser test systems to achieve monitoring and feedback of laser power....View product →
Laser modelsLaser Application Series ExperimentComponents & AccessoriesLaser ranging experiment; Laser display system; Infrared active laser night vision comprehensive experiment; Laser processing experiment; Laser eavesdropping; Laser communication …View product →
Laser modelsLaser Crystal Absorption Coefficient Measurement System NEWMeasurement & SafetyThe laser power before and after passing through the sample is monitored in real time by using the difference principle of dual-optical paths.View product →
Laser modelsLaser for Medical Treatment532, 561, 589, 1064 nm Application SystemsThe Laser for Medical Treatment is a 532, 561, 589, 1064 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 modelsLaser for Raman Spectroscopy637 nm Spectrum Analysis637 nm | output 1-200 mW | Series: Laser for Raman SpectroscopyView product →
Laser modelsLaser Goggles1100 nm Measurement & Safety1100 nm | Laser goggles with beautiful shape, comfortable fit, high definition, extrusion deformation prevention material, are able to protect human eyes from the laser radiation damage from 200-1100nm.View product →
Laser modelsLaser Induced Breakdown Spectroscpoy SystemSpectrum AnalysisWith the features of rapid and simple detection process, it is widely used in alloy, coal, waste water, waste gas and various fields which is relevant with elements detection.View product →
Laser modelsLaser Optogenetics & NeuroscienceApplication SystemsThe Laser Optogenetics & Neuroscience 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 modelsLaser Power&Stability MeasurementMeasurement & SafetyLaser power meter is used to measure laser power and power stability. Catalog configurations include customers thermoelectric and photoelectric power meters...View product →
Laser modelsLaser Principle Series ExperimentComponents & AccessoriesSpontaneous emission and stimulated emission; Absorption spView product →
Laser modelsLaser Pulse MeasurementMeasurement & SafetyPhotoelectric detector combined with oscilloscope can monitor ultra-fast pulsed laser and measure pulse duration, frequency, period and other parameters of lasers...View product →
Laser modelsLaser RangingApplication SystemsThe Laser Ranging 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 modelsLaser Source1064 nm Spectrum Analysis1064 nm | A variety of linewidth options at: 257, 360, 405, 473, 514.5, 532, 633, 660, 785, 830, 980, 1064 nm...View product →
Laser modelsLaser SourcesSpectrum AnalysisCatalog configurations include narrow spectral bandwidth, high spectral purity and high wavelength stability, which guarantees the stability and accuracy of the testing results.View product →
Laser modelsLaser Spectrum Series ExperimentComponents & AccessoriesLaser induced breakdown spectroscopy (LIBS); Raman spectrum measurement; Confocal microscopic fluorescence experiment; Cavity ring down spectroscopy technology; Measurement of liquid flow rate by laser Doppler …View product →
Laser modelsLaser Technology ExperimentComponents & AccessoriesLaser transverse/ longitudinal mode observation and selection technique; Acousto-optic/ Electro-optics Q-switched experiment; Laser modulation experiment; Laser amplification technology; Experiment of laser actively/ passively mode-locked …View product →
Laser modelsLaser Wavelength MeasurementMeasurement & SafetyFiber optic spectrometer is used to measure wavelength, line width of laser and common light source, also to measure fluorescence, Raman, plasma spectrum...View product →
Laser modelsLDM-1064-10-21064 nm CW LasersThe LDM-1064-10-2 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. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-1064-100-21064 nm CW LasersThe LDM-1064-100-2 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. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-1064-30-21064 nm CW LasersThe LDM-1064-30-2 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. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-1064-976-808-21064 nm CW LasersThe LDM-1064-976-808-2 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. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-1064-980-915-808-640-450-41064 nm CW LasersThe LDM-1064-980-915-808-640-450-4 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. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-1470-10-21470 nm CW LasersThe LDM-1470-10-2 is a 1470 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 modelsLDM-1470-15-21470 nm CW LasersThe LDM-1470-15-2 is a 1470 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 modelsLDM-1470-30-21470 nm CW LasersThe LDM-1470-30-2 is a 1470 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 modelsLDM-1470-5-21470 nm CW LasersThe LDM-1470-5-2 is a 1470 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 modelsLDM-1470-50-21470 nm CW LasersThe LDM-1470-50-2 is a 1470 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 modelsLDM-1470-980-21470 nm CW LasersThe LDM-1470-980-2 is a 1470 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 modelsLDM-1470-980-635-21470 nm CW LasersThe LDM-1470-980-635-2 is a 1470 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 modelsLDM-1470-980-640-21470 nm CW LasersThe LDM-1470-980-640-2 is a 1470 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 modelsLDM-1550-10-21550 nm CW LasersThe LDM-1550-10-2 is a 1550 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 modelsLDM-1550-15-21550 nm CW LasersThe LDM-1550-15-2 is a 1550 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 modelsLDM-1940-15-21940 nm CW LasersThe LDM-1940-15-2 is a 1940 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 modelsLDM-405-10-2405 nm CW LasersThe LDM-405-10-2 is a 405 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-405-100-6405 nm CW LasersThe LDM-405-100-6 is a 405 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-405-150-8405 nm CW LasersThe LDM-405-150-8 is a 405 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-405-16-2405 nm CW LasersThe LDM-405-16-2 is a 405 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-405-20-4405 nm CW LasersThe LDM-405-20-4 is a 405 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-405-24-4405 nm CW LasersThe LDM-405-24-4 is a 405 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-405-30-4405 nm CW LasersThe LDM-405-30-4 is a 405 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-405-50-6405 nm CW LasersThe LDM-405-50-6 is a 405 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-405-60-6405 nm CW LasersThe LDM-405-60-6 is a 405 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-405-8-2405 nm CW LasersThe LDM-405-8-2 is a 405 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-450-10-1450 nm CW LasersThe LDM-450-10-1 is a 450 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 modelsLDM-450-100-1450 nm CW LasersThe LDM-450-100-1 is a 450 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 modelsLDM-450-15-1450 nm CW LasersThe LDM-450-15-1 is a 450 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 modelsLDM-450-200-2450 nm CW LasersThe LDM-450-200-2 is a 450 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 modelsLDM-450-3-1450 nm CW LasersThe LDM-450-3-1 is a 450 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 modelsLDM-450-30-1450 nm CW LasersThe LDM-450-30-1 is a 450 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 modelsLDM-450-40-1450 nm CW LasersThe LDM-450-40-1 is a 450 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 modelsLDM-450-50-0.5450 nm CW LasersThe LDM-450-50-0.5 is a 450 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 modelsLDM-520-10-1520 nm CW LasersThe LDM-520-10-1 is a 520 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-520-20-2520 nm CW LasersThe LDM-520-20-2 is a 520 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-520-4-1520 nm CW LasersThe LDM-520-4-1 is a 520 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-520-40-2520 nm CW LasersThe LDM-520-40-2 is a 520 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-520-7-1520 nm CW LasersThe LDM-520-7-1 is a 520 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-520-70-4520 nm CW LasersThe LDM-520-70-4 is a 520 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-638-10-2638 nm CW LasersThe LDM-638-10-2 is a 638 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 modelsLDM-638-2.5-1638 nm CW LasersThe LDM-638-2.5-1 is a 638 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 modelsLDM-638-20-2638 nm CW LasersThe LDM-638-20-2 is a 638 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 modelsLDM-638-30-4638 nm CW LasersThe LDM-638-30-4 is a 638 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 modelsLDM-638-40-4638 nm CW LasersThe LDM-638-40-4 is a 638 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 modelsLDM-638-5-1638 nm CW LasersThe LDM-638-5-1 is a 638 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 modelsLDM-638-7-1638 nm CW LasersThe LDM-638-7-1 is a 638 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 modelsLDM-660-10-2660 nm CW LasersThe LDM-660-10-2 is a 660 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 modelsLDM-660-15-2660 nm CW LasersThe LDM-660-15-2 is a 660 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 modelsLDM-660-3-2660 nm CW LasersThe LDM-660-3-2 is a 660 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 modelsLDM-660-6-2660 nm CW LasersThe LDM-660-6-2 is a 660 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 modelsLDM-660-8-2660 nm CW LasersThe LDM-660-8-2 is a 660 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 modelsLDM-793-10-1793 nm CW LasersThe LDM-793-10-1 is a 793 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 modelsLDM-793-20-1793 nm CW LasersThe LDM-793-20-1 is a 793 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-793-30-1793 nm CW LasersThe LDM-793-30-1 is a 793 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-793-5-1793 nm CW LasersThe LDM-793-5-1 is a 793 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 modelsLDM-793-50-1793 nm CW LasersThe LDM-793-50-1 is a 793 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-793-90-1793 nm CW LasersThe LDM-793-90-1 is a 793 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-808-100-4808 nm CW LasersThe LDM-808-100-4 is a 808 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-808-14-4808 nm CW LasersThe LDM-808-14-4 is a 808 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. The specified fiber connection delivers the generated light to the experiment; its core size, numerical aperture and connector need to match the receiving optics.View product →
Laser modelsLDM-808-20-4808 nm CW LasersThe LDM-808-20-4 is a 808 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. The specified fiber connection delivers the generated light to the experiment; its core size, numerical aperture and connector need to match the receiving optics.View product →
Laser modelsLDM-808-200-4808 nm CW LasersThe LDM-808-200-4 is a 808 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsLDM-808-30-4808 nm CW LasersThe LDM-808-30-4 is a 808 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. The specified fiber connection delivers the generated light to the experiment; its core size, numerical aperture and connector need to match the receiving optics.View product →

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