Server-rendered product directory
Lasers model catalog
Browse 3,778 canonical product destinations across 12 product families. Page 11 lists models 1,201–1,320.
- Laser modelsLDM-808-300-2808 nm CW LasersThe LDM-808-300-2 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-808-4.5-1808 nm CW LasersThe LDM-808-4.5-1 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-808-50-4808 nm CW LasersThe LDM-808-50-4 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-808-500-8808 nm CW LasersThe LDM-808-500-8 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-878.6VBG-100-2878 nm CW LasersThe LDM-878.6VBG-100-2 is a 878 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-878.6VBG-120-2878 nm CW LasersThe LDM-878.6VBG-120-2 is a 878 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-878.6VBG-180-4878 nm CW LasersThe LDM-878.6VBG-180-4 is a 878 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-878.6VBG-30-2878 nm CW LasersThe LDM-878.6VBG-30-2 is a 878 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-878.6VBG-40-2878 nm CW LasersThe LDM-878.6VBG-40-2 is a 878 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-878.6VBG-70-2878 nm CW LasersThe LDM-878.6VBG-70-2 is a 878 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-915-100-2915 nm CW LasersThe LDM-915-100-2 is a 915 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-915-150-4915 nm CW LasersThe LDM-915-150-4 is a 915 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-915-200-4915 nm CW LasersThe LDM-915-200-4 is a 915 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-915-30-2915 nm CW LasersThe LDM-915-30-2 is a 915 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-915-300-2915 nm CW LasersThe LDM-915-300-2 is a 915 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-915-50-2915 nm CW LasersThe LDM-915-50-2 is a 915 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-940-100-2940 nm CW LasersThe LDM-940-100-2 is a 940 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
- Laser modelsLDM-940-170-1940 nm CW LasersThe LDM-940-170-1 is a 940 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
- Laser modelsLDM-940-200-2940 nm CW LasersThe LDM-940-200-2 is a 940 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
- Laser modelsLDM-940-80-1940 nm CW LasersThe LDM-940-80-1 is a 940 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-976VBG-100-1976 nm CW LasersThe LDM-976VBG-100-1 is a 976 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-976VBG-140-1976 nm CW LasersThe LDM-976VBG-140-1 is a 976 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-976VBG-30-1976 nm CW LasersThe LDM-976VBG-30-1 is a 976 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-976VBG-60-1976 nm CW LasersThe LDM-976VBG-60-1 is a 976 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-976VBG-9-1976 nm CW LasersThe LDM-976VBG-9-1 is a 976 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-980-100-2980 nm CW LasersThe LDM-980-100-2 is a 980 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-980-200-4980 nm CW LasersThe LDM-980-200-4 is a 980 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-980-30-2980 nm CW LasersThe LDM-980-30-2 is a 980 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-980-300-2980 nm CW LasersThe LDM-980-300-2 is a 980 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-980-50-2980 nm CW LasersThe LDM-980-50-2 is a 980 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 modelsLED light source/ solid-state light sourceSpectrum AnalysisMicroscope LED white light source/solid-state light source, multi-channel LED multi-color light source, high-power fiber-coupled LED light source, providing high-brightness light source, used in a series of medical, biotechnology and industrial applications. The wavelength ranges from the ultraviolet to the near-infrared spectral region. Other wavelengths can be provided as required.View product →
- Laser modelsLGS-589.159-PS589.159 nm Pulsed LasersThe LGS-589.159-PS is a 589.159 nm nanosecond 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. Mode locking fixes the phase relationship between resonator modes so they add together into a regular train of short pulses. Pulse duration and pulse spacing describe different time scales. At the nominal 100 MHz repetition rate, successive pulses arrive about 10 ns apart.View product →
- Laser modelsLIBS: Laser Induced BreakdownApplication SystemsThe LIBS: Laser Induced Breakdown 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 modelsLIF: Laser Induced FluorescenceApplication SystemsThe LIF: Laser Induced Fluorescence 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 modelsLinear Variable Long Wave Pass FilterSpectrum AnalysisThe quartz substrate was coated by ion sputtering to achieve minimum autofluorescence and high laser damage threshold.View product →
- Laser modelsLong Coherence Length637 nm CW LasersThe Long Coherence Length is a 637 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
- Laser modelsLong Coherent Length488 nm CW LasersThe Long Coherent Length is a 488 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 modelsLongitudinal Mode MeasurementMeasurement & SafetyS canning F-P interferometer is used for longitudinal mode measurement. Laser longitudinal mode refers to the axial distribution of the light field along to its direction of propagation...View product →
- Laser modelsLow Noise637 nm CW LasersThe Low Noise is a 637 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
- Laser modelsLow Noise457 nm CW LasersThe Low Noise is a 457 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 modelsLow Noise488 nm CW LasersThe Low Noise is a 488 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 modelsLPS-1064-A1064 nm Pulsed LasersThe LPS-1064-A is a 1064 nm nanosecond lamp-pumped solid-state laser. The specified pulse energy is 50–200 mJ. Select energy, timing and cooling for the same configuration. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 10 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsLPS-1064-L1064 nm Pulsed LasersThe LPS-1064-L is a 1064 nm nanosecond lamp-pumped solid-state laser. The specified pulse energy is 300–1000 mJ. Select energy, timing and cooling for the same configuration. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 modelsLPS-1064-M1064 nm Pulsed LasersThe LPS-1064-M is a 1064 nm pulsed lamp-pumped solid-state laser. The specified pulse energy is 1–10 J at 5 ms. Select energy, timing and cooling for the same configuration. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 modelsLPS-1064-M Long pulse1064 nm Pulsed LasersThe LPS-1064-M Long pulse is a 1064 nm pulsed lamp-pumped solid-state laser. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 modelsLPS-1064-PS1064 nm Pulsed LasersThe LPS-1064-PS is a 1064 nm picosecond lamp-pumped solid-state laser. The specified pulse energy is >100 mJ. Select energy, timing and cooling for the same configuration. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. Pulses shorter than 30 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsLPS-1064-Q1064 nm Pulsed LasersThe LPS-1064-Q is a 1064 nm nanosecond lamp-pumped solid-state laser. The specified pulse energy is 350–850 mJ. Select energy, timing and cooling for the same configuration. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 10 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsLPS-1064-Q Small size1064 nm Pulsed LasersThe LPS-1064-Q Small size is a 1064 nm nanosecond lamp-pumped solid-state laser. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 10 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsLPS-1064-S1064 nm Pulsed LasersThe LPS-1064-S is a 1064 nm nanosecond lamp-pumped solid-state laser. The specified pulse energy is 50–300 mJ. Select energy, timing and cooling for the same configuration. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 modelsLPS-1064-Subnano1064 nm Pulsed LasersThe LPS-1064-Subnano is a 1064 nm picosecond lamp-pumped solid-state laser. The specified pulse energy is 30–200 mJ. Select energy, timing and cooling for the same configuration. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. Pulses shorter than 500 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsLPS-2940-S2940 nm Pulsed LasersThe LPS-2940-S is a 2940 nm pulsed laser source. The specified pulse energy is 50–100 mJ at 4 Hz; 100–200 mJ at 2 Hz. Select energy, timing and cooling for the same configuration. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. Pulses lasting 0.9 ms deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsLPS-355-L355 nm Pulsed LasersThe LPS-355-L is a 355 nm nanosecond lamp-pumped solid-state laser. The specified pulse energy is 80–200 mJ. Select energy, timing and cooling for the same configuration. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 10 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsLPS-355-Q355 nm Pulsed LasersThe LPS-355-Q is a 355 nm nanosecond lamp-pumped solid-state laser. The specified pulse energy is 80–200 mJ. Select energy, timing and cooling for the same configuration. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 10 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsLPS-355-Q Small size355 nm Pulsed LasersThe LPS-355-Q Small size is a 355 nm nanosecond lamp-pumped solid-state laser. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 10 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsLPS-355-S355 nm Pulsed LasersThe LPS-355-S is a 355 nm nanosecond lamp-pumped solid-state laser. The specified pulse energy is 10–80 mJ. Select energy, timing and cooling for the same configuration. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 10 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsLPS-532-A532 nm Pulsed LasersThe LPS-532-A is a 532 nm nanosecond lamp-pumped solid-state laser. The specified pulse energy is 20–100 mJ. Select energy, timing and cooling for the same configuration. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 modelsLPS-532-L532 nm Pulsed LasersThe LPS-532-L is a 532 nm nanosecond lamp-pumped solid-state laser. The specified pulse energy is 150–450 mJ. Select energy, timing and cooling for the same configuration. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 modelsLPS-532-Q532 nm Pulsed LasersThe LPS-532-Q is a 532 nm nanosecond lamp-pumped solid-state laser. The specified pulse energy is 150–500 mJ. Select energy, timing and cooling for the same configuration. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 10 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsLPS-532-Q Small size532 nm Pulsed LasersThe LPS-532-Q Small size is a 532 nm nanosecond lamp-pumped solid-state laser. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 10 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsLPS-532-S532 nm Pulsed LasersThe LPS-532-S is a 532 nm nanosecond lamp-pumped solid-state laser. The specified pulse energy is 30–150 mJ. Select energy, timing and cooling for the same configuration. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 modelsLPS-532-Subnano532 nm Pulsed LasersThe LPS-532-Subnano is a 532 nm picosecond lamp-pumped solid-state laser. The specified pulse energy is 15–100 mJ. Select energy, timing and cooling for the same configuration. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. Pulses shorter than 500 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsLPS-755-M755 nm Pulsed LasersThe LPS-755-M is a 755 nm pulsed lamp-pumped solid-state laser. The specified pulse energy is 1–40 J at 3 ms; 40–60 J at 5 ms. Select energy, timing and cooling for the same configuration. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. At the nominal 1 Hz repetition rate, successive pulses arrive about 1 s apart.View product →
- Laser modelsLPS-L-10641064 nm Pulsed LasersThe LPS-L-1064 is a 1064 nm pulsed lamp-pumped solid-state laser. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 modelsLPS-L-532532 nm Pulsed LasersThe LPS-L-532 is a 532 nm pulsed lamp-pumped solid-state laser. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 modelsLPS-M-10641064 nm Pulsed LasersThe LPS-M-1064 is a 1064 nm pulsed lamp-pumped solid-state laser. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 modelsLPS-T-710-810710–810 nm Pulsed LasersThe LPS-T-710-810 is a 710–810 nm nanosecond lamp-pumped solid-state laser. The specified pulse energy is 1–20 mJ at 765–800 nm; 1–8 mJ at 710–810 nm. Select energy, timing and cooling for the same configuration. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 at most 15 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsLPS-TUN-420-1200420–1200 nm Pulsed LasersThe LPS-TUN-420-1200 is a 420–1200 nm nanosecond lamp-pumped solid-state laser. The specified pulse energy is Up to 20 mJ. Select energy, timing and cooling for the same configuration. A pump lamp supplies optical energy to a solid gain medium, and the resonator amplifies the laser light. Lamp excitation and thermal recovery are important when setting the repetition rate. 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 Hz repetition rate, pulses shorter than 8 ns arrive about 100 ms apart.View product →
- Laser modelsLR-1064-201064 nm Pulsed LasersThe LR-1064-20 is a 1064 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 50 / 80 mJ options. 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 20 Hz repetition rate, pulses shorter than 10 ns arrive about 50 ms apart.View product →
- Laser modelsM² Measurement SystemMeasurement & SafetyBeam quality and focusing capability are key laser parameters, usually characterized by the M² factor. This factor is measured using an M²-Meter...View product →
- Laser modelsMBL-425(FC)425 nm CW LasersThe MBL-425(FC) is a 425 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 modelsMBL-429(FC)429 nm CW LasersThe MBL-429(FC) is a 429 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 modelsMBL-430(FC)430 nm CW LasersThe MBL-430(FC) is a 430 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 modelsMBL-433(FC)433 nm CW LasersThe MBL-433(FC) is a 433 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 modelsMBL-434(FC)434 nm CW LasersThe MBL-434(FC) is a 434 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 modelsMBL-435(FC)435 nm CW LasersThe MBL-435(FC) is a 435 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 modelsMBL-457(FC)457 nm CW LasersThe MBL-457(FC) is a 457 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 modelsMBL-457(Line)457 nm CW LasersThe MBL-457(Line) is a 457 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 modelsMBL-473(FC)473 nm CW LasersThe MBL-473(FC) is a 473 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 modelsMBL-473(Line)473 nm CW LasersThe MBL-473(Line) is a 473 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 modelsMBL-480(FC)480 nm CW LasersThe MBL-480(FC) is a 480 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
- Laser modelsMBL-484(FC)484 nm CW LasersThe MBL-484(FC) is a 484 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 modelsMBL-488(Line)488 nm CW LasersThe MBL-488(Line) is a 488 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 modelsMBL-491(FC)491 nm CW LasersThe MBL-491(FC) is a 491 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 modelsMBL-DF-488488 nm CW LasersThe MBL-DF-488 is a 488 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 modelsMBL-F-457457 nm CW LasersThe MBL-F-457 is a 457 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 modelsMBL-F-473473 nm CW LasersThe MBL-F-473 is a 473 nm continuous-wave diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
- Laser modelsMBL-F-480480 nm CW LasersThe MBL-F-480 is a 480 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 modelsMBL-FN-473473 nm CW LasersThe MBL-FN-473 is a 473 nm continuous-wave diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
- Laser modelsMBL-FN-473-AOM473 nm CW LasersThe MBL-FN-473-AOM is a 473 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. 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 modelsMBL-III-473-AOM473 nm CW LasersThe MBL-III-473-AOM is a 473 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. 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 modelsMBL-K-457457 nm CW LasersThe MBL-K-457 is a 457 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 modelsMBL-K-457-Water457 nm CW LasersThe MBL-K-457-Water is a 457 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 modelsMBL-S-473473 nm CW LasersThe MBL-S-473 is a 473 nm continuous-wave diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
- Laser modelsMBL-S-473-SM473 nm Fiber LasersThe MBL-S-473-SM is a 473 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
- Laser modelsMBL-U-425-SF425 nm Single-Frequency LasersThe MBL-U-425-SF is a 425 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 modelsMBL-U-430-SF429 nm CW LasersThe MBL-U-430-SF is a 429 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 modelsMBL-U-430-SF430 nm CW LasersThe MBL-U-430-SF is a 430 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 modelsMBL-U-432.7-SF432.7 nm CW LasersThe MBL-U-432.7-SF is a 432.7 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 modelsMBL-U-433-SF433 nm CW LasersThe MBL-U-433-SF is a 433 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 modelsMBL-U-457457 nm CW LasersThe MBL-U-457 is a 457 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 modelsMBL-U-473473 nm CW LasersThe MBL-U-473 is a 473 nm continuous-wave diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
- Laser modelsMBL-U-484-SF484 nm CW LasersThe MBL-U-484-SF is a 484 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 modelsMBL-U-488-SF488 nm CW LasersThe MBL-U-488-SF is a 488 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 modelsMBL-U-491-SF491 nm CW LasersThe MBL-U-491-SF is a 491 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 modelsMBL-U-496-SF496 nm CW LasersThe MBL-U-496-SF is a 496 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 modelsMBL-W-473473 nm CW LasersThe MBL-W-473 is a 473 nm continuous-wave diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
- Laser modelsMBL-W-473-SM473 nm Fiber LasersThe MBL-W-473-SM is a 473 nm continuous-wave fiber-coupled laser source. The laser output is coupled into an optical fiber for delivery to the experiment. The fiber core, numerical aperture and connector determine compatibility with the receiving optics. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →
- Laser modelsMBL-XS-457457 nm CW LasersThe MBL-XS-457 is a 457 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
- Laser modelsMDL-1060(FC)1060 nm CW LasersThe MDL-1060(FC) is a 1060 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 modelsMDL-1120(FC)1120 nm CW LasersThe MDL-1120(FC) is a 1120 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 modelsMDL-1130(FC)1130 nm Application SystemsThe MDL-1130(FC) is a 1130 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 modelsMDL-1140(FC)1140 nm Application SystemsThe MDL-1140(FC) is a 1140 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 modelsMDL-1150(FC)1150 nm CW LasersThe MDL-1150(FC) is a 1150 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 modelsMDL-1160(FC)1160 nm Application SystemsThe MDL-1160(FC) is a 1160 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 modelsMDL-1208(FC)1208 nm Application SystemsThe MDL-1208(FC) is a 1208 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 modelsMDL-1270(FC)1270 nm CW LasersThe MDL-1270(FC) is a 1270 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 modelsMDL-1310(FC)1310 nm CW LasersThe MDL-1310(FC) is a 1310 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 modelsMDL-1320(FC)1320 nm Application SystemsThe MDL-1320(FC) is a 1320 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 modelsMDL-1370(FC)1370 nm Application SystemsThe MDL-1370(FC) is a 1370 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 modelsMDL-1380(FC)1380 nm Application SystemsThe MDL-1380(FC) is a 1380 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 →