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Lasers model catalog
Browse 3,778 canonical product destinations across 12 product families. Page 3 lists models 241–360.
- Laser modelsAO-Mini-946946 nm Pulsed LasersThe AO-Mini-946 is a 946 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 modelsAO-Mini-E-10641064 nm Pulsed LasersThe AO-Mini-E-1064 is a 1064 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. 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 20 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-Mini-E-13191319 nm Pulsed LasersThe AO-Mini-E-1319 is a 1319 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 modelsAO-Mini-E-266266 nm Pulsed LasersThe AO-Mini-E-266 is a 266 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. 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 8 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-Mini-E-355355 nm Pulsed LasersThe AO-Mini-E-355 is a 355 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. 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 9 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-Mini-E-532532 nm Pulsed LasersThe AO-Mini-E-532 is a 532 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. Pulses lasting approximately 7 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-RM-280280 nm Pulsed LasersThe AO-RM-280 is a 280 nm nanosecond 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. At the nominal 5 kHz repetition rate, pulses shorter than 25 ns arrive about 200 µs apart.View product →
- Laser modelsAO-RM-287287 nm Pulsed LasersThe AO-RM-287 is a 287 nm nanosecond 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. At the nominal 5 kHz repetition rate, pulses shorter than 25 ns arrive about 200 µs apart.View product →
- Laser modelsAO-RM-295295 nm Pulsed LasersThe AO-RM-295 is a 295 nm nanosecond 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. At the nominal 5 kHz repetition rate, pulses shorter than 25 ns arrive about 200 µs apart.View product →
- Laser modelsAO-RM-560560 nm Pulsed LasersThe AO-RM-560 is a 560 nm nanosecond 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. At the nominal 5 kHz repetition rate, pulses shorter than 25 ns arrive about 200 µs apart.View product →
- Laser modelsAO-RM-590590 nm Pulsed LasersThe AO-RM-590 is a 590 nm nanosecond 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. At the nominal 5 kHz repetition rate, pulses shorter than 25 ns arrive about 200 µs apart.View product →
- Laser modelsAO-S-10471047 nm Pulsed LasersThe AO-S-1047 is a 1047 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy.View product →
- Laser modelsAO-S-10531053 nm Pulsed LasersThe AO-S-1053 is a 1053 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy.View product →
- Laser modelsAO-S-10641064 nm Pulsed LasersThe AO-S-1064 is a 1064 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample.View product →
- Laser modelsAO-S-13421342 nm Pulsed LasersThe AO-S-1342 is a 1342 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 27 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-S-261-H261 nm Pulsed LasersThe AO-S-261-H is a 261 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. Pulses lasting approximately 9 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-S-261-H/1-15uJ261 nm Pulsed LasersThe AO-S-261-H/1-15uJ is a 261 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 modelsAO-S-263-H/1-15uJ263 nm Pulsed LasersThe AO-S-263-H/1-15uJ is a 263 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 modelsAO-S-266266 nm Pulsed LasersThe AO-S-266 is a 266 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. Pulses lasting approximately 4 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-S-266-H266 nm Pulsed LasersThe AO-S-266-H is a 266 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. Pulses lasting approximately 9 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-S-349349 nm Pulsed LasersThe AO-S-349 is a 349 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample.View product →
- Laser modelsAO-S-349-FL349 nm Pulsed LasersThe AO-S-349-FL is a 349 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. Pulses lasting approximately 5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-S-351351 nm Pulsed LasersThe AO-S-351 is a 351 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy.View product →
- Laser modelsAO-S-355355 nm Pulsed LasersThe AO-S-355 is a 355 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample.View product →
- Laser modelsAO-S-523.5523.5 nm Pulsed LasersThe AO-S-523.5 is a 523.5 nm pulsed diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy.View product →
- Laser modelsAO-S-523.5-H523.5 nm Pulsed LasersThe AO-S-523.5-H is a 523.5 nm pulsed diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy.View product →
- Laser modelsAO-S-526.5526.5 nm Pulsed LasersThe AO-S-526.5 is a 526.5 nm pulsed diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. 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 modelsAO-S-526.5-H526.5 nm Pulsed LasersThe AO-S-526.5-H is a 526.5 nm pulsed diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. 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 modelsAO-S-532532 nm Pulsed LasersThe AO-S-532 is a 532 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample.View product →
- Laser modelsAO-S-532-H532 nm Pulsed LasersThe AO-S-532-H is a 532 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. Pulses lasting approximately 4.8 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-S-671-H671 nm Pulsed LasersThe AO-S-671-H is a 671 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 23 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-S-946946 nm Pulsed LasersThe AO-S-946 is a 946 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. Pulses lasting approximately 22 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-T-10641064 nm Pulsed LasersThe AO-T-1064 is a 1064 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. 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 35 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-T-532532 nm Pulsed LasersThe AO-T-532 is a 532 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. 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 modelsAO-T-532A532 nm Pulsed LasersThe AO-T-532A is a 532 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. 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 23 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-Ti-360360 nm Pulsed LasersThe AO-Ti-360 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. At the nominal 30 kHz repetition rate, pulses lasting approximately 25 ns arrive about 33.33 µs apart. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
- Laser modelsAO-Ti-720720 nm Pulsed LasersThe AO-Ti-720 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 modelsAO-U-1064-HE1064 nm Pulsed LasersThe AO-U-1064-HE is a 1064 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. Pulses lasting approximately 12 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-U-213-DP213 nm Pulsed LasersThe AO-U-213-DP is a 213 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 12 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-U-262/1-80uJ262 nm Pulsed LasersThe AO-U-262/1-80uJ is a 262 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 modelsAO-U-263/1-60uJ263 nm Pulsed LasersThe AO-U-263/1-60uJ is a 263 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 modelsAO-U-266266 nm Pulsed LasersThe AO-U-266 is a 266 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. Pulses lasting approximately 15 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-U-303-DP303 nm Pulsed LasersThe AO-U-303-DP is a 303 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. Pulses lasting approximately 18 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-U-320-DP320 nm Pulsed LasersThe AO-U-320-DP is a 320 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. Pulses lasting approximately 13 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-U-524/1mJ524 nm Pulsed LasersThe AO-U-524/1mJ is a 524 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 modelsAO-U-527527 nm Pulsed LasersThe AO-U-527 is a 527 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 20 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-U-532532 nm Pulsed LasersThe AO-U-532 is a 532 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. 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 12 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-U-532-HE532 nm Pulsed LasersThe AO-U-532-HE 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 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 modelsAO-U-532& 266266 nm Pulsed LasersThe AO-U-532& 266 is a 266 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. Pulses lasting approximately 10 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-U-607-DP607 nm Pulsed LasersThe AO-U-607-DP is a 607 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. Pulses lasting approximately 35 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-U-639-DP639 nm Pulsed LasersThe AO-U-639-DP is a 639 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. Pulses lasting approximately 18 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-U-721-DP721 nm Pulsed LasersThe AO-U-721-DP is a 721 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 20 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-UA-10641064 nm Pulsed LasersThe AO-UA-1064 is a 1064 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. Pulses lasting approximately 10 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-UA-532532 nm Pulsed LasersThe AO-UA-532 is a 532 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. Pulses lasting approximately 10 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-V-10471047 nm Pulsed LasersThe AO-V-1047 is a 1047 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. Pulses lasting approximately 10 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
- Laser modelsAO-V-10641064 nm Application SystemsThe AO-V-1064 is a 1064 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. 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 20 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-V-1064A1064 nm Pulsed LasersThe AO-V-1064A is a 1064 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. 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 12 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-V-349349 nm Pulsed LasersThe AO-V-349 is a 349 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. Pulses lasting approximately 10 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
- Laser modelsAO-V-355355 nm Pulsed LasersThe AO-V-355 is a 355 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. 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 12 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-V-355-Water355 nm Application SystemsThe AO-V-355-Water is a 355 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 modelsAO-V-473473 nm Pulsed LasersThe AO-V-473 is a 473 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. 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 80 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-V-473/50uJ473 nm Pulsed LasersThe AO-V-473/50uJ is a 473 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 modelsAO-V-532532 nm Pulsed LasersThe AO-V-532 is a 532 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. Pulses lasting approximately 12 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-V-671671 nm Pulsed LasersThe AO-V-671 is a 671 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 modelsAO-X-10641064 nm Pulsed LasersThe AO-X-1064 is a 1064 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. 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 20 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-X-532532 nm Pulsed LasersThe AO-X-532 is a 532 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. Pulses lasting approximately 15 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-XF-640640 nm Pulsed LasersThe AO-XF-640 is a 640 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 30 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsBeam Diameter/Divergence TestingMeasurement & SafetyUsing laser profilometer to measure the energy distribution, beam diameter, divergence, ellipticity and other characteristics of the laser transverse mode...View product →
- Laser modelsBlue Laser for Raman Spectroscopy488 nm Spectrum Analysis488 nm | output 1-70 mW | Series: Blue Laser for Raman Spectroscopy; Features: Fiber coupled, Linewidth <0.06 nmView product →
- Laser modelsCoherence Length MeasurementMeasurement & SafetyUsing Michelson interferometer to split the laser beam in two. When the two light beams recombine, they interfere and form interference fringes in the focal plane...View product →
- Laser modelsCombined Raman Spectrum SystemSpectrum AnalysisFast connection, flexible operation. Wavelength is optional according to customer's actual requirements.View product →
- Laser modelsCombined Raman Spectrum SystemSpectrum AnalysisFast connection, flexible operation. Wavelength is optional according to customer's actual requirements.View product →
- Laser modelsCommunication and ImagingApplication SystemsThe Communication and Imaging 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 modelsComprehensive Experiment of Optics, Mechanics, Electrics and ComputerComponents & AccessoriesMachine vision recognition rejected comprehensive experiment; Machine vision high precision dimension measurement system; Weld visual tracking experiment; Manipulator grasping system experiment …View product →
- Laser modelsComputational Imaging System : Ghost Imaging NEWMeasurement & SafetyGhost Imaging System is a new imaging technology that uses the second order coherence of light field to recover the spatial information of the object to be measured.View product →
- Laser modelsConfocal Laser Scanning MicroscopyApplication SystemsThe Confocal Laser Scanning Microscopy is a 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 modelsCRDS Detection SystemSpectrum AnalysisLong absorption optical path, unaffected by light intensity fluctuation, easy to quantitative measurement, gas concentration variation precision measurement.View product →
- Laser modelsCustomized for Teaching and Scientific ResearchComponents & AccessoriesCatalog configurations include the quality and technology for a strong backing, according to customers' research and teaching demands, we provide teaching experiments and skills training system with customized service.View product →
- Laser modelsCW-729729 nm CW LasersThe CW-729 is a 729 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 modelsCW-760-840760 nm CW LasersThe CW-760-840 is a 760 nm continuous-wave Ti:sapphire laser. An optical pump excites titanium ions in a sapphire crystal. Their broad gain spectrum allows the resonator to select and tune the output wavelength within the specified range. Tuning changes the selected output wavelength so spectral features can be scanned with the same source. The tuning band specifies which lines can be reached; linewidth describes the width of the selected line.View product →
- Laser modelsCW-760-840775 nm CW LasersThe CW-760-840 is a 775 nm continuous-wave Ti:sapphire laser. An optical pump excites titanium ions in a sapphire crystal. Their broad gain spectrum allows the resonator to select and tune the output wavelength within the specified range. Tuning changes the selected output wavelength so spectral features can be scanned with the same source. The tuning band specifies which lines can be reached; linewidth describes the width of the selected line.View product →
- Laser modelsCW-760-840786 nm CW LasersThe CW-760-840 is a 786 nm continuous-wave Ti:sapphire laser. An optical pump excites titanium ions in a sapphire crystal. Their broad gain spectrum allows the resonator to select and tune the output wavelength within the specified range. Tuning changes the selected output wavelength so spectral features can be scanned with the same source. The tuning band specifies which lines can be reached; linewidth describes the width of the selected line.View product →
- Laser modelsCW-760-840793 nm CW LasersThe CW-760-840 is a 793 nm continuous-wave Ti:sapphire laser. An optical pump excites titanium ions in a sapphire crystal. Their broad gain spectrum allows the resonator to select and tune the output wavelength within the specified range. Tuning changes the selected output wavelength so spectral features can be scanned with the same source. The tuning band specifies which lines can be reached; linewidth describes the width of the selected line.View product →
- Laser modelsCW-760-840825 nm CW LasersThe CW-760-840 is a 825 nm continuous-wave Ti:sapphire laser. An optical pump excites titanium ions in a sapphire crystal. Their broad gain spectrum allows the resonator to select and tune the output wavelength within the specified range. Tuning changes the selected output wavelength so spectral features can be scanned with the same source. The tuning band specifies which lines can be reached; linewidth describes the width of the selected line.View product →
- Laser modelsCW-760-840810 nm CW LasersThe CW-760-840 is a 810 nm continuous-wave Ti:sapphire laser. An optical pump excites titanium ions in a sapphire crystal. Their broad gain spectrum allows the resonator to select and tune the output wavelength within the specified range. Tuning changes the selected output wavelength so spectral features can be scanned with the same source. The tuning band specifies which lines can be reached; linewidth describes the width of the selected line.View product →
- Laser modelsCW-760~840760 nm CW LasersThe CW-760~840 is a 760 nm continuous-wave Ti:sapphire laser. An optical pump excites titanium ions in a sapphire crystal. Their broad gain spectrum allows the resonator to select and tune the output wavelength within the specified range. Tuning changes the selected output wavelength so spectral features can be scanned with the same source. The tuning band specifies which lines can be reached; linewidth describes the width of the selected line.View product →
- Laser modelsCW-760~840775 nm CW LasersThe CW-760~840 is a 775 nm continuous-wave Ti:sapphire laser. An optical pump excites titanium ions in a sapphire crystal. Their broad gain spectrum allows the resonator to select and tune the output wavelength within the specified range. Tuning changes the selected output wavelength so spectral features can be scanned with the same source. The tuning band specifies which lines can be reached; linewidth describes the width of the selected line.View product →
- Laser modelsCW-760~840786 nm CW LasersThe CW-760~840 is a 786 nm continuous-wave Ti:sapphire laser. An optical pump excites titanium ions in a sapphire crystal. Their broad gain spectrum allows the resonator to select and tune the output wavelength within the specified range. Tuning changes the selected output wavelength so spectral features can be scanned with the same source. The tuning band specifies which lines can be reached; linewidth describes the width of the selected line.View product →
- Laser modelsCW-760~840793 nm CW LasersThe CW-760~840 is a 793 nm continuous-wave Ti:sapphire laser. An optical pump excites titanium ions in a sapphire crystal. Their broad gain spectrum allows the resonator to select and tune the output wavelength within the specified range. Tuning changes the selected output wavelength so spectral features can be scanned with the same source. The tuning band specifies which lines can be reached; linewidth describes the width of the selected line.View product →
- Laser modelsCW-760~840825 nm CW LasersThe CW-760~840 is a 825 nm continuous-wave Ti:sapphire laser. An optical pump excites titanium ions in a sapphire crystal. Their broad gain spectrum allows the resonator to select and tune the output wavelength within the specified range. Tuning changes the selected output wavelength so spectral features can be scanned with the same source. The tuning band specifies which lines can be reached; linewidth describes the width of the selected line.View product →
- Laser modelsCW-760~840810 nm CW LasersThe CW-760~840 is a 810 nm continuous-wave Ti:sapphire laser. An optical pump excites titanium ions in a sapphire crystal. Their broad gain spectrum allows the resonator to select and tune the output wavelength within the specified range. Tuning changes the selected output wavelength so spectral features can be scanned with the same source. The tuning band specifies which lines can be reached; linewidth describes the width of the selected line.View product →
- Laser modelsCW-810810 nm CW LasersThe CW-810 is a 810 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 modelsD-Light deuterium light sour ce185, 700 nm Spectrum Analysis185, 700 nm | The continuous spectral range is continuously output from 185 nm to 700 nm, the D-Light deuterium light source can be used as a reference light source for absorbance, transmittance and reflectance measurements.View product →
- Laser modelsDesktop Raman Spectrum SystemSpectrum AnalysisBuild-in narrow line width laser - power adjustable, high sensitivity spectrometer - used for weak signal detection.View product →
- Laser modelsDesktop Raman Spectrum SystemSpectrum AnalysisBuild-in narrow line width laser - power adjustable, high sensitivity spectrometer - used for weak signal detection.View product →
- Laser modelsDH-Light Deuterium Halogen Source2500 nm Spectrum Analysis2500 nm | Wide wavelength range with 190-2500nm, can be used for high precision analytical measuring instrument.View product →
- Laser modelsDigital PCRApplication SystemsThe Digital PCR 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 modelsDiode laser457 nm CW LasersThe Diode laser 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 modelsDL-HD-640640 nm CW LasersThe DL-HD-640 is a 640 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 modelsDL-HD-642642 nm CW LasersThe DL-HD-642 is a 642 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
- Laser modelsDL-MD-640640 nm CW LasersThe DL-MD-640 is a 640 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 modelsDL-MD-642642 nm CW LasersThe DL-MD-642 is a 642 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
- Laser modelsDPS-1064-A1064 nm Pulsed LasersThe DPS-1064-A is a 1064 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–10 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. 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 modelsDPS-1064-B1064 nm Pulsed LasersThe DPS-1064-B is a 1064 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 10–30 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. 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 modelsDPS-1064-BS-D1064 nm Pulsed LasersThe DPS-1064-BS-D is a 1064 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 30–100 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. 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 modelsDPS-1064-D1064 nm Pulsed LasersThe DPS-1064-D is a 1064 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–10 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. 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 modelsDPS-1064-D M²≤1.51064 nm Pulsed LasersThe DPS-1064-D M²≤1.5 is a 1064 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. Pulses 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 modelsDPS-1064-E1064 nm Pulsed LasersThe DPS-1064-E is a 1064 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–8 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. Pulses shorter than 4 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsDPS-1064-E Narrow pulse width1064 nm Pulsed LasersThe DPS-1064-E Narrow pulse width is a 1064 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. Pulses shorter than 4 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsDPS-1064-G1064 nm Pulsed LasersThe DPS-1064-G is a 1064 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 50–300 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 100 Hz repetition rate, pulses shorter than 12 ns arrive about 10 ms apart.View product →
- Laser modelsDPS-1064-H1064 nm Pulsed LasersThe DPS-1064-H is a 1064 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 10–30 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. Pulses shorter than 5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsDPS-1064-H M²<1.51064 nm Pulsed LasersThe DPS-1064-H M²<1.5 is a 1064 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. Pulses shorter than 5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsDPS-1064-LR1064 nm Pulsed LasersThe DPS-1064-LR is a 1064 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. At the nominal 20 Hz repetition rate, pulses shorter than 10 ns arrive about 50 ms apart.View product →
- Laser modelsDPS-1064-Neoma1064 nm Pulsed LasersThe DPS-1064-Neoma is a 1064 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. Pulses shorter than 13 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsDPS-1064-P-Mini1064 nm Pulsed LasersThe DPS-1064-P-Mini is a 1064 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 6 mJ (Mini-I); 5 mJ (Mini-II). 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.View product →
- Laser modelsDPS-1064-P-Subnano1064 nm Pulsed LasersThe DPS-1064-P-Subnano is a 1064 nm picosecond diode-pumped solid-state laser. The specified pulse energy is 1–30 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. 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 modelsDPS-1064-Pico1064 nm Pulsed LasersThe DPS-1064-Pico is a 1064 nm picosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy.View product →
- Laser modelsDPS-1064-PIV1064 nm Pulsed LasersThe DPS-1064-PIV is a 1064 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 100 mJ per pulse. 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. 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 modelsDPS-1064-PS1064 nm Pulsed LasersThe DPS-1064-PS is a 1064 nm picosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. 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 modelsDPS-1064-Q1064 nm Pulsed LasersThe DPS-1064-Q is a 1064 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–40 mJ at 1–100 Hz; 1–10 mJ at 1–1000 Hz. 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.View product →