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Lasers model catalog

Browse 3,778 canonical product destinations across 12 product families. Page 4 lists models 361–480.

Laser modelsDPS-1064-Q High rep.rate1064 nm Pulsed LasersThe DPS-1064-Q High rep.rate is a 1064 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 modelsDPS-1535-P1535 nm Pulsed LasersThe DPS-1535-P is a 1535 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy.View product →
Laser modelsDPS-1573-A1573 nm Pulsed LasersThe DPS-1573-A is a 1573 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–5 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-1573-Q1573 nm Pulsed LasersThe DPS-1573-Q is a 1573 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 5–25 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 8 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsDPS-213-Pico213 nm Pulsed LasersThe DPS-213-Pico is a 213 nm picosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. At the nominal 5 MHz repetition rate, pulses shorter than 50 ps arrive about 200 ns apart.View product →
Laser modelsDPS-266-Neoma266 nm Pulsed LasersThe DPS-266-Neoma is a 266 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–3 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 12 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsDPS-266-Pico266 nm Pulsed LasersThe DPS-266-Pico is a 266 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. At the nominal 5 MHz repetition rate, successive pulses arrive about 200 ns apart.View product →
Laser modelsDPS-266-Q266 nm Pulsed LasersThe DPS-266-Q is a 266 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–5 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-280-R280 nm Pulsed LasersThe DPS-280-R is a 280 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–500 μJ. 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-295-R295 nm Pulsed LasersThe DPS-295-R is a 295 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-355-E355 nm Pulsed LasersThe DPS-355-E is a 355 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–2 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-355-Neoma355 nm Pulsed LasersThe DPS-355-Neoma is a 355 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–4 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 12 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsDPS-355-Pico355 nm Pulsed LasersThe DPS-355-Pico is a 355 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. At the nominal 5 MHz repetition rate, pulses shorter than 50 ps arrive about 200 ns apart.View product →
Laser modelsDPS-355-Q355 nm Pulsed LasersThe DPS-355-Q is a 355 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-527-PIV527 nm Pulsed LasersThe DPS-527-PIV is a 527 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–20 mJ at 1 kHz. 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-527-Q527 nm Pulsed LasersThe DPS-527-Q is a 527 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–20 mJ at 1 kHz. 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-532-A532 nm Pulsed LasersThe DPS-532-A is a 532 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–5 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-532-B532 nm Pulsed LasersThe DPS-532-B is a 532 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 5–15 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-532-BS-D532 nm Pulsed LasersThe DPS-532-BS-D is a 532 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 15–50 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 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-532-E532 nm Pulsed LasersThe DPS-532-E is a 532 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–4 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-532-E Narrow pulse width532 nm Pulsed LasersThe DPS-532-E Narrow pulse width 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 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-532-G532 nm Pulsed LasersThe DPS-532-G is a 532 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 30–150 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 10 ns arrive about 10 ms apart.View product →
Laser modelsDPS-532-H532 nm Pulsed LasersThe DPS-532-H is a 532 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 5–10 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 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-532-H M²<1.5532 nm Pulsed LasersThe DPS-532-H M²<1.5 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 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-532-Neoma532 nm Pulsed LasersThe DPS-532-Neoma is a 532 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–25 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 12 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsDPS-532-P-Subnano532 nm Pulsed LasersThe DPS-532-P-Subnano is a 532 nm picosecond diode-pumped solid-state laser. The specified pulse energy is 1–15 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-532-Pico532 nm Pulsed LasersThe DPS-532-Pico is a 532 nm picosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. Pulses shorter than 50 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsDPS-532-Q532 nm Pulsed LasersThe DPS-532-Q is a 532 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–20 mJ at 1–100 Hz; 1–5 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 →
Laser modelsDPS-532-Q High rep.rate532 nm Pulsed LasersThe DPS-532-Q High rep.rate 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 modelsDPS-560-R560 nm Pulsed LasersThe DPS-560-R is a 560 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-589-R589 nm Pulsed LasersThe DPS-589-R is a 589 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. 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 modelsDPSS Laser488 nm Pulsed LasersThe DPSS Laser is a 488 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 modelsEL-10641064 nm Application SystemsThe EL-1064 is a 1064 nm laser source. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsEngineering and Physical Optics ExperimentComponents & AccessoriesFraunhofer diffraction experiment; Interference principle and application experiment; Michelson interferometer experiment; Polarized light analysis experimentView product →
Laser modelsEO-1047-N1047 nm Pulsed LasersThe EO-1047-N is a 1047 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–1000 μJ at 100 Hz; 1–200 μJ at 1 kHz. 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 modelsEO-1053-N1053 nm Pulsed LasersThe EO-1053-N is a 1053 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–1000 μJ at 100 Hz; 1–200 μJ at 1 kHz. 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 modelsEO-1064-D1064 nm Pulsed LasersThe EO-1064-D is a 1064 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–4 mJ at 5 kHz. 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 modelsEO-1064-G1064 nm Pulsed LasersThe EO-1064-G is a 1064 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 10 μJ–2.5 mJ, depending on rate and variant. 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 modelsEO-1064-G M²<1 .2, Air cooled1064 nm Pulsed LasersThe EO-1064-G M²<1.2, Air cooled 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 8 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-1064-H1064 nm Pulsed LasersThe EO-1064-H is a 1064 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 0.75 mJ at 5 kHz; 0.75–1.5 mJ at 3 kHz. 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 modelsEO-1064-H M²<1.51064 nm Pulsed LasersThe EO-1064-H M²<1.5 is a 1064 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 modelsEO-1064-N1064 nm Pulsed LasersThe EO-1064-N is a 1064 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 0.3–1.5 mJ, depending on rate and variant. 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 modelsEO-1064-P1064 nm Pulsed LasersThe EO-1064-P 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 5 kHz repetition rate, pulses lasting approximately 2.6 ns arrive about 200 µs apart.View product →
Laser modelsEO-1064-P-Subnano1064 nm Pulsed LasersThe EO-1064-P-Subnano is a 1064 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–1000 μJ at 2 kHz; 1–200 μJ at 50 kHz. 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 1 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-1064-PS1064 nm Pulsed LasersThe EO-1064-PS is a 1064 nm picosecond diode-pumped solid-state laser. The specified pulse energy is 1–150 μJ at 200 kHz. 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. 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. Pulses shorter than 15 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-1064-Subnano1064 nm Pulsed LasersThe EO-1064-Subnano is a 1064 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–1000 μJ at 1 kHz; 1–700 μJ at 10 kHz. 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 modelsEO-1064-Subnano-Hi1064 nm Pulsed LasersThe EO-1064-Subnano-Hi is a 1064 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–4 mJ at 5 kHz. 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. The specified fiber connection delivers the generated light to the experiment; its core size, numerical aperture and connector need to match the receiving optics.View product →
Laser modelsEO-1573-Q1573 nm Pulsed LasersThe EO-1573-Q is a 1573 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. At the nominal 1 kHz repetition rate, successive pulses arrive about 1 ms apart.View product →
Laser modelsEO-213-Subnano213 nm Pulsed LasersThe EO-213-Subnano 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 shorter than 2 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-213-Subnano-Hi213 nm Pulsed LasersThe EO-213-Subnano-Hi is a 213 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–100 μJ at 5 kHz. 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 modelsEO-266-G266 nm Pulsed LasersThe EO-266-G 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 shorter than 9 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-266-N266 nm Pulsed LasersThe EO-266-N 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 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 modelsEO-266-P-Subnano266 nm Pulsed LasersThe EO-266-P-Subnano is a 266 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–110 μJ at 2 kHz. 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 1 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-266-Subnano266 nm Pulsed LasersThe EO-266-Subnano is a 266 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–100 μJ at 1 kHz. 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 modelsEO-266-Subnano-Hi266 nm Pulsed LasersThe EO-266-Subnano-Hi is a 266 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–500 μJ at 5 kHz. 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 modelsEO-266W266 nm Pulsed LasersThe EO-266W 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 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 modelsEO-335335 nm Pulsed LasersThe EO-335 is a 335 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. At the nominal 10 kHz repetition rate, pulses shorter than 5 ns arrive about 100 µs apart.View product →
Laser modelsEO-355-G355 nm Pulsed LasersThe EO-355-G 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 shorter than 6 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-355-N355 nm Pulsed LasersThe EO-355-N 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 shorter than 6 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-355-P-Subnano355 nm Pulsed LasersThe EO-355-P-Subnano is a 355 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–130 μJ at 2 kHz. 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 1 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-355-PS355 nm Pulsed LasersThe EO-355-PS is a 355 nm picosecond diode-pumped solid-state laser. The specified pulse energy is 1–40 μJ at 200 kHz. 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. 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. Pulses shorter than 15 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-355-Subnano355 nm Pulsed LasersThe EO-355-Subnano is a 355 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–100 μJ at 1 kHz; 1–20 μJ at 5 kHz. 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 modelsEO-355-Subnano-Hi355 nm Pulsed LasersThe EO-355-Subnano-Hi is a 355 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–600 μJ at 5 kHz. 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 modelsEO-532-D532 nm Pulsed LasersThe EO-532-D is a 532 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–2 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.View product →
Laser modelsEO-532-G532 nm Pulsed LasersThe EO-532-G is a 532 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 10–1500 μJ, depending on rate and variant. 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 modelsEO-532-G M²<1.2532 nm Pulsed LasersThe EO-532-G M²<1.2 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 8 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-532-H532 nm Pulsed LasersThe EO-532-H is a 532 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 0.4 mJ at 5 kHz; 0.4–0.8 mJ at 3 kHz. 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 modelsEO-532-H M²<1.5532 nm Pulsed LasersThe EO-532-H M²<1.5 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 6 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-532-N532 nm Pulsed LasersThe EO-532-N is a 532 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 0.1–0.8 mJ, depending on rate and variant. 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 modelsEO-532-P-Subnano532 nm Pulsed LasersThe EO-532-P-Subnano is a 532 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–500 μJ at 2 kHz; 1–100 μJ at 50 kHz. 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 1 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-532-PS532 nm Pulsed LasersThe EO-532-PS is a 532 nm picosecond diode-pumped solid-state laser. The specified pulse energy is 1–60 μJ at 200 kHz. 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. 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. Pulses shorter than 15 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-532-Subnano532 nm Pulsed LasersThe EO-532-Subnano is a 532 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 1–500 μJ at 1 kHz; 1–300 μJ at 10 kHz. 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 modelsEO-532-Subnano-Hi532 nm Pulsed LasersThe EO-532-Subnano-Hi is a 532 nm nanosecond diode-pumped solid-state laser. The specified pulse energy is 10 μJ–2 mJ at 5 kHz. 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. The specified fiber connection delivers the generated light to the experiment; its core size, numerical aperture and connector need to match the receiving optics.View product →
Laser modelsEO-HS-10641064 nm Pulsed LasersThe EO-HS-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 5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-HS-532532 nm Pulsed LasersThe EO-HS-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 4 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-LS-10301030 nm Pulsed LasersThe EO-LS-1030 is a 1030 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. At the nominal 1 kHz repetition rate, pulses shorter than 20 ns arrive about 1 ms apart. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
Laser modelsEO-LS-10641064 nm Pulsed LasersThe EO-LS-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 shorter than 7 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 modelsEO-LS-515515 nm Pulsed LasersThe EO-LS-515 is a 515 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. At the nominal 1 kHz repetition rate, pulses shorter than 20 ns arrive about 1 ms apart. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
Laser modelsEO-LS-532532 nm Pulsed LasersThe EO-LS-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 shorter than 6 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 modelsEO-RS-10641064 nm Pulsed LasersThe EO-RS-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 5 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 modelsEO-RS-532532 nm Pulsed LasersThe EO-RS-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 4 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 modelsEO-S-10641064 nm Pulsed LasersThe EO-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. 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 modelsEO-S-1064-L1064 nm Pulsed LasersThe EO-S-1064-L is a 1064 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. Pulses lasting approximately 5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-S-1064-RS1064 nm Pulsed LasersThe EO-S-1064-RS 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 modelsEO-S-213-RS213 nm Pulsed LasersThe EO-S-213-RS 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 1.5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-S-266-RS266 nm Pulsed LasersThe EO-S-266-RS is a 266 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. Pulses lasting approximately 1.3 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-S-355-L355 nm Pulsed LasersThe EO-S-355-L is a 355 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. Pulses lasting approximately 5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-S-355-RS355 nm Pulsed LasersThe EO-S-355-RS is a 355 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. Pulses lasting approximately 1.3 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-S-532532 nm Pulsed LasersThe EO-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. Pulses lasting approximately 6 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-S-532-L532 nm Pulsed LasersThe EO-S-532-L 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 5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-S-532-RS532 nm Pulsed LasersThe EO-S-532-RS is a 532 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. Pulses lasting approximately 1.3 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-XS-10641064 nm Pulsed LasersThe EO-XS-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 4 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-XS-13421342 nm Pulsed LasersThe EO-XS-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. At the nominal 10 kHz repetition rate, pulses lasting approximately 4 ns arrive about 100 µs apart.View product →
Laser modelsEO-XS-223223 nm Pulsed LasersThe EO-XS-223 is a 223 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. At the nominal 10 kHz repetition rate, pulses lasting approximately 4 ns arrive about 100 µs apart. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
Laser modelsEO-XS-228228 nm Pulsed LasersThe EO-XS-228 is a 228 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. At the nominal 10 kHz repetition rate, pulses lasting approximately 4 ns arrive about 100 µs apart. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
Laser modelsEO-XS-2600-44102600 nm Pulsed LasersThe EO-XS-2600-4410 is a 2600 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 modelsEO-XS-2600-44102800 nm Pulsed LasersThe EO-XS-2600-4410 is a 2800 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 modelsEO-XS-2600-44103000 nm Pulsed LasersThe EO-XS-2600-4410 is a 3000 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 modelsEO-XS-2600-44103100 nm Pulsed LasersThe EO-XS-2600-4410 is a 3100 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 modelsEO-XS-2600-44103200 nm Pulsed LasersThe EO-XS-2600-4410 is a 3200 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 modelsEO-XS-2600-44103300 nm Pulsed LasersThe EO-XS-2600-4410 is a 3300 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 modelsEO-XS-2600-44103400 nm Pulsed LasersThe EO-XS-2600-4410 is a 3400 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 modelsEO-XS-2600-44103600 nm Pulsed LasersThe EO-XS-2600-4410 is a 3600 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 modelsEO-XS-2600-44103700 nm Pulsed LasersThe EO-XS-2600-4410 is a 3700 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 modelsEO-XS-2600-44104100 nm Pulsed LasersThe EO-XS-2600-4410 is a 4100 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 modelsEO-XS-2600-44103900 nm Pulsed LasersThe EO-XS-2600-4410 is a 3900 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 modelsEO-XS-2600-44104000 nm Pulsed LasersThe EO-XS-2600-4410 is a 4000 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 modelsEO-XS-2600-44104200 nm Pulsed LasersThe EO-XS-2600-4410 is a 4200 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 modelsEO-XS-2600-44104400 nm Pulsed LasersThe EO-XS-2600-4410 is a 4400 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 modelsEO-XS-2600-44103800 nm Pulsed LasersThe EO-XS-2600-4410 is a 3800 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 modelsEO-XS-305305 nm Pulsed LasersThe EO-XS-305 is a 305 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. At the nominal 10 kHz repetition rate, pulses lasting approximately 3 ns arrive about 100 µs apart.View product →
Laser modelsEO-XS-335335 nm Pulsed LasersThe EO-XS-335 is a 335 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. At the nominal 10 kHz repetition rate, pulses lasting approximately 4 ns arrive about 100 µs apart.View product →
Laser modelsEO-XS-355355 nm Pulsed LasersThe EO-XS-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 4 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-XS-40004000 nm Pulsed LasersThe EO-XS-4000 is a 4000 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 modelsEO-XS-447447 nm Pulsed LasersThe EO-XS-447 is a 447 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. At the nominal 10 kHz repetition rate, pulses lasting approximately 4 ns arrive about 100 µs apart.View product →
Laser modelsEO-XS-457457 nm Pulsed LasersThe EO-XS-457 is a 457 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. At the nominal 10 kHz repetition rate, pulses lasting approximately 3 ns arrive about 100 µs apart.View product →
Laser modelsEO-XS-532532 nm Pulsed LasersThe EO-XS-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 4 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsEO-XS-671671 nm Pulsed LasersThe EO-XS-671 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. At the nominal 10 kHz repetition rate, pulses lasting approximately 4 ns arrive about 100 µs apart.View product →
Laser modelsEO-XS-914914 nm Pulsed LasersThe EO-XS-914 is a 914 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. At the nominal 10 kHz repetition rate, pulses lasting approximately 4 ns arrive about 100 µs apart.View product →
Laser modelsF-444-HS444 nm Single-Frequency LasersThe F-444-HS is a 444 nm continuous-wave direct diode laser. Electrical current creates optical gain in a semiconductor junction, and the diode generates the laser light directly. Optical feedback selects the oscillating modes, while drive current and junction temperature affect output power and wavelength. The TTL and analog modulation options control different things: TTL gates the beam on and off, while analog control varies its intensity. Modulation bandwidth sets how quickly the source can follow a changing command.View product →

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