Server-rendered product directory
Lasers model catalog
Browse 3,778 canonical product destinations across 12 product families. Page 2 lists models 121–240.
- Laser models1064 nm Single-Frequency LasersThe 1064 is a 1064 nm pulsed laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. At the nominal 80 MHz repetition rate, successive pulses arrive about 12.5 ns apart.View product →
- Laser models1080 nm Fiber LasersThe 1080 is a 1080 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 models1100 nm Fiber LasersThe 1100 is a 1100 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 models1112 nm Single-Frequency LasersThe 1112 is a 1112 nm laser source. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
- Laser models1120 nm Fiber LasersThe 1120 is a 1120 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 models1122 nm Single-Frequency LasersThe 1122 is a 1122 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 models1313 nm Single-Frequency LasersThe 1313 is a 1313 nm pulsed laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. At the nominal 80 MHz repetition rate, successive pulses arrive about 12.5 ns apart.View product →
- Laser models1319 nm Pulsed LasersThe 1319 is a 1319 nm nanosecond laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. Pulses lasting approximately 250 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser models1319 nm Single-Frequency LasersThe 1319 is a 1319 nm pulsed laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. At the nominal 80 MHz repetition rate, successive pulses arrive about 12.5 ns apart.View product →
- Laser models1342 nm Single-Frequency LasersThe 1342 is a 1342 nm pulsed laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. At the nominal 80 MHz repetition rate, successive pulses arrive about 12.5 ns apart.View product →
- Laser models1525-1596 nm Fiber LasersThe 1525-1596 is a 1525-1596 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 models1550 nm Fiber LasersThe 1550 is a 1550 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 models1573 nm Pulsed LasersThe 1573 is a 1573 nm nanosecond laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. 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 models1800-2000 nm Fiber LasersThe 1800-2000 is a 1800-2000 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 models1908 nm Fiber LasersThe 1908 is a 1908 nm pulsed laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. At the nominal 80 MHz repetition rate, successive pulses arrive about 12.5 ns apart.View product →
- Laser models213 nm Pulsed LasersThe 213 is a 213 nm pulsed laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample.View product →
- Laser models266 nm Pulsed LasersThe 266 is a 266 nm pulsed laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample.View product →
- Laser models280 nm Pulsed LasersThe 280 is a 280 nm nanosecond laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. 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 models2940 nm Pulsed LasersThe 2940 is a 2940 nm pulsed laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. Pulses lasting 0.9 ms deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser models320 nm Single-Frequency LasersThe 320 is a 320 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 models335 nm Single-Frequency LasersThe 335 is a 335 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 models349 nm Single-Frequency LasersThe 349 is a 349 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 models355 nm Pulsed LasersThe 355 is a 355 nm picosecond laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. 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 models355 nm Single-Frequency LasersThe 355 is a 355 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 models360 nm Single-Frequency LasersThe 360 is a 360 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 models369 nm Single-Frequency LasersThe 369 is a 369 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 models375 nm Single-Frequency LasersThe 375 is a 375 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 models405 nm Single-Frequency LasersThe 405 is a 405 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 models411 nm Single-Frequency LasersThe 411 is a 411 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 models420~1200 nm Pulsed LasersThe 420 ~ 1200 is a 420~1200 nm nanosecond laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. At the nominal 10 Hz repetition rate, pulses shorter than 8 ns arrive about 100 ms apart.View product →
- Laser models457 nm Single-Frequency LasersThe 457 is a 457 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 models473 nm Single-Frequency LasersThe 473 is a 473 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 models507 nm Fiber LasersThe 507 is a 507 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 models509 nm Fiber LasersThe 509 is a 509 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 models513 nm Fiber LasersThe 513 is a 513 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 models515 nm Single-Frequency LasersThe 515 is a 515 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 models520 nm Fiber LasersThe 520 is a 520 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 models522 nm Single-Frequency LasersThe 522 is a 522 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 models523.5 nm Single-Frequency LasersThe 523.5 is a 523.5 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 models525 nm Fiber LasersThe 525 is a 525 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 models526.5 nm Single-Frequency LasersThe 526.5 is a 526.5 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 models527 nm Pulsed LasersThe 527 is a 527 nm pulsed laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample.View product →
- Laser models532 nm Spectrum Analysis532 nm | output 1~150 mW | linewidth <1 MHz | M²: <1.1View product →
- Laser models540 nm Fiber LasersThe 540 is a 540 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 models543 nm Single-Frequency LasersThe 543 is a 543 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 models550 nm Single-Frequency LasersThe 550 is a 550 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 models552 nm Single-Frequency LasersThe 552 is a 552 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 models556 nm Components & Accessories556 nm | output 1~80 mW | linewidth <1 MHz | M²: <1.2View product →
- Laser models556 nm Pulsed LasersThe 556 is a 556 nm nanosecond laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. Pulses lasting approximately 100 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser models560 nm Fiber LasersThe 560 is a 560 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 models561 nm Single-Frequency LasersThe 561 is a 561 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 models577 nm Single-Frequency LasersThe 577 is a 577 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 models588 nm Single-Frequency LasersThe 588 is a 588 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 models589 nm Pulsed LasersThe 589 is a 589 nm nanosecond laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample.View product →
- Laser models589 nm Single-Frequency LasersThe 589 is a 589 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 models607 nm Single-Frequency LasersThe 607 is a 607 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 models618 nm Fiber LasersThe 618 is a 618 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 models631 nm Fiber LasersThe 631 is a 631 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 models633 nm Single-Frequency LasersThe 633 is a 633 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 models638 nm Single-Frequency LasersThe 638 is a 638 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 models639 nm Single-Frequency LasersThe 639 is a 639 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 models640 nm Single-Frequency LasersThe 640 is a 640 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 models656.5 nm Single-Frequency LasersThe 656.5 is a 656.5 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 models660 nm Pulsed LasersThe 660 is a 660 nm nanosecond laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. At the nominal 5 kHz repetition rate, pulses lasting approximately 150 ns arrive about 200 µs apart.View product →
- Laser models660 nm Single-Frequency LasersThe 660 is a 660 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 models671 nm Single-Frequency LasersThe 671 is a 671 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 models698 nm Single-Frequency LasersThe 698 is a 698 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 models710~810 nm Pulsed LasersThe 710 ~ 810 is a 710~810 nm nanosecond laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. Pulses lasting at most 15 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser models721 nm Single-Frequency LasersThe 721 is a 721 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 models729 nm Single-Frequency LasersThe 729 is a 729 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 models755 nm Pulsed LasersThe 755 is a 755 nm pulsed laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. At the nominal 1 Hz repetition rate, successive pulses arrive about 1 s apart.View product →
- Laser models770 nm Single-Frequency LasersThe 770 is a 770 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 models775 nm Fiber LasersThe 775 is a 775 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 models780 nm Single-Frequency LasersThe 780 is a 780 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 models783 nm Single-Frequency LasersThe 783 is a 783 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 models785 nm Single-Frequency LasersThe 785 is a 785 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 models793 nm Single-Frequency LasersThe 793 is a 793 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 models800 nm Single-Frequency LasersThe 800 is a 800 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 models808 nm 500 W Pulsed Laser808 nm Pulsed LasersThe 808 nm 500 W Pulsed Laser delivers 500 W peak illumination for high-speed imaging. Its integrated optical system, pulse driver and temperature control synchronize short light pulses with a camera through a 5 V TTL trigger. Select pulse width and repetition rate together within the recommended 2% duty cycle.View product →
- Laser models808 nm Single-Frequency LasersThe 808 is a 808 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 models830 nm Single-Frequency LasersThe 830 is a 830 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 models852 nm Single-Frequency LasersThe 852 is a 852 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 models914 nm Single-Frequency LasersThe 914 is a 914 nm laser source. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
- Laser models946 nm Single-Frequency LasersThe 946 is a 946 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 models976 nm Single-Frequency LasersThe 976 is a 976 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 modelsA/T/R Spectrum Detection SystemSpectrum AnalysisComplete equipment which is applied to sample absorbance, use to monitoring chemical reaction process, lens coating transmission band detection.View product →
- Laser modelsAO-1064A1064 nm Pulsed LasersThe AO-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 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-1064W-HE1064 nm Pulsed LasersThe AO-1064W-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 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-1342W1342 nm Pulsed LasersThe AO-1342W is a 1342 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-1573(FC)1573 nm CW LasersThe AO-1573(FC) is a 1573 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 modelsAO-266A266 nm Pulsed LasersThe AO-266A 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-266W266 nm Pulsed LasersThe AO-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 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-266W-HE266 nm Pulsed LasersThe AO-266W-HE 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. At the nominal 10 kHz repetition rate, pulses lasting approximately 12 ns arrive about 100 µs apart.View product →
- Laser modelsAO-355A355 nm Pulsed LasersThe AO-355A 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-355B355 nm Pulsed LasersThe AO-355B 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-355W355 nm Pulsed LasersThe AO-355W 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 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-532532 nm Pulsed LasersThe AO-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 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-532A532 nm Pulsed LasersThe AO-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 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-532A & 355A355 nm Pulsed LasersThe AO-532A & 355A 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 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-532B532 nm Pulsed LasersThe AO-532B 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-532W532 nm Pulsed LasersThe AO-532W 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-532W-HE532 nm Pulsed LasersThe AO-532W-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 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-532W-LP532 nm Pulsed LasersThe AO-532W-LP is a 532 nm nanosecond diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Q-switching stores energy in the gain medium while resonator losses are high, then lowers those losses to release a pulse. Pulse energy and repetition rate must be considered together, because changing the pulse spacing changes the average power for a fixed pulse energy. Pulses lasting approximately 100 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-DF-244244 nm Pulsed LasersThe AO-DF-244 is a 244 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-DF-248248 nm Pulsed LasersThe AO-DF-248 is a 248 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-DF-488488 nm Pulsed LasersThe AO-DF-488 is a 488 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 30 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
- Laser modelsAO-DF-496496 nm Pulsed LasersThe AO-DF-496 is a 496 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 4 kHz repetition rate, pulses lasting approximately 20 ns arrive about 250 µs apart.View product →
- Laser modelsAO-DP-640640 nm Pulsed LasersThe AO-DP-640 is a 640 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-I-10641064 nm Application SystemsThe AO-I-1064 is a 1064 nm nanosecond laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample. 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-K-12021202 nm Pulsed LasersThe AO-K-1202 is a 1202 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 25 ns arrive about 100 µs apart.View product →
- Laser modelsAO-K-280/20uJ280 nm Pulsed LasersThe AO-K-280/20uJ is a 280 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-K-280&295280 nm Pulsed LasersThe AO-K-280&295 is a 280 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-K-280&295&532&560280 nm Pulsed LasersThe AO-K-280&295&532&560 is a 280 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-K-289/1-5uJ289 nm Pulsed LasersThe AO-K-289/1-5uJ is a 289 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-K-295/20uJ295 nm Pulsed LasersThe AO-K-295/20uJ is a 295 nm pulsed laser source. Pulse duration sets how briefly the energy is delivered, while repetition rate sets the interval between pulses; average power alone does not describe the peak intensity at the sample.View product →
- Laser modelsAO-K-300300 nm Pulsed LasersThe AO-K-300 is a 300 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 10 ns arrive about 100 µs apart.View product →
- Laser modelsAO-K-560560 nm Pulsed LasersThe AO-K-560 is a 560 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-K-579579 nm Pulsed LasersThe AO-K-579 is a 579 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 15 ns arrive about 100 µs apart.View product →
- Laser modelsAO-K-601601 nm Pulsed LasersThe AO-K-601 is a 601 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 10 ns arrive about 100 µs apart.View product →
- Laser modelsAO-L-532532 nm Pulsed LasersThe AO-L-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 →