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Lasers model catalog

Browse 3,778 canonical product destinations across 12 product families. Page 9 lists models 961–1,080.

Laser modelsFL-1550-SLM1550 nm Fiber LasersThe FL-1550-SLM is a 1550 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1560-SLM1560 nm Fiber LasersThe FL-1560-SLM is a 1560 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1570-SLM1570 nm Fiber LasersThe FL-1570-SLM is a 1570 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1908-LN-L1908 nm Fiber LasersThe FL-1908-LN-L is a 1908 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1908-SLM1908 nm Fiber LasersThe FL-1908-SLM is a 1908 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-1940-CW1940 nm Fiber LasersThe FL-1940-CW is a 1940 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-266-Nano266 nm Fiber LasersThe FL-266-Nano is a 266 nm nanosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-266-Pico266 nm Fiber LasersThe FL-266-Pico is a 266 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-266-PS266 nm Fiber LasersThe FL-266-PS is a 266 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. A semiconductor saturable absorber mirror (SESAM) becomes less absorbing at higher intensity, helping short pulses build through passive mode locking. Pulses shorter than 10 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsFL-343-Nano343 nm Fiber LasersThe FL-343-Nano is a 343 nm nanosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-343-Pico343 nm Fiber LasersThe FL-343-Pico is a 343 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-343-PS343 nm Fiber LasersThe FL-343-PS is a 343 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. A semiconductor saturable absorber mirror (SESAM) becomes less absorbing at higher intensity, helping short pulses build through passive mode locking. Pulses shorter than 10 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsFL-355355 nm Fiber LasersThe FL-355 is a 355 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 3 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsFL-355-Nano355 nm Fiber LasersThe FL-355-Nano is a 355 nm nanosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-355-Pico355 nm Fiber LasersThe FL-355-Pico is a 355 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-355-PS355 nm Fiber LasersThe FL-355-PS 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 10 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsFL-507-LN-L507 nm Fiber LasersThe FL-507-LN-L is a 507 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-507-SLM507 nm Fiber LasersThe FL-507-SLM is a 507 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-509-LN-L509 nm Fiber LasersThe FL-509-LN-L is a 509 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-509-SLM509 nm Fiber LasersThe FL-509-SLM is a 509 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-513-LN-L513 nm Fiber LasersThe FL-513-LN-L is a 513 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-513-SLM513 nm Fiber LasersThe FL-513-SLM is a 513 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-515-LN-L515 nm Fiber LasersThe FL-515-LN-L is a 515 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-515-Nano515 nm Fiber LasersThe FL-515-Nano is a 515 nm nanosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-515-Pico515 nm Fiber LasersThe FL-515-Pico is a 515 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-515-PS515 nm Fiber LasersThe FL-515-PS is a 515 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. A semiconductor saturable absorber mirror (SESAM) becomes less absorbing at higher intensity, helping short pulses build through passive mode locking. Pulses shorter than 10 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsFL-515-SLM515 nm Fiber LasersThe FL-515-SLM is a 515 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-520-LN-L520 nm Fiber LasersThe FL-520-LN-L is a 520 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-520-SLM520 nm Fiber LasersThe FL-520-SLM is a 520 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-525-LN-L525 nm Fiber LasersThe FL-525-LN-L is a 525 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-525-SLM525 nm Fiber LasersThe FL-525-SLM is a 525 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-532532 nm Application SystemsThe FL-532 is a 532 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 5 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsFL-532-AO532 nm Fiber LasersThe FL-532-AO is a 532 nm nanosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-532-LN-H532 nm Fiber LasersThe FL-532-LN-H is a 532 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-532-LN-L532 nm Fiber LasersThe FL-532-LN-L is a 532 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-532-Nano532 nm Fiber LasersThe FL-532-Nano is a 532 nm nanosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-532-Pico532 nm Fiber LasersThe FL-532-Pico is a 532 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-532-PS532 nm Fiber LasersThe FL-532-PS is a 532 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. A semiconductor saturable absorber mirror (SESAM) becomes less absorbing at higher intensity, helping short pulses build through passive mode locking. Pulses shorter than 10 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsFL-532-SLM532 nm Fiber LasersThe FL-532-SLM is a 532 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-532-SLM-E532 nm Fiber LasersThe FL-532-SLM-E is a 532 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-532-SLM-H532 nm Fiber LasersThe FL-532-SLM-H is a 532 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-535-Pico535 nm Fiber LasersThe FL-535-Pico is a 535 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-540-LN-L540 nm Fiber LasersThe FL-540-LN-L is a 540 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-540-Nano540 nm Fiber LasersThe FL-540-Nano is a 540 nm nanosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-540-Pico540 nm Fiber LasersThe FL-540-Pico is a 540 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-540-SLM540 nm Fiber LasersThe FL-540-SLM is a 540 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-550-LN-L550 nm Fiber LasersThe FL-550-LN-L is a 550 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-550-SLM550 nm Fiber LasersThe FL-550-SLM is a 550 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-560-LN-L560 nm Fiber LasersThe FL-560-LN-L is a 560 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-560-SLM560 nm Fiber LasersThe FL-560-SLM is a 560 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-589-CW589 nm Fiber LasersThe FL-589-CW is a 589 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-618-LN-L618 nm Fiber LasersThe FL-618-LN-L is a 618 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-618-SLM618 nm Fiber LasersThe FL-618-SLM is a 618 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-620-CW620 nm Fiber LasersThe FL-620-CW is a 620 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-631-LN-L631 nm Fiber LasersThe FL-631-LN-L is a 631 nm fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment.View product →
Laser modelsFL-631-SLM631 nm Fiber LasersThe FL-631-SLM is a 631 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-633-LN-L633 nm Fiber LasersThe FL-633-LN-L is a 633 nm fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment.View product →
Laser modelsFL-633-SLM633 nm Fiber LasersThe FL-633-SLM is a 633 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-775-LN-L775 nm Fiber LasersThe FL-775-LN-L is a 775 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-775-Pico775 nm Fiber LasersThe FL-775-Pico is a 775 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 modelsFL-775-SLM775 nm Fiber LasersThe FL-775-SLM is a 775 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-780-LN-L780 nm Fiber LasersThe FL-780-LN-L is a 780 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-780-SLM780 nm Fiber LasersThe FL-780-SLM is a 780 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-785-LN-L785 nm Fiber LasersThe FL-785-LN-L is a 785 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-785-SLM785 nm Fiber LasersThe FL-785-SLM is a 785 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-852-SLM852 nm Fiber LasersThe FL-852-SLM is a 852 nm continuous-wave fiber laser. A seed laser establishes the optical signal, and a fiber amplifier increases its power while guiding the light in active fiber. A separate nonlinear module converts the amplified light to the output wavelength. Single-longitudinal-mode operation selects one resonator frequency. Linewidth describes the spread around that frequency, while frequency drift describes how its center moves over time. This distinction matters when matching the source to a narrow resonance or an interferometer.View product →
Laser modelsFL-976-CW976 nm Fiber LasersThe FL-976-CW is a 976 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-H-1030-PS1030 nm Fiber LasersThe FL-H-1030-PS is a 1030 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 ps 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 modelsFL-H-1064-PS1064 nm Fiber LasersThe FL-H-1064-PS is a 1064 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 ps 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 modelsFL-H-515-PS515 nm Fiber LasersThe FL-H-515-PS is a 515 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
Laser modelsFL-H-532-PS532 nm Fiber LasersThe FL-H-532-PS is a 532 nm picosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
Laser modelsFL-LN-FA(1014-1120)1014 nm Fiber LasersThe FL-LN-FA(1014-1120) is a 1014 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-SC-OEM (1~200 mW)470~2400 nm Fiber LasersThe FL-SC-OEM (1~200 mW) is a 470~2400 nm picosecond supercontinuum source. Nonlinear optical processes broaden the pump light into a continuous spectrum. Filters can then select wavelength bands for an experiment. 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 2 MHz repetition rate, pulses lasting approximately 350 ps arrive about 500 ns apart.View product →
Laser modelsFL-SC-OEM (200~350 mW)470~2400 nm Fiber LasersThe FL-SC-OEM (200~350 mW) is a 470~2400 nm picosecond supercontinuum source. Nonlinear optical processes broaden the pump light into a continuous spectrum. Filters can then select wavelength bands for an experiment. 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 4 MHz repetition rate, pulses lasting approximately 350 ps arrive about 250 ns apart.View product →
Laser modelsFL-SC-OEM (350~500 mW)470~2400 nm Fiber LasersThe FL-SC-OEM (350~500 mW) is a 470~2400 nm picosecond supercontinuum source. Nonlinear optical processes broaden the pump light into a continuous spectrum. Filters can then select wavelength bands for an experiment. 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 350 ps deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsFL-SC-OEM (500~1000 mW)470~2400 nm Fiber LasersThe FL-SC-OEM (500~1000 mW) is a 470~2400 nm nanosecond supercontinuum source. Nonlinear optical processes broaden the pump light into a continuous spectrum. Filters can then select wavelength bands for an experiment. 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 MHz repetition rate, pulses lasting 1.5 ns arrive about 1 µs apart.View product →
Laser modelsFL-SLM-Seed(1014-1120)1014 nm Fiber LasersThe FL-SLM-Seed(1014-1120) is a 1014 nm continuous-wave fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsFL-SLM-Seed(1800-2000)1800 nm Fiber LasersThe FL-SLM-Seed(1800-2000) is a 1800 nm fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment.View product →
Laser modelsFlow CytometryApplication SystemsThe Flow Cytometry is a laser source. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsFluorescence SpectrometerSpectrum AnalysisWith high sensitivity, strong selectivity, micro samples and simple operation, it is applied to cry stal, rare earth elements and other fluorescence spectrum detection.View product →
Laser modelsFN-522522 nm CW LasersThe FN-522 is a 522 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 modelsFS-F-1030A1030 nm Pulsed LasersThe FS-F-1030A is a 1030 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 MHz repetition rate, pulses shorter than 300 fs arrive about 1 µs apart. An integrated acousto-optic modulator controls intensity by diffracting light, allowing fast power modulation after the light is generated.View product →
Laser modelsFS-F-1030B1030 nm Pulsed LasersThe FS-F-1030B is a 1030 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 300 fs deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample. An integrated acousto-optic modulator controls intensity by diffracting light, allowing fast power modulation after the light is generated.View product →
Laser modelsFS-F-1030B&515B1030 nm Pulsed LasersThe FS-F-1030B&515B is a 1030 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 300 fs deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample. An integrated acousto-optic modulator controls intensity by diffracting light, allowing fast power modulation after the light is generated.View product →
Laser modelsFS-F-1030C1030 nm Pulsed LasersThe FS-F-1030C is a 1030 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 MHz repetition rate, pulses shorter than 300 fs arrive about 1 µs apart. An integrated acousto-optic modulator controls intensity by diffracting light, allowing fast power modulation after the light is generated.View product →
Laser modelsFS-F-1030D1030 nm Pulsed LasersThe FS-F-1030D is a 1030 nm pulsed fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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. An integrated acousto-optic modulator controls intensity by diffracting light, allowing fast power modulation after the light is generated.View product →
Laser modelsFS-F-515A515 nm Pulsed LasersThe FS-F-515A is a 515 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 MHz repetition rate, pulses shorter than 300 fs arrive about 1 µs apart. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
Laser modelsFS-F-515B515 nm Pulsed LasersThe FS-F-515B is a 515 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 300 fs 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 modelsFS-F-515C515 nm Pulsed LasersThe FS-F-515C is a 515 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 300 fs 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 modelsFS-F-515D515 nm Pulsed LasersThe FS-F-515D is a 515 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 300 fs 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 modelsFS-G-1030A1030 nm Pulsed LasersThe FS-G-1030A is a 1030 nm femtosecond 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 800 fs deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample. An integrated acousto-optic modulator controls intensity by diffracting light, allowing fast power modulation after the light is generated. The stated optical loss through this stage is 15%.View product →
Laser modelsFS-G-1030B1030 nm Pulsed LasersThe FS-G-1030B is a 1030 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. An integrated acousto-optic modulator controls intensity by diffracting light, allowing fast power modulation after the light is generated.View product →
Laser modelsFS-G-515A515 nm Pulsed LasersThe FS-G-515A is a 515 nm femtosecond 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 500 fs deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample. An integrated acousto-optic modulator controls intensity by diffracting light, allowing fast power modulation after the light is generated.View product →
Laser modelsFS-H-1030A1030 nm Pulsed LasersThe FS-H-1030A is a 1030 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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, pulses shorter than 150 fs arrive about 12.5 ns apart. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
Laser modelsFS-H-1030B1030 nm Pulsed LasersThe FS-H-1030B is a 1030 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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, pulses shorter than 150 fs arrive about 12.5 ns apart. An integrated acousto-optic modulator controls intensity by diffracting light, allowing fast power modulation after the light is generated. The stated optical loss through this stage is 15%.View product →
Laser modelsFS-H-1030C1030 nm Pulsed LasersThe FS-H-1030C is a 1030 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 250 fs deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample. An integrated acousto-optic modulator controls intensity by diffracting light, allowing fast power modulation after the light is generated.View product →
Laser modelsFS-H-1030D1030 nm Pulsed LasersThe FS-H-1030D is a 1030 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 250 fs deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample. An integrated acousto-optic modulator controls intensity by diffracting light, allowing fast power modulation after the light is generated.View product →
Laser modelsFS-H-1030E1030 nm Pulsed LasersThe FS-H-1030E is a 1030 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 250 fs deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample. An integrated acousto-optic modulator controls intensity by diffracting light, allowing fast power modulation after the light is generated.View product →
Laser modelsFS-H-1064A1064 nm Pulsed LasersThe FS-H-1064A is a 1064 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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, pulses shorter than 150 fs arrive about 12.5 ns apart. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
Laser modelsFS-H-1064B1064 nm Pulsed LasersThe FS-H-1064B is a 1064 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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, pulses shorter than 150 fs arrive about 12.5 ns apart. An integrated acousto-optic modulator controls intensity by diffracting light, allowing fast power modulation after the light is generated. The stated optical loss through this stage is 15%. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
Laser modelsFS-H-1560A1560 nm Pulsed LasersThe FS-H-1560A is a 1560 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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, pulses shorter than 50 fs arrive about 12.5 ns apart. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
Laser modelsFS-H-515A515 nm Pulsed LasersThe FS-H-515A is a 515 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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, pulses shorter than 150 fs arrive about 12.5 ns apart. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
Laser modelsFS-H-515B515 nm Pulsed LasersThe FS-H-515B is a 515 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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, pulses shorter than 150 fs arrive about 12.5 ns apart. An integrated acousto-optic modulator controls intensity by diffracting light, allowing fast power modulation after the light is generated. The stated optical loss through this stage is 15%. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
Laser modelsFS-H-515C515 nm Pulsed LasersThe FS-H-515C is a 515 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 250 fs 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 modelsFS-H-515D515 nm Pulsed LasersThe FS-H-515D is a 515 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 250 fs 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 modelsFS-H-515E515 nm Pulsed LasersThe FS-H-515E is a 515 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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 250 fs 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 modelsFS-H-532A532 nm Pulsed LasersThe FS-H-532A is a 532 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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, pulses shorter than 150 fs arrive about 12.5 ns apart. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
Laser modelsFS-H-532B532 nm Pulsed LasersThe FS-H-532B is a 532 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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, pulses shorter than 150 fs arrive about 12.5 ns apart. An integrated acousto-optic modulator controls intensity by diffracting light, allowing fast power modulation after the light is generated. The stated optical loss through this stage is 15%. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
Laser modelsFS-H-780A780 nm Pulsed LasersThe FS-H-780A is a 780 nm femtosecond fiber laser. Pump energy is supplied to an active fiber, which guides the light and provides optical gain as it propagates. Output coupling then delivers the amplified beam to the experiment. 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, pulses shorter than 100 fs arrive about 12.5 ns apart. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →
Laser modelsFull-Spectrum Optical Parameter Testing SystemMeasurement & SafetyKey components: collimator, multi-spectral target generator, high-precision rotation stage, and image analyzer on an optical platform.View product →
Laser modelsH-420420 nm CW LasersThe H-420 is a 420 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 modelsHigh Stability637 nm CW LasersThe High Stability is a 637 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsHigh Stability457 nm CW LasersThe High Stability is a 457 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsHigh Stability488 nm CW LasersThe High Stability is a 488 nm continuous-wave laser source. Continuous-wave operation provides a sustained beam for experiments that need steady illumination. Output power describes the optical energy delivered per second. At the sample, irradiance also depends on the beam area and losses through the optical path, so the delivered spot must be considered along with the source rating.View product →
Laser modelsHLS-1000 Halogen Tungsten Light Source2000 nm Spectrum Analysis2000 nm | Wide range of continuous spectrum (340-2000nm), can be used for sample detection of absorbance and transmittance.View product →
Laser modelsHLS-2000 Halogen Tungsten Light Source1600 nm Spectrum Analysis1600 nm | Wide range of continuous spectrum (400-1600nm), can be used for brightfield microscopy, laboratory and illumination.View product →
Laser modelsHPL-1064-CW1064 nm CW LasersThe HPL-1064-CW is a 1064 nm continuous-wave diode-pumped solid-state laser. Laser diodes optically pump a solid gain medium inside a resonator. The pump supplies the energy; repeated passes through the gain medium amplify the laser light. Continuous-wave operation provides a sustained beam for experiments that need steady illumination.View product →
Laser modelsHPL-1064-Q1064 nm Pulsed LasersThe HPL-1064-Q 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 100 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsHPL-1064-QM1064 nm Pulsed LasersThe HPL-1064-QM 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 300 ns deliver the energy in a brief interval; pulse energy and focused spot size determine the intensity at the sample.View product →
Laser modelsHPL-1064A-PA1064 nm Pulsed LasersThe HPL-1064A-PA 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 200 Hz repetition rate, pulses lasting approximately 10 ns arrive about 5 ms apart. The quoted power range represents factory-set configurations; specify the required output rating when ordering.View product →

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