Q0002-QL080-015-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0002-QL080-015-1064

Q0003-QL080-015-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0003-QL080-015-1064

Q0015-FL027-040-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0015-FL027-040-1064

Q0016-FL041-050-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0016-FL041-050-1064

Q0017-QL080-030-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0017-QL080-030-1064

Q0018-QL041-015-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0018-QL041-015-1064

Q0019-QL068-030-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0019-QL068-030-1064

Q0020-FL027-060-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0020-FL027-060-1064

Q0021-FS041-060-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0021-FS041-060-1064

Q0022-QL068-060-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0022-QL068-060-1064

Q0023-QL080-010-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0023-QL080-010-1064

Q0027-QL080-015-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0027-QL080-015-1064

Q0029-QL080-015-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0029-QL080-015-1064

Q0030-QL080-012-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0030-QL080-012-1064

Q0031-QL041-015-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0031-QL041-015-1064

Q0032-QL080-025-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0032-QL080-025-1064

Q0033-QL068-030-1030

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0033-QL068-030-1030

Q0034-QL080-012-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0034-QL080-012-1064

Q0035-QL041-015-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0035-QL041-015-1064

Q0036-FS041-060-2000

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0036-FS041-060-2000

Q0037-FS068-060-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0037-FS068-060-1064

Q0038-QL080-050-1030

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0038-QL080-050-1030

Q0040-FL027-020-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0040-FL027-020-1064

Q0041-QL068-025-1880

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0041-QL068-025-1880

Q0042-QL080-015-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0042-QL080-015-1064

Q0043-QL041-040-2000

ModuOptik has a complete solution can be applied to polarized(Brewster angle cut)or non-polarized lasers and can be adapted to lamp pumped lasers and LD pumped lasers.Our AOQS product wavelength range from UV to far infrared,diameter up to 12 mm.AOQS selects AO materials with excellent quality (Fused quartz,Crystalline quartz,Gecrystal,etc.),which can be designed into shearand longitudinal wave mode according to needs.High quality optical polishing,anti-reflective coatings with low reflection and high damage threshold,reliable welding techniques,and novel acoustic management and optical mechanical design techniques enable excellent thermal management, maintaining excellent beam quality and high transmittance.

Q0043-QL041-040-2000

Q0044-QL041-012-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0044-QL041-012-1064

Q0045-QL080-010-1540

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0045-QL080-010-1540

Q0046-FS027-020-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0046-FS027-020-1064

Q0047-TL080-012-1030

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0047-TL080-012-1030

Q0048-QL080-010-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0048-QL080-010-1064

Q0049-FL041-040-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0049-FL041-040-1064

Q0050-FS041-040-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0050-FS041-040-1064

Q0051-FS041-050-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0051-FS041-050-1064

Q0052-FL027-020-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0052-FL027-020-1064

Q0053-FL041-020-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0053-FL041-020-1064

Q0054-QL060-040-1030

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0054-QL060-040-1030

Q0056-QL080-030-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0056-QL080-030-1064

Q0057-QL080-010-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0057-QL080-010-1064

Q0058-QL080-015-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0058-QL080-015-1064

Q0059-QL080-010-1535

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0059-QL080-010-1535

Q0060-QL080-015-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0060-QL080-015-1064

Q0061-QL080-015-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0061-QL080-015-1064

Q0062-QL080-010-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0062-QL080-010-1064

Q0063-QL041-015-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0063-QL041-015-1064

Q0065-FL027-030-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0065-FL027-030-1064

Q0066-QL041-050-2000

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0066-QL041-050-2000

Q0067-FS050-030-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0067-FS050-030-1064

Q0068-QL080-012-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0068-QL080-012-1064

Q0069-QL080-015-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0069-QL080-015-1064

Q0070-TL120-010-1064

Acousto-optic Q-switches are in-cavity devices used to generate very high peak power, short duration laser pulses. Acousto-optic Q-switches are typically loss modulators that operate on a zero-level beam. The goal of a Q-switch is to diffract as much power as possible from the zero-level to increase cavity losses and prevent laser output. When the Q-switched RF driver turns off instantaneously, the optical power accumulated in the laser is emitted as a short pulse. The process can be repeated at a rate of more than 100KHz. Depending on the frequency and interaction length, acousto-optic Q-switches either operate in Bragg mode, like AOM, using mainly a single diffracted beam, or use multiple diffracted beams in Raman-Nath mode.

Q0070-TL120-010-1064

M0006-QL110-030-532

Acousto optic modulators (AOM) are commonly used to adjust laser intensity (amplitude modulation,AM) outside the laser cavity. This can be simple ON/OFF modulation for fast switching, or variable modulation for laser intensity. The modulation mode is determined by the type of RF driver, which can be digital (on/off) or analog (sinusoidal, square wave, linear, random, etc). Generally, the RF driver of AOM operates at a fixed frequency.

M0006-QL110-030-532

M0009-QL170-060-355

Acousto optic modulators (AOM) are commonly used to adjust laser intensity (amplitude modulation,AM) outside the laser cavity. This can be simple ON/OFF modulation for fast switching, or variable modulation for laser intensity. The modulation mode is determined by the type of RF driver, which can be digital (on/off) or analog (sinusoidal, square wave, linear, random, etc). Generally, the RF driver of AOM operates at a fixed frequency.

M0009-QL170-060-355

M0010-TL080-020-450-900

Acousto optic modulators (AOM) are commonly used to adjust laser intensity (amplitude modulation,AM) outside the laser cavity. This can be simple ON/OFF modulation for fast switching, or variable modulation for laser intensity. The modulation mode is determined by the type of RF driver, which can be digital (on/off) or analog (sinusoidal, square wave, linear, random, etc). Generally, the RF driver of AOM operates at a fixed frequency.

M0010-TL080-020-450-900

M0011-QL110-060-343

Acousto optic modulators (AOM) are commonly used to adjust laser intensity (amplitude modulation,AM) outside the laser cavity. This can be simple ON/OFF modulation for fast switching, or variable modulation for laser intensity. The modulation mode is determined by the type of RF driver, which can be digital (on/off) or analog (sinusoidal, square wave, linear, random, etc). Generally, the RF driver of AOM operates at a fixed frequency.

M0011-QL110-060-343

M0012-QL200-035-266

Acousto optic modulators (AOM) are commonly used to adjust laser intensity (amplitude modulation,AM) outside the laser cavity. This can be simple ON/OFF modulation for fast switching, or variable modulation for laser intensity. The modulation mode is determined by the type of RF driver, which can be digital (on/off) or analog (sinusoidal, square wave, linear, random, etc). Generally, the RF driver of AOM operates at a fixed frequency.

M0012-QL200-035-266

M0015-QL100-030-780

Acousto optic modulators (AOM) are commonly used to adjust laser intensity (amplitude modulation,AM) outside the laser cavity. This can be simple ON/OFF modulation for fast switching, or variable modulation for laser intensity. The modulation mode is determined by the type of RF driver, which can be digital (on/off) or analog (sinusoidal, square wave, linear, random, etc). Generally, the RF driver of AOM operates at a fixed frequency.

M0015-QL100-030-780

M0016-QL100-010-800

Acousto optic modulators (AOM) are commonly used to adjust laser intensity (amplitude modulation,AM) outside the laser cavity. This can be simple ON/OFF modulation for fast switching, or variable modulation for laser intensity. The modulation mode is determined by the type of RF driver, which can be digital (on/off) or analog (sinusoidal, square wave, linear, random, etc). Generally, the RF driver of AOM operates at a fixed frequency.

M0016-QL100-010-800

M0017-TL250-003-780-950

Acousto optic modulators (AOM) are commonly used to adjust laser intensity (amplitude modulation,AM) outside the laser cavity. This can be simple ON/OFF modulation for fast switching, or variable modulation for laser intensity. The modulation mode is determined by the type of RF driver, which can be digital (on/off) or analog (sinusoidal, square wave, linear, random, etc). Generally, the RF driver of AOM operates at a fixed frequency.

M0017-TL250-003-780-950

M0020-QL170-050-405

Acousto optic modulators (AOM) are commonly used to adjust laser intensity (amplitude modulation,AM) outside the laser cavity. This can be simple ON/OFF modulation for fast switching, or variable modulation for laser intensity. The modulation mode is determined by the type of RF driver, which can be digital (on/off) or analog (sinusoidal, square wave, linear, random, etc). Generally, the RF driver of AOM operates at a fixed frequency.

M0020-QL170-050-405