Passive Q-switch laser and method for optimizing action of the same

Patent metadata

Field	Value
Publication number	US-10153607-B2
Application number	US-201515565607-A
Country	US
Kind code	B2
Filing date	May 12, 2015
Priority date	May 12, 2015
Publication date	Dec 11, 2018
Grant date	Dec 11, 2018

Abstract

A passive Q-switch laser has an excitation source 1 for outputting excitation light; a laser medium 3 between a pair of reflective mirrors 5a, 5b that constitute part of an optical resonator, the laser medium emitting laser light upon being excited by the excitation light from the excitation source: a saturable absorber 4 disposed between the pair of reflective mirrors, the saturable absorber being configured such that the transmittance thereof increases as the laser light beam the laser medium is absorbed, a matrix table 22 in which the excitation-source output and the optimal value of the pulse width are stored in association with the repetition frequency; and a control unit 21 for referring to the matrix table, reading out the excitation-source output and the optimal value of the pulse width that correspond to an inputted repetition frequency, and controlling the excitation source such that the read-out excitation-source output and optimal value of the pulse width are attained.

First claim

What is claimed is:

1. A passive Q-switch laser, comprising:
an excitation source that is excited at a repetition frequency and outputs an excitation light;
a laser medium that is in-place between a pair of reflection mirrors consisting of an optic resonator that emits a laser beam excited by the excitation light from the excitation source;
a saturable absorber that is in-place between said pair of the mirrors increases a transmittance in accordance with an absorption of the laser beam from said laser medium;
a matrix table that stores an output of said excitation source relative to said repetition frequency in coordination with an optimal value of a pulse width;
a control element that reads out the optimal value of the output of said excitation source and the optimal value of the pulse width, respectively corresponding to the input repetition frequency, referring to said matrix table and controls said excitation source to provide the respective values that are the same as the optimal value of the read-out output of said excitation source and the optimal value of the pulse width;
a first wavelength conversion element that converts a fundamental wave, which is a laser beam from said saturable absorber, to a second harmonic; and
a second wavelength conversion element that converts the second harmonic from said first wavelength conversion element and the rest of the fundamental wave to a third harmonic;
wherein:
said matrix table stores correspondingly an optimal value of a temperature of said first wavelength conversion element and an optimal value of temperature of said second wavelength conversion element, which are corresponding to said repetition frequency; said control element, referring to said matrix table, reads out an optimal value of temperature of said first wavelength conversion element and an optimal value of temperature of said second wavelength conversion element, which are corresponding to said input-repetition frequency; and which controls the temperature of said first wavelength conversion element and the temperature of said second wavelength conversion element to be respectively equal to a read-out optimal value of the temperature of said first wavelength conversion element and a read-out optimal value of said second wavelength conversion element.

2. The passive Q-switch laser, according to claim 1 , further comprising:
a temperature adjustment element that is installed to said first wavelength conversion element and said second wavelength conversion element respectively; and
wherein, said control element outputs a temperature control signal that controls said temperature adjustment element.

3. The passive Q-switch laser, according to claim 1 , wherein:
said laser medium comprises a rare-earth dope YAG.

4. The passive Q-switch laser, according to claim 1 , wherein:
said saturable absorber comprises Cr:YAG.

5. An operation optimization method of a passive Q-switch laser, which comprises an excitation source that is excited at a repetition frequency and outputs an excitation light; a laser medium that is in-place between a pair of reflection mirrors consisting of a optic resonator outputs a laser beam excited by an excitation light from said excitation source; and a saturable absorber that is in-place between said pair of the mirrors increases a transmittance in accordance with an absorption of the laser beam from said laser medium; the method comprising steps of:
generating a matrix table that stores an optimal value of the output of said excitation source and an optimal value of the pulse width relative to said repetition frequency in coordination with one another; and
controlling said control element that reads out the optimal value of the output of said excitation source and the optimal value of the pulse width, respectively corresponding to the input repetition frequency, and that refers to said matrix table and controls the excitation source so as to have a read-out optimal value of the output of said excitation source and a read-out optimal value of the pulse width; and
wherein said passive Q-switch laser further comprises:
a first wavelength conversion element that converts a fundamental wave, which is a laser beam from said saturable absorber, to a second harmonic; and
a second wavelength conversion element that converts the second harmonic from said first wavelength conversion element and the rest of the fundamental wave to a third harmonic;
wherein said matrix table stores correspondingly an optimal value of a temperature of said first wavelength conversion element and an optimal value of temperature of said second wavelength conversion element, which are corresponding to said repetition frequency; said control element, referring to said matrix table, reads out an optimal value of temperature of said first wavelength conversion element and an optimal value of temperature of said second wavelength conversion element, which are corresponding to said input-repetition frequency; and which controls the temperature of said first wavelength conversion element and the temperature of said second wavelength conversion element to be respectively equal to a read-out optimal value of the temperature of said first wavelength conversion element and a read-out optimal value of said second wavelength conversion element.

Assignees

• Shimadzu Corp

Inventors

• Bhandari Rakesh
• Tojo Koji
• Ishigaki Naoya
• Uno Shingo

Classifications

• G02F1/37

  for second-harmonic generation {(G02F1/3532 takes precedence)} · CPC title

• H01S3/0092

  Nonlinear frequency conversion, e.g. second harmonic generation [SHG] or sum- or difference-frequency generation outside the laser cavity (nonlinear frequency conversion per se G02F1/35) · CPC title

• H01S3/09415

  the pumping beam being parallel to the lasing mode of the pumped medium, e.g. end-pumping · CPC title

• H01S3/1022

  by controlling the optical pumping · CPC title

• H01S3/113 Primary

  using intracavity saturable absorbers · CPC title