Optical wavelength conversion method and laser-diode-pumped solid-state laser

• US 5,175,741 A
• Filed: 06/07/1990
• Issued: 12/29/1992
• Est. Priority Date: 06/07/1989
• Status: Expired due to Term

• Current Assignee: Fujifilm Corporation (Fujifilm Holdings Corporation)
• Original Assignee: Fuji Photo Film Co Limited (Fujifilm Holdings Corporation)
• Inventors: Okazaki, Yoji
• Primary Examiner(s): Epps, Georgia Y.
• Application Number:
  US07/534,214
• Time in Patent Office: 936 Days
• Field of Search: 372/21, 372/75, 372/69, 372/70, 359/326, 359/328
• US Class Current: 372/75
• CPC Class Codes: G02F 1/3534 Three-wave interaction, e.g. sum-difference frequency generation G02F1/3532 takes precedence
• CPC Class Codes: H01S 3/108 using non-linear optical devices, e.g. exhibiting Brillouin or Raman scattering mode locking using a non-linear element H01S3/1112

Abstract

An optical wavelength conversion method employs a bulk-crystal-type optical wavelength converter device of a single crystal of nonlinear optical material known as PRA. Linearly polarized fundamental waves whose wavelengths range from 450 to 4,000 nm are applied to the bulk single crystal, and angle phase matching of the type I is achieved, thereby producing a wave whose frequency is the sum of the frequencies of the applied fundamental waves. A laser-diode-pumped solid-state laser includes a solid-state laser rod doped with a rare-earth material such as neodymium or the like and pumped by a semiconductor laser, and a bulk single crystal of organic nonlinear optical material disposed in a resonator. The bulk single crystal converts the wavelength of a laser beam which is oscillated by the solid-state laser rod and the wavelength of a pumping laser beam into the wavelength of a wave whose frequency is the sum of the frequencies of the laser beams.

Claims

1. A method of converting the wavelengths of two linearly polarized fundamental waves applied to a bulk single crystal of a nonlinear optical material represented by the following molecular diagram:

##STR2## into the wavelength of a sum-frequency wave whose frequency is the sum of the frequencies of the fundamental waves, said method comprising the step of;

i) applying fundamental waves whose wavelengths range from 450 to 4,000 nm to the nonlinear optical material to achieve angle phase matching of the type I, thereby producing a wave whose frequency is the sum of the frequencies of the applied fundamental waves.

2. A laser-diode-pumped solid-state laser comprising:

i) a solid-state laser rod doped with a rare-earth material;

ii) a semiconductor laser for emitting a laser beam to pump said solid-state laser rod to oscillate a beam; and

iii) a resonator including a bulk single crystal of an organic nonlinear optical material for converting the wavelength of the beam which is oscillated by said solid-state laser rod and the wavelength of the laser beam which is emitted by said semiconductor laser into the wavelength of a sum-frequency wave whose frequency is the sum of the frequencies of the oscillated beam and the laser beam, wherein said organic nonlinear optical material is represented by the following formula;

##STR3##

4. A laser-diode-pumped solid-state laser according to claim 2, wherein said solid-state laser rod and said semi-conductor laser produce laser beams having wavelengths ranging from 450 to 4,000 nm, said bulk single crystal being arranged to achieve angle phase matching of the type I for generating said sum-frequency wave.

6. A laser-diode-pumped solid-state laser according to any one of claims 2, 3, 4 and 5 wherein said semiconductor laser comprises a single-transverse-mode, single-longitudinal-mode semiconductor laser.

3. A laser-diode-pumped solid-state laser comprising:

i) a solid-state laser rod doped with a rare-earth material;

ii) a semiconductor laser for emitting a laser beam to pump said solid-state laser rod to oscillate a beam;

iii) a laser beam source, separate from said semiconductor laser, for emitting a laser beam; and

iv) a resonator including a bulk single crystal of an organic nonlinear optical material for converting the wavelength of the beam which is oscillated by said solid-state laser rod and the wavelength of the laser beam which is emitted by said laser beam source into the wavelength of a sum-frequency wave whose frequency is the sum of the frequencies of the oscillated beam and the laser beam, wherein said organic nonlinear optical material is represented by the following formula;

##STR4##

5. A laser-diode-pumped solid-state laser according to claim 3, wherein said solid-state laser rod and said laser beam source produce laser beams having wavelengths ranging from 450 to 4,000 nm, said bulk single crystal being arranged to achieve angle phase matching of Type I for generating sum-frequency wave.