Efficient angle tunable output from a monolithic serial KTA optical parametric oscillator

• US 6,834,063 B2
• Filed: 08/24/2001
• Issued: 12/21/2004
• Est. Priority Date: 01/06/2000
• Status: Expired due to Term

• Current Assignee: Raytheon Company (Rtx Corporation)
• Original Assignee: Raytheon Company (Rtx Corporation)
• Inventors: Fukumoto, Joseph M.
• Primary Examiner(s): Harvey, Minsun Oh
• Assistant Examiner(s): Nguyen, Tuan N.
• Application Number:
  US09/939,004
• Publication Number:
  US 20020048077A1
• Time in Patent Office: 1,215 Days
• Field of Search: 372/21-23, 372/25, 372/20, 372/11, 372/12, 372/75, 372/97, 372/106, 359/326-332
• US Class Current: 372/21
• CPC Class Codes: G02F 1/3553 having the formula MTiOYO4, where M=K, Rb, TI, NH4 or Cs and Y=P or As, e.g. KTP
• CPC Class Codes: G02F 1/39 for parametric generation or amplification of light, infrared or ultraviolet waves
• CPC Class Codes: G02F 2201/16 series; tandem
• CPC Class Codes: G02F 2201/17 Multi-pass arrangements, i.e. arrangements to pass light a plurality of times through the same element, e.g. by using an enhancement cavity
• CPC Class Codes: G02F 2201/34 reflector
• CPC Class Codes: G02F 2203/05 wavelength dependent
• CPC Class Codes: G02F 2203/58 Multi-wavelength, e.g. operation of the device at a plurality of wavelengths
• CPC Class Codes: H01S 3/0809 Two-wavelenghth emission

Abstract

An arrangement (10) for efficiently shifting energy received at a first wavelength and outputting the shifted energy at a second wavelength. The arrangement (10) includes a laser (12) and an optical parametric oscillator (14) of unique design. The oscillator (14) is constructed with an energy shifting crystal (20) and first and second reflective elements (16) and (18) disposed on either side thereof. Light from the laser (12) at a fundamental frequency is shifted by the crystal and output at a second wavelength. The second wavelength is a secondary emission of energy induced by a primary emission generated by the first wavelength in the crystal. A novel feature of the invention is a coating applied on the reflective elements (16 and/or 18) for containing the primary emission and enhancing the secondary emission. This constrains the energy to be output by the arrangement (10) at the wavelength of the desired secondary emission.

Claims

1. An optical parametric oscillator comprising:

a crystal adapted to

receive pump energy at a first wavelength,

convert said pump energy to energy at both a primary signal wavelength and a primary idler wavelength by means of a primary process, and

convert said energy at a primary signal wavelength to energy at both a second signal wavelength and second idler wavelength by means of a cascaded secondary process; and

a mechanism disposed in functional alignment with said crystal for containing said energy at a primary signal wavelength and enhancing said secondary process thereby, said mechanism including first and second mirrors, both of said mirrors being highly reflective at said primary signal wavelength, and at least one of said mirrors being at least partially transmissive to energy at said second signal wavelength.

2. The invention of claim 1 wherein said crystal is X cut.

3. The invention of claim 1 wherein said crystal is Y cut.

4. The invention of claim 1 wherein said crystal is potassium titanyl arsenate.

5. The invention of claim 1 wherein said first wavelength is approximately 1.06 microns, said second signal wavelength is approximately 2.59 microns and said primary signal wavelength is approximately 1.53 microns.

6. The invention of claim 1 wherein said first wavelength is approximately 1.06 microns, said second signal wavelength is approximately 3.76 microns and said primary signal wavelength is approximately 1.53 microns.

7. The invention of claim 1 wherein said crystal is angle tunable.

8. The invention of claim 1 wherein both of said first and second mirrors are highly transparent at said primary idler wavelength and said secondary idler wavelength.

9. The invention of claim 1 wherein one of said first and second mirrors is highly reflective at said second signal wavelength.