Solid state lasers with spherical resonators

• US 4,829,537 A
• Filed: 12/01/1986
• Issued: 05/09/1989
• Est. Priority Date: 12/01/1986
• Status: Expired due to Fees

• Current Assignee: Spectra-Physics Incorporated (MKS Instruments Incorporated)
• Original Assignee: Spectra-Physics Incorporated (MKS Instruments Incorporated)
• Inventors: Baer, Thomas M.
• Primary Examiner(s): NOT, DEFINED
• Assistant Examiner(s): Vo, Xuan T.
• Application Number:
  US06/936,284
• Time in Patent Office: 890 Days
• Field of Search: 372/66, 372/108, 372/92, 372/95, 372/72, 372/16, 372/75, 372/97, 372/99, 372/109, 372/705, 372/94, 356/350
• US Class Current: 372/66
• CPC Class Codes: G01C 19/64 Gyrometers using the Sagnac effect, i.e. rotation-induced shifts between counter-rotating electromagnetic beams
• CPC Class Codes: H01S 3/0602 Crystal lasers or glass lasers H01S3/063 takes precedence
• CPC Class Codes: H01S 3/0627 the resonator being monolithic, e.g. microlaser
• CPC Class Codes: H01S 3/083 Ring lasers fibre ring lasers H01S3/06791

Abstract

A nonstandard spherical resonator which produces laser radiation having spherical modes of oscillation is formed entirely within a sphere of laser gain material. The resonator is pumped to produce the spherical modes. By pumping an isotropically coated sphere at normal incidence the entire sphere forms the resonator, and the laser radiates uniformly in all directions as from a point source. By pumping obliquely to totally internally reflect the laser radiation at the surface of the sphere, or by applying an equatorial coating on the sphere to internally reflect the laser radiation, toroidal region within the sphere forms the resonator. The pumping volume can be controlled so that the laser radiation is single longitudinal mode and single frequency by limiting the active mode volume. Prisms can be used for input and output coupling to the toroidal resonator; and optical fiber can also be used for output coupling. A compact laser design uses a Nd:YAG sphere pumped by a laser diode. The spherical resonators can be used for traking, holography, levelling and ring laser gyroscope applications. The toroidal resonator forms an ideal ring laser for use as a gyroscope; a sphere with three orthongonal toroidal resonators provides three degree of freedom measurement capability.

Claims

1. A laser apparatus comprising:

a laser gain medium formed in the shape of a solid sphere;

pumping means operatively associated with the gain medium for exciting a pumping volume in the sphere;

a resonant cavity formed within and entirely enclosed within the sphere wherein laser radiation having spherical modes of oscillation is produced when the gain medium in the pumping volume is excited by the pumping means;

output coupling means for removing a portion of the laser radiation.

2. The apparatus of claim 1 wherein the sphere is made of Nd:

YAG.

3. The apparatus of claim 1 wherein the pumping means is a laser diode.

4. The apparatus of claim 1 wherein the pumping means is oriented so that pumping radiation is incident obliquely onto the sphere and the resonant cavity is a toroidal shaped region which is formed by total internal reflection of laser radiation at the surface of the sphere.

5. The apparatus of claim 4 further including an input coupling prism contacting the sphere through which pumping radiation is input into the sphere so that the pumping radiation is totally internally reflected in the sphere.

6. The apparatus of claim 1 further including an equatorial coating on the sphere which is highly transmissive to pumping radiation and highly reflective to laser radiation and wherein the pumping radiation is incident obliquely onto the sphere and the resonant cavity is a toroidal shaped region which is formed by reflection of the laser radiation by the equatorial coating.

7. The apparatus of claim 1 further including an isotropic coating on the entire surface of the sphere which is highly transmissive to pumping radiation and highly reflective to laser radiation wherein the pumping means is oriented so that the pumping radiation is incident normal to the sphere and the resonant cavity occupies the entire sphere.

8. The apparatus of claim 5 wherein the input coupling prism is rotatable to select the pumping volume within the sphere.

9. The apparatus of claim 1 wherein the resonant cavity is a toroidal shaped region contacting the surface of the sphere which produces laser radiation which radiates in a circle in the plane of the toroidal region.

10. The apparatus of claim 9 wherein the pumping volume is matched to an active mode volume in the resonant cavity which produces laser radiation which is single longitudinal mode and single frequency.

11. The apparatus of claim 4 wherein the output coupling means is an output coupling prism placed adjacent to a point on the surface of the sphere to frustrate total internal reflection at that point.

12. The apparatus of claim 4 wherein the output coupling means is an optical fiber contacting a point on the surface of the sphere and oriented so that the laser radiation from the sphere is emitted within the acceptance angle of the fiber.

13. The apparatus of claim 9 further including a detector operatively connected to the toroidal resonant cavity to detect changes in the laser radiation produced by rotation of the sphere.

14. A three degree of freedom laser gyroscope, comprising:

a laser gain medium formed in the shape of a solid sphere;

pumping means operatively associated with the gain medium;

three orthogonal toroidal resonant cavities formed within and entirely enclosed within the sphere when the gain medium in each cavity is pumped by the pumping means;

detector means operatively connected to each of the three toroidal resonator cavities to detect variations in the laser radiation produced in each cavity by rotation of the sphere.

15. A method of producing laser radiation, comprising:

forming a laser gain medium into a solid sphere;

forming a laser resonant cavity within the sphere of gain material which produces laser radiation having spherical modes of oscillation;

pumping a pumping volume in the gain medium in the cavity to produce an active mode volume in the resonant cavity;

removing laser radiation from the cavity.

16. The method of claim 15 wherein the resonant cavity is formed by totally internally reflecting laser radiation from the surface of the sphere to create a toroidal shaped resonant cavity contacting the surface of the sphere along an equatorial circle where total internal reflection occurs.

17. The method of claim 15 wherein the resonant cavity is formed by forming an equatorial coating on the surface of the sphere which is highly reflective to laser radiation and highly transmissive to pumping radiation to create a toroidal shaped resonant cavity within the sphere.

18. The method of claim 15 wherein the resonant cavity is formed by forming an isotropic coating on the entire surface of the sphere which is highly reflective to laser radiation and highly transmissive to pumping radiation.

19. The method of claim 15 wherein the sphere is formed of Nd:

YAG and pumped by a laser diode.