Multiple crystal pumping cavity laser with thermal and mechanical isolation

• US 4,910,746 A
• Filed: 11/09/1988
• Issued: 03/20/1990
• Est. Priority Date: 06/14/1984
• Status: Expired due to Fees

• Current Assignee: Holographics Incorporated
• Original Assignee: Holographics Incorporated
• Inventors: Nicholson, Peter
• Primary Examiner(s): Scott, Jr., Leon
• Application Number:
  US07/270,425
• Time in Patent Office: 496 Days
• Field of Search: 372/38, 372/68, 372/69, 372/66, 372/41, 372/72, 372/35, 372/19, 372/97, 372/20
• US Class Current: 372/68
• CPC Class Codes: H01S 3/025 of solid state lasers, e.g. housings or mountings
• CPC Class Codes: H01S 3/0912 Electronics or drivers for the pump source, i.e. details of drivers or circuitry specific for laser pumping laser diode drivers H01S5/042
• CPC Class Codes: H01S 3/093 focusing or directing the excitation energy into the active medium
• CPC Class Codes: H01S 3/2316 Cascaded amplifiers

Abstract

A multiple crystal, single pumping cavity laser system comprises an optical pumping cavity, several laser crystal rods disposed in the cavity and having differently sized diameters and with their axes parallel, an optical coupling device for coupling the rods in a chain of increasing diametrical size, an optical pumping source for providing an optimum pumping level for the largest rod, and attenuators for all but the largest sized rod for attenuating the energy absorbed by the smaller rods. Since all of the laser rods are disposed and pumped in a single pumping capacity, only a single pumping source is required. The housing containing the pumping cavity is thermally and mechanically isolated from the rail holding the other system components to prevent shock from being transmitted to the other components.

Claims

1. A laser system comprising:

an optical pumping chamber;

a plurality of laser crystals enclosed in said pumping chamber each of which requires a different optimum level of pumping energy for generating a desired mode therein;

pumping means for optically supplying energy to said pumping chamber at a level which is optimum for a first enclosed laser crystal requiring the highest level of pumping energy; and

attenuating means disposed within said pumping chamber for selectively limiting the pumping energy supplied to each, except the first, of said laser crystals to a level that is optimum for generating a desired mode therein.

2. A laser system according to claim 1, wherein said attenuating means comprises a plurality of dielectric-coated flow tubes each enclosing a respective one, except the first, of said laser crystals for reflecting a predetermined portion of the pumping energy incident thereon back into the pumping chamber.

3. A laser system according to claim 1, wherein said attenuating means comprises a plurality of flow tubes each enclosing a respective one, except the first, of said laser crystals, at least one of the inner and outer surfaces of each of said flow tubes being suitably diffuse to absorb a predetermined amount of the pumping energy incident thereon.

4. A laser system according to claim 1, wherein said attenuating means comprises a plurality of substantially light-transparent flow tubes each enclosing a respective one, except the first, of said laser crystals, and means for pumping through said flow tubes a light-absorbing dye that absorbs a predetermined amount of the incident pumping energy within the pump band of the enclosed crystal.

5. A laser system according to claim 1, wherein said attenuating means comprises a plurality of flow-tubes formed of light-absorbing material each enclosing a respective one, except the first, of said laser crystals, for absorbing a predetermined amount of the pumping energy incident thereon.

6. A laser system according to claim 1, wherein each of said laser crystals, except the first, is wrapped with a respective coil of light-reflecting material for attenuating the light impinging upon the crystal by reflecting a predetermined amount of the pumping energy incident on the coil back into said pumping chamber.

7. A laser system according to claim 1, 2, 3, 4 5, or 6, wherein said laser crystals are laser rods having different diameters and said first rod has the largest diameter, and wherein said system further comprises:

means for optically coupling said plurality of laser rods in a chain in order of increasing diameter wherein one end of said first laser rod is optically coupled to one end of a second laser rod to receive light outputted from one end of said second laser rod.