High efficiency 2 micrometer laser utilizing wing-pumped Tm.sup.3+ and a laser diode array end-pumping architecture

• US 5,689,522 A
• Filed: 10/02/1995
• Issued: 11/18/1997
• Est. Priority Date: 10/02/1995
• Status: Expired due to Term

• Current Assignee: Lawrence Livermore National Security LLC (Government of the United States of America)
• Original Assignee: Regents of the University of California (University of California)
• Inventors: Beach, Raymond J.
• Primary Examiner(s): Ullah, Akm E.
• Assistant Examiner(s): Wise, Robert E.
• Application Number:
  US08/537,371
• Time in Patent Office: 778 Days
• Field of Search: 372/75, 372/41, 372/70, 372/101, 359/710
• US Class Current: 372/75
• CPC Class Codes: H01S 3/094053 Fibre coupled pump, e.g. delivering pump light using a fibre or a fibre bundle
• CPC Class Codes: H01S 3/094057 by tapered duct or homogenized light pipe, e.g. for concentrating pump light
• CPC Class Codes: H01S 3/09415 the pumping beam being parallel to the lasing mode of the pumped medium, e.g. end-pumping
• CPC Class Codes: H01S 3/1616 thulium
• CPC Class Codes: H01S 3/164 garnet
• CPC Class Codes: H01S 5/4025 Array arrangements, e.g. constituted by discrete laser diodes or laser bar H01S5/42 takes precedence

Abstract

Wing pumping a Tm³⁺ doped, end pumped solid state laser generates 2 μm laser radiation at high average powers with high efficiency. Using laser diode arrays to end-pump the laser rod or slab in the wing of the Tm³⁺ absorption band near 785 nm results in 2-for-1 quantum efficiency in Tm³⁺ because high Tm³⁺ concentrations can be used. Wing pumping allows the thermal power generated in the rod or slab to be distributed over a large enough volume to make thermal management practical in the laser gain medium even at high average power operation. The approach is applicable to CW, Q-switched, and rep-pulsed free-laser operation.

Claims

1. An apparatus, comprising:

a laser crystal doped with Tm³⁺ ions and having an end pump face coated to transmit light within a first range of about 755 nm to about 815 nm, said laser crystal comprising an output face, wherein said end pump face is coated to reflect light at about 2 micrometers; and

means for end pumping said laser crystal at a wavelength located on the wings of its main absorption feature, wherein said main absorption feature is located at approximately 785 nm, wherein said wings are located within a second range and a third range, wherein said second range is from about 755 nm to about 775 nm and wherein said third range is from about 790 nm to about 815 nm, wherein said Tm³⁺ ions produce laser light when said laser crystal doped with Tm³⁺ ions is end pumped at said wavelength located on said wings of said main absorption feature of said laser crystal, wherein said laser crystal is operable at high average power.

2. The apparatus of claim 1, further comprising an output coupler operatively located to complete an optical cavity with said laser crystal.

3. The apparatus of claim 1, wherein said output face is coated to transmit light at about 2 micrometers.

4. The apparatus of claim 1, wherein said output face is coated to partially reflect light at about 2 micrometers.

5. The apparatus of claim 1, wherein said means for end-pumping said laser crystal comprise at least one semiconductor laser diode array.

6. The apparatus of claim 5,

wherein said at least one semiconductor laser diode array comprises microchannel coolers,

wherein said at least one semiconductor laser diode array further comprises at least one cylindrical lens configured to collect light from said at least one semiconductor laser diode array, and

wherein said apparatus further comprises a lens duct to collect light from said microlens and to deliver said light to an end of said laser crystal.

7. The apparatus of claim 6, wherein said cylindrical lens comprises:

a first optical surface; and

,

a second optical surface positioned between 50 and 1000 microns of the first surface;

said first and second surfaces being formed so that the lens is substantially diffraction limited over its numerical aperture;

said cylindrical microlens having a numerical aperture greater than 0.4.

8. The apparatus of claim 6, wherein said lens duct comprises a material which is optically transparent and can be polished;

said lensing duct including an input end, an output end, and a plurality of continuously extending flat sides interconnecting said input and output ends;

said input end being of a greater cross-section than said output end and including a coating of antireflective material; and

said plurality of sides being uncoated and preventing light from escaping by reflective waveguiding due to internal reflection of the light beam.

9. The apparatus of claim 6, wherein said lens duct comprises a block of material which is optically transparent and can be polished, said block comprising:

a curved input end having an antireflective coating thereon, and an output end, said input and output ends being connected by uncoated sides which perform a waveguide function;

said uncoated sides each defining a continuous flat surface; and

said curved input end of said block having a greater cross-section than said output end of said block.

10. The apparatus of claim 6, wherein said lens duct comprises optically transparent material which can be polished and having an input and an output end interconnected by a continuous tapering section for focusing down a beam from said at least one laser diode array onto laser crystal;

said input end being provided with an anti-reflective coating, and said tapering section being uncoated and producing reflective waveguiding by internal reflection of the beam.

11. The apparatus of claim 10, wherein said lensing duct has a curved input end face and has a length, L, defined by the formula L=α

nR/(n-1), where α

is a numerical optimization factor, n is the index of refraction of the material, and R is the radius of curvature of the curved face of said input end.

12. The apparatus of claim 1, wherein said crystal is selected from a group consisting of a rod and a slab.

13. The apparatus of claim 12, wherein said laser crystal comprises YAG.

14. The apparatus of claim 12, wherein said crystal comprises at least 2% Tm³⁺.

15. The apparatus of claim 1, wherein said laser crystal comprises a host material selected from a group consisting of Y₃ Al₅ O₁₂ (YAG), (Y,Lu)₃ Al₅ O₁₂ (LYAG) and Lu₃ Al₅ O₁₂ (LAG).

16. The apparatus of claim 15, wherein said crystal is pumped at a wavelength anywhere in the wing of the main absorption feature located at approximately 785 nm.

17. An apparatus, comprising:

a laser crystal doped with Tm³⁺ ions and having an end pump face coated to transmit light within a first range of about 755 nm to about 815 nm, said laser crystal comprising an output face, wherein said end pump face is coated to reflect light at about 2 micrometers, wherein said crystal comprises about 4% Tm³⁺ in a host material of YAG, wherein said crystal comprises an end pump face coated to transmit light at about 805 nm; and

means for end pumping said laser crystal at 805 nm.