Laser system and method having a nonlinear crystal resonator

• US 5,394,414 A
• Filed: 05/28/1993
• Issued: 02/28/1995
• Est. Priority Date: 05/28/1993
• Status: Expired due to Fees

• Current Assignee: International Business Machines Corporation
• Original Assignee: International Business Machines Corporation
• Inventors: Risk, William P., Kozlovsky, William J.
• Primary Examiner(s): Ullah, Akm E.
• Application Number:
  US08/069,312
• Time in Patent Office: 641 Days
• Field of Search: 372/21, 372/22, 372/32, 372/27, 372/92, 372/94, 372/109
• US Class Current: 372/22
• CPC Class Codes: G02F 1/3542 Multipass arrangements, i.e. arrangements to make light pass multiple times through the same element, e.g. using an enhancement cavity
• CPC Class Codes: G02F 1/37 for second-harmonic generation G02F1/3532 takes precedence

Abstract

A laser system uses a nonlinear crystal ring resonator to produce Type II nonlinear second harmonic generated light. The reflective surfaces of the resonator are oriented to form two closed beam paths for the two fundamental frequency light beams having different orthogonal polarization. The two beam paths overlap along one segment which is parallel to an axis of the nonlinear crystal. Second harmonic generated light is produced along this segment of the beam paths.

Claims

1. A laser system comprising:

a nonlinear crystal for receiving a first and a second polarization radiation beams and producing second harmonic radiation; and

a ring resonator integral to the nonlinear crystal for resonating the first and second polarization radiation beams, the resonator having a plurality of reflecting surfaces which form a first beam path for the first polarization radiation beam and a second beam path for the second polarization radiation beam, wherein a portion of the first and second beam paths overlap along an overlap segment, the beams in the overlap segment having a direction of propagation which is parallel to a crystalographic axis of the nonlinear crystal.

2. The system of claim 1, wherein the first and second polarization radiation beams are produced by diode lasers.

3. The system of claim 1, wherein the nonlinear crystal is a type II nonlinear crystal.

4. The system of claim 1, wherein the nonlinear crystal is comprised of KTP.

5. The system of claim 1, wherein there are four reflective surfaces.

6. The system of claim 1, wherein the first and second beam paths each have four segments and the overlap occurs along one of the segments.

7. The system of claim 1, wherein the first and second beam paths are each shaped as two intersecting triangles.

8. The system of claim 1, wherein the reflective surfaces comprise a first, second, third, and fourth reflective surfaces, the first and second reflective surfaces each having reflective planes which are parallel to one another, and the third and fourth reflective surfaces each having reflective planes which are parallel to one another.

9. The system of claim 1, wherein the reflective surfaces each have reflective planes which are nonparallel to any of the planes containing two of the crystalographic axes of the nonlinear crystal.

10. The system of claim 1, wherein the crystalographic axis is the b axis.

11. A laser system comprising:

a first radiation source for producing a first radiation beam of a first polarization;

a second radiation source for producing a second radiation beam of a second polarization different from said first polarization;

a nonlinear crystal for receiving the first and second polarization radiation beams and producing second harmonic radiation; and

a ring resonator integral to the nonlinear crystal for resonating the first and second polarization radiation beams, the resonator having a plurality of reflecting surfaces which form a first beam path for the first polarization radiation beam and a second beam path for the second polarization radiation beam, wherein a portion of the first and second beam paths overlap along an overlap segment, the beams in the overlap segment having a direction of propagation which is parallel to a crystalographic axis of the nonlinear crystal.

12. The system of claim 11, wherein the first and second polarization radiation beams are produced by diode lasers.

13. The system of claim 11, wherein the nonlinear crystal is a type II nonlinear crystal.

14. The system of claim 11, wherein the nonlinear crystal is comprised of KTP.

15. The system of claim 11, wherein there are four reflective surfaces.

16. The system of claim 11, wherein the first and second beam paths each have four segments and the overlap occurs along one of the segments.

17. The system of claim 11, wherein the first and second beam paths are each shaped as two intersecting triangles.

18. The system of claim 11, wherein the reflective surfaces comprise a first, second, third, and fourth reflective surfaces, the first and second reflective surfaces each having reflective planes which are parallel to one another, and the third and fourth reflective surfaces each having reflective planes which are parallel to one another.

19. The system of claim 11, wherein the reflective surfaces each have reflective planes which are nonparallel to any of the planes containing two of the crystalographic axes of the nonlinear crystal.

20. The system of claim 11, wherein the crystalographic axis is the b axis.

21. A method for frequency conversion of radiation comprising the steps of:

generating a first radiation beam of a first polarization;

generating a second radiation beam of a second polarization different from said first polarization;

coupling the first and second polarization radiation beams to a nonlinear crystal to produce second harmonic radiation; and

resonating the first and second polarization radiation beams inside a ring resonator integral to the nonlinear crystal by reflecting the beams off of a plurality of reflecting surfaces which form a first beam path for the first polarization radiation beam and a second beam path for the second polarization radiation beam, wherein a portion of the first and second beam paths overlap along an overlap segment, the beams in the overlap segment having a direction of propagation which is parallel to a crystalographic axis of the nonlinear crystal.

22. The system of claim 21, wherein the first and second polarization radiation beams are produced by diode lasers.

23. The system of claim 21, wherein the nonlinear crystal is a type II nonlinear crystal.

24. The system of claim 21, wherein the nonlinear crystal is comprised of KTP.

25. The system of claim 21, wherein there are four reflective surfaces.

26. The system of claim 21, wherein the first and second beam paths each have four segments and the overlap occurs along one of the segments.

27. The system of claim 21, wherein the first and second beam paths are each shaped as two intersecting triangles.

28. The system of claim 21, wherein the reflective surfaces comprise a first, second, third, and fourth reflective surfaces, the first and second reflective surfaces each having reflective planes which are parallel to one another, and the third and fourth reflective surfaces each having reflective planes which are parallel to one another.

29. The system of claim 21, wherein the reflective surfaces each have reflective planes which are nonparallel to any of the planes containing two of the crystalographic axis of the nonlinear crystal.

30. The system of claim 21, wherein the crystalographic axis is the b axis.

31. A laser system comprising:

a first radiation source for producing a first radiation beam of a first polarization;

a second radiation source for producing a second radiation beam of a second polarization different from said first polarization;

a nonlinear crystal for receiving the first and second polarization radiation beams and producing second harmonic radiation;

a ring resonator integral to the nonlinear crystal for resonating the first and second polarization radiation beams, the resonator having a plurality of reflective surfaces which form a first beam path for the first polarization radiation beam and a second beam path for the second polarization radiation beam, wherein a portion of the first and second beam paths overlap along an overlap segment, the beams in the overlap segment having a direction of propagation which is parallel to a crystalographic axis of the nonlinear crystal;

a means for receiving an optical data storage medium;

an optical transmission means for directing said second harmonic radiation from the resonator to the optical data storage medium; and

an optical reception means for receiving a return second harmonic radiation beam from the medium and for providing a data signal responsive thereto.

32. The system of claim 31, further comprising:

a plurality of cartridges containing optical data storage media;

a plurality of storage means sized to receive the cartridges; and

a movement means for moving the cartridges between the storage means and the means for receiving an optical data storage medium.

33. The system of claim 31, wherein the first and second polarization radiation beams are produced by diode lasers.

34. The system of claim 31, wherein the nonlinear crystal is a type II nonlinear crystal.

35. The system of claim 31, wherein the nonlinear crystal is comprised of KTP.

36. The system of claim 31, wherein there are four reflective surfaces.

37. The system of claim 31, wherein the first and second beam paths each have four segments and the overlap occurs along one of the segments.

38. The system of claim 31, wherein the first and second beam paths are each shaped as two intersecting triangles.

39. The system of claim 31, wherein the reflective surfaces comprise a first, second, third, and fourth reflective surfaces, the first and second reflective surfaces each having reflective planes which are parallel to one another, and the third and fourth reflective surfaces each having reflective planes which are parallel to one another.

40. The system of claim 31, wherein the reflective surfaces each have reflective planes which are nonparallel to any of the planes containing two of the crystalographic axis of the nonlinear crystal.

41. The system of claim 31, wherein the crystalographic axis is the b axis.