Apparatus and method for frequency conversion and mixing of laser light

• US 6,763,042 B2
• Filed: 12/14/2001
• Issued: 07/13/2004
• Est. Priority Date: 12/14/2001
• Status: Expired due to Fees

• Current Assignee: Evans & Sutherland Computer Comporation
• Original Assignee: Evans & Sutherland Computer Corp. (Elevate Entertainment, Inc.)
• Inventors: Williams, Forrest L., Tanner, Allen H., Grapov, Yuri S., Elkins, Dennis F.
• Primary Examiner(s): Ip, Paul
• Assistant Examiner(s): Rodriguez, Armando
• Application Number:
  US10/017,162
• Publication Number:
  US 20030112835A1
• Time in Patent Office: 942 Days
• Field of Search: 372/20, 372/21, 372/6, 372/22, 372/26, 372/27, 372/29.011, 372/32, 372/28
• US Class Current: 372/6
• CPC Class Codes: H01S 3/067 Fibre lasers
• CPC Class Codes: H01S 3/0816 having 4 reflectors, e.g. Z-shaped resonators
• CPC Class Codes: H01S 3/094026 for synchronously pumping, e.g. for mode locking
• CPC Class Codes: H01S 3/108 using non-linear optical devices, e.g. exhibiting Brillouin or Raman scattering mode locking using a non-linear element H01S3/1112
• CPC Class Codes: H01S 3/131 by controlling the active medium, e.g. by controlling the processes or apparatus for excitation
• CPC Class Codes: H01S 3/1317 by controlling the temperature

Abstract

A method and device for the nonlinear combination of laser light which produces a beam of uniform intensity, high spatial purity, and high conversion efficiency. The method includes emitting a laser light from a tunable distributed feedback fiber laser having both thermal and piezoelectric control elements which produces a laser light at a given frequency, wavelength, and intensity; converting the laser light in a nonlinear resonator which uses a nonlinear optical crystal for frequency conversion or mixing; and measuring the resonant frequency of the nonlinear resonator and adjusting the laser light frequency using both the thermal and piezoelectric elements of the fiber laser light source to match the resonant frequency conditions within the nonlinear resonator.

Claims

1. A device for the nonlinear combination of laser light comprising:

a) a tunable fiber laser light source which produces a first energy beam along an optical path at a given frequency, wavelength, and intensity and includes thermal and piezoelectric elements for providing variable adjustment to at least the frequency of the first energy beam;

b) a nonlinear resonator placed in the optical path of the first energy beam;

c) a nonlinear optical crystal disposed in the optical path of the first energy beam within the nonlinear resonator for converting the frequency of the first energy beam; and

d) a feedback system operatively connected to the nonlinear resonator and the thermal and piezoelectric elements of the fiber laser light source, said feedback system being configured to adjust the frequency of the laser light source to match resonant frequency conditions within the nonlinear resonator.

2. The device of claim 1, wherein the nonlinear resonator has a ring configuration and includes at least a first mirror located at a point of entry of the first energy beam to the resonator, a second, a third, and a fourth reflective mirror located within the nonlinear resonator wherein each mirror is positioned at an angle which is non-normal.

3. The device of claim 2, wherein an inside surface of the first reflective mirror is partially reflective at the wavelengths of the first energy beam and highly reflective at other wavelengths, and an inside surface of the second, third, and fourth reflective mirrors which are each highly reflective at the wavelengths of the first energy beam and highly transmissive at other wavelengths.

4. The device of claim 3, wherein an outside surface of the first reflective mirror is highly transmissive at the wavelength of the first energy beam.

5. The device of claim 1, wherein said fiber laser light source is a tunable distributed feedback laser light source.

6. The device of claim 1, wherein the feedback system further comprises a detector operatively connected to the nonlinear resonator and responsive to light within the resonator and a controller coupled to the laser light source and responsive to input from the detector for tuning the first energy beam via the thermal and piezoelectric elements.

7. The device of claim 6, further comprising a phase modulator placed in the optical path of the first energy beam after the fiber laser light source and before the nonlinear resonator, for modulating sidebands to the first energy beam and coupled to the feedback system in accordance with a Pound-Drever control scheme to adjust the frequency of the first energy beam via the controller.

8. The device of claim 7, further comprising a first polarization rotator placed in the path of the first energy beam after the tunable fiber laser light source and before the phase modulator.

9. The device of claim 1, further comprising a power amplifier operatively connected to the optical path before the nonlinear resonator, for amplifying the intensity of the first energy beam.

10. The device of claim 9, wherein the power of the converted energy beam from the nonlinear resonator is between about 25 mW and 100 W.

11. The device of claim 9, further comprising a second polarization rotator placed in the path of the first energy beam after the power amplifier and before the nonlinear resonator.

12. The device of claim 1, further comprising a temperature transducer operatively coupled to the nonlinear optical crystal, for controlling the temperature of the nonlinear optical crystal.

13. The device of claim 1, further comprising:

a) a second tunable laser light source configured to emit a second energy beam along a second optical path at a given frequency, wavelength, and intensity and which includes thermal and piezoelectric elements for providing variable adjustment to at least the frequency of the second energy beam and wherein the first and second energy beams are resonantly coupled to the nonlinear resonator for frequency mixing; and

b) wherein the thermal and piezoelectric elements of the second laser light source arc coupled to the feedback system to adjust the frequency of the second energy beam to match resonant frequency conditions within the nonlinear resonator.

14. The device of claim 13, wherein the first energy beam has a wavelength of approximately 1064 nm and the second energy beam has a wavelength of approximately 1550 nm.

15. The device of claim 13, wherein the first energy beam has a wavelength of approximately 775 nm and the second energy beam has a wavelength of approximately 1064 nm.

16. The device of claim 1, wherein the first energy beam has a wavelength between about 400 nm and 1700 nm and a power between about 50 mW and 10 W upon entering the nonlinear resonator.

17. The device of claim 16, wherein the first energy beam has a wavelength of approximately 1064 nm.

18. The device of claim 16, wherein the first energy beam has a wavelength of approximately 1310 nm.

19. The device of claim 16, wherein the first energy beam has a wavelength of approximately 980 nm.

20. The device of claim 1, wherein the nonlinear optical crystal is selected from the group consisting of potassium titanyl phosphate (KTP), potassium titanyl arsenate (KTA), lithium triborate (LBO), lithium niobate (LN), beta-barium borate (BBO), periodically-poled KTP, periodically-poled KTA, and periodically-poled LN.

21. A device for the nonlinear combination of laser light comprising:

a) a tunable fiber laser light source which produces an energy beam along an optical path at a given frequency, wavelength, and intensity and includes thermal and piezoelectric elements for providing variable adjustment to at least the frequency of the energy beam;

b) a nonlinear resonator, having four reflective mirrors, positioned along the optical path;

c) a nonlinear optical crystal disposed in the optical path of the energy beam within the nonlinear resonator;

d) a power amplifier operatively connected to the optical path before the nonlinear resonator, for amplifying the intensity of the energy beam;

e) a first polarization rotator placed in the optical path after the laser light source and before the power amplifier and a second polarization rotator placed in the optical path after the power amplifier and before the nonlinear resonator;

f) a feedback system operatively connected to the nonlinear resonator and the thermal and piezoelectric elements of the fiber laser light source using a Pound-Drever control scheme to adjust the frequency of the energy beam to match resonant frequency conditions within the nonlinear resonator, wherein the feedback system comprises a detector operatively connected to the nonlinear resonator and responsive to light within the resonator and a controller operatively coupled to the tunable fiber laser light source which is responsive to input from the detector for tuning the energy beam via the thermal and piezoelectric elements; and

g) a phase modulator placed in the optical path of the energy beam before the amplifier and after the first polarization rotator, for modulating sidebands to the energy beam and coupled to the feedback system in accordance with the Pound-Drever control scheme.

22. A method for maintaining resonant conditions within a nonlinear resonator comprising the steps of:

a) emitting a laser light from a tunable laser light source which produces the laser light at a given frequency, wavelength, and intensity, said laser light source including both thermal and piezoelectric tuning elements;

b) modifying a physical parameter of the laser light in a nonlinear resonator having a nonlinear optical crystal operatively disposed therein; and

c) measuring a physical parameter of the nonlinear resonator and adjusting at least one parameter of the laser light using both the thermal and piezoelectric elements of the tunable laser light source.

23. The method of claim 22, wherein the physical parameter of the laser light source and of the nonlinear resonator is frequency.

24. The method of claim 22, further comprising the step of introducing sideband signals to the laser light using a phase modulator placed before the linear resonator and wherein the step of measuring further comprises combining the resonant frequency and reflected non-resonant signals according to a Pound-Drever feedback control scheme, so as to produce signals to the phase modulator and the thermal and piezoelectric elements for adjusting the frequency of the laser light to match the resonant frequency.