Tunable optical parametric oscillator

• US 5,999,547 A
• Filed: 02/02/1998
• Issued: 12/07/1999
• Est. Priority Date: 02/07/1997
• Status: Expired due to Term

• Current Assignee: Universitã¤T Konstanz
• Original Assignee: Universitat Konstanz
• Inventors: Schneider, Klaus, Kramper, Patrick, Mlynek, Jurgen, Schiller, Stephan
• Primary Examiner(s): Lee, John D.
• Application Number:
  US09/017,964
• Time in Patent Office: 673 Days
• Field of Search: 372/21, 372/22, 359/326, 359/328, 359/330
• US Class Current: 372/21
• CPC Class Codes: G02F 1/3546 Active phase matching, e.g. by electro- or thermo-optic tuning
• CPC Class Codes: G02F 1/39 for parametric generation or amplification of light, infrared or ultraviolet waves

Abstract

An optical parameter oscillator system is proposed for use in a continuous wave pump laser system having a single-frequency pump source. The system comprises a single-resonance resonator having a nonlinear medium to produce a first and second parametrically generated wave in response to the pump wave from the single-frequency pump source. The system includes means for controlling the cavity length of the resonator, means for controlling the pump frequency of the pump source and means for controlling the temperature of the nonlinear medium. The system provides for a reliable singly-resonant optical parametric oscillator capable of emitting laser light with high spectral purity and frequency stability over a wide spectral range and is resistant to mode hopping.

Claims

1. An optical parametric oscillator system for use in a continuous-wave pumped laser device having a single-frequency pump source, the system comprising:

a single resonance resonator having a nonlinear medium for producing a first parametrically generated wave and a second parametrically generated wave in response to a pump wave from the single-frequency pump source, said resonator having low loss for said first parametrically generated wave and high transmission for said second parametrically generated wave; and

means for limiting temporal variations of independent parameters influencing an optical path length of said resonator and a wavevector mismatch of parametric generation to a level substantially smaller than that which would lead to a change in wave vector mismatch comparable to a difference of wavevector mismatches corresponding to frequencies of said first parametrically generated wave spaced by one free spectral range of said resonator.

2. The system of claim 1, wherein said resonator is a monolithic block.

3. The system of claim 1, wherein said nonlinear medium comprises a quasi-phasematched crystal.

4. The system of claim 1, wherein said resonator has high transmission for said pump wave and said independent parameters comprise a pump wave frequency, a temperature of said nonlinear medium, and a round-trip optical path length of said first parametrically generated wave external to said nonlinear medium.

5. The system of claim 1, wherein said resonator has high transmission for said pump wave, an electro-optic medium is disposed within said resonator, and said limiting means comprise means for applying an electric field to said medium, wherein said independent parameters comprise a pump frequency, a temperature of said nonlinear medium, said electric field, and a part of a round-trip optical path length of said first parametrically generated wave external to said nonlinear medium.

6. The system of claim 1, wherein said resonator comprises mirrors for said first and said second parametrically generated waves and said pump wave, said resonator has low loss for said pump wave, said pump wave is resonantly enhanced between said mirrors, and said limiting means comprise means for maximizing a circulating pump power through control of a pump frequency.

7. The system of claim 1, wherein said resonator comprises mirrors for said first and said second parametrically generated waves and said pump wave, said resonator has low loss for said pump wave and said pump wave is resonantly enhanced between said mirrors, wherein said limiting means comprise means for controlling an optical path length of said resonator to maximize a circulating pump power.

8. The system of claim 6, wherein a transmission of an input coupling mirror for said pump wave is optimized for maximum power conversion to one of said first and said said second parametrically generated waves.

9. The system of claim 7, wherein a transmission of an input coupling mirror for said pump wave is optimized for maximum power conversion to one of said first and said second generated waves.

10. The system of claim 1, wherein said limiting means comprise means for controlling an optical path length of said resonator, means for changing an optical path length by a controlled amount, and means for adjusting a phase mismatch of said resonator in response to a change in said optical path length to maximize a power conversion efficiency of the system.

11. The system of claim 1, further comprising a frequency-stable reference, means for comparing a frequency of one of said first and said second parametrically generated waves with said reference, and means for adjusting said frequency of one of said waves to minimize a detuning between said frequency and said reference.

12. The system of claim 11, wherein said resonator comprises mirrors having high reflectivity at a wavelength of a probe wave circulating in said resonator, and said limiting means comprise means for detection of a detuning of said probe wave from resonance and means for minimizing said detuning of said probe wave by one of controlling said frequency of said pump wave and controlling an optical path length of said resonator.

13. The system of claim 12, wherein said probe wave is generated as a second harmonic of one of said pump wave, said first and said second parametrically generated waves.

14. The system of claim 12, wherein said probe wave is obtained by selecting a part of said first wave emitted from said resonator and sending said selected part into said resonator, and further comprising means to rotate polarization of said selected part before entering said resonator.

15. The system of claim 1, wherein said resonator consists essentially of a semi-monolithic resonator comprising a quasi-phasematched multigrating medium, an external concave mirror having a mirror coating on a curved surface thereof, wherein a first end face of said multigrating medium is flat and has a mirror coating and a second end face of said medium has an anti-reflection coating, and further comprising means to translate said medium.

16. The system of claim 15, wherein said mirror coating on said first end face has different spectral reflectivity properties on different gratings.

17. The system of claim 15, wherein said anti-reflection coating has different spectral reflectivity properties on different gratings.

18. The system of claim 1, wherein said resonator consists essentially of a Brewster-angle cut resonator comprising at least one external concave mirror having a radius of curvature equal to a distance between an exit point out of a Brewster-angle surface of said nonlinear medium and a curved reflecting surface of said external concave mirror, wherein said nonlinear medium has at least one Brewster-angle surface to minimize Fresnel-reflection losses for waves having a polarization vector parallel to a plane of incidence with waves of different wavelength propagating colinearly within said nonlinear medium, further comprising means for focussing within said nonlinear medium.

19. The system of claim 18, wherein said focussing means consists essentially of a curved surface having a mirror coating.

20. The system of claim 18, wherein said focussing means consists essentially of a curved surface having total internal reflection.