Methods and apparatus for generating RGB laser light
View Patent ↗A dual-cavity single longitudinal mode (SLM) laser oscillator generates a pulsed laser signal having a long pulsewidth, long coherence length, and good shot-to-shot energy stability. The laser oscillator has a first cavity between an output coupler and a rear mirror and a second cavity between the output coupler and an intra-cavity mirror disposed between the output coupler and rear mirror. High-loss cavity optics and a passive Q-switch achieve a very high number of round trips that reduce the number of cavity modes down to two or three. The dual cavity design further discriminates between the remaining modes and allows SLM operation. The laser oscillator and an amplifier can be used as a pump laser for a laser system that generates red, green, and blue pulses for holographic recording. A wavelength conversion stage uses optical parametric amplifier(s), doubling crystals, and sum-frequency mixers to produce RGB light from the pump pulses.
1. A dual-cavity single longitudinal mode (SLM) laser oscillator for generating a pulsed laser signal, comprising:
an output coupler;
a rear mirror forming a first cavity with the output coupler;
an intra-cavity mirror disposed between the output coupler and the rear mirror along a common axis and forming a second cavity with the output coupler;
a laser medium disposed between the output coupler and the intra-cavity mirror for generating laser light; and
a passive Q-switch disposed between the output coupler and the intra-cavity mirror, the passive Q-switch limiting a number of modes in the laser oscillator to no more than three, wherein the first and second cavities are configured to provide further mode discrimination such that the laser oscillator generates single longitudinal mode laser pulses.
2. The laser oscillator of claim 1 , wherein in laser light makes more than 1,000 passes through the laser oscillator.
3. The laser oscillator of claim 1 , wherein the output coupler is less than 30% reflective at the wavelength of the laser signal.
4. The laser oscillator of claim 1 , wherein the output coupler is less than 10% reflective at the wavelength of the laser signal.
5. The laser oscillator of claim 1 , wherein the intra-cavity mirror has a reflectivity that permits an approximately equal distribution of laser energy between the first and second cavities.
6. The laser oscillator of claim 1 , wherein the laser oscillator is not seeded.
7. A pump laser, comprising:
the laser oscillator of claim 1 ; and
an amplifier for amplifying an energy of the SLM laser pulses generated by the laser oscillator.
8. A laser system for generating red, green, and blue (RGB) laser light, comprising:
the pump laser of claim 7 ; and
a wavelength conversion stage comprising non-linear optics configured to generate red, green, and blue pulses from the pump pulses.
9. The laser system of claim 8 , wherein the wavelength conversion stage comprises:
an optical parametric amplifier seeded with laser light at a signal wavelength, the optical parametric amplifier generating signal pulses at the signal wavelength from the pump pulses; and
a sum-frequency mixer configured to generate the red pulses at a red wavelength by sum- frequency mixing the signal pulses and at least a portion of the pump pulses.
10. The laser system of claim 9 , further comprising:
a frequency-doubling stage configured to frequency double a portion of the signal pulses; and
a second sum-frequency mixer configured to generate the blue pulses at a blue wavelength by sum-frequency mixing the frequency-doubled signal pulses and at least a portion of the pump pulses.
11. The laser system of claim 9 , further comprising:
a second sum-frequency mixer configured to generated the blue pulses at a blue wavelength by sum-frequency mixing a portion of the red pulses and at least a portion of the pump pulses.
12. The laser system of claim 8 , wherein the wavelength conversion stage comprises:
an optical parametric amplifier seeded with laser light at a signal wavelength, the optical parametric amplifier generating signal pulses at the signal wavelength from the pump pulses;
a frequency-doubling stage configured to frequency double the signal pulses; and
a sum-frequency mixer configured to generate the blue pulses at a blue wavelength by sum-frequency mixing the frequency-doubled signal pulses and at least a portion of the pump pulses.
13. A method of generating a pulsed laser signal, comprising:
generating laser light from a laser medium in a dual-cavity single longitudinal mode (SLM) laser oscillator such that laser light photons propagate through a first cavity formed between an output coupler and a rear mirror and through a second cavity formed between the output coupler and an intra-cavity mirror disposed between the output coupler and the rear mirror along a common axis, the laser light encountering the laser medium and a passive Q-switch positioned between the output coupler and the intra-cavity mirror;
oscillating the laser light through the laser oscillator such that the laser light makes more than 1,000 round trip passes through the laser oscillator before issuing as an SLM pulsed laser signal from the laser oscillator.
14. The method of claim 13 , wherein the passive Q-switch limits a number of modes in the laser oscillator to no more than three, and wherein the first and second cavities further mode discrimination to achieve single longitudinal mode operation.
15. The method of claim 13 , further comprising:
operating the laser oscillator without seeding the laser oscillator with a seed signal.
16. A method of generating red, green, and blue (RGB) laser light, comprising:
using pulses of the SLM pulse laser signal generated according to claim 13 as pump pulses at a pump wavelength; and
generating red, green, and blue pulses from the pump pulses.
17. The method of claim 16 , further comprising:
generating signal pulses at a signal wavelength via optical parametric amplification of the pump pulses; and
sum-frequency mixing the signal pulses with at least a portion of the pump pulses to generate the red pulses.
18. The method of claim 17 , further comprising:
frequency doubling a portion of the signal pulses; and
sum-frequency mixing the frequency-doubled signal pulses and at least a portion of the pump pulses to generate the blue pulses.
19. The method of claim 17 , further comprising:
sum-frequency mixing a portion of the red pulses and at least a portion of the pump pulses to generate the blue pulses.
20. The method of claim 16 , further comprising:
generating signal pulses at a signal wavelength via optical parametric amplification of the pump pulses;
frequency doubling the signal pulses; and
sum-frequency mixing the frequency-doubled signal pulses and at least a portion of the pump pulses to generate the blue pulses.
21. The laser oscillator of claim 1 , wherein the intra-cavity mirror has a reflectivity between 30% and 40% at the wavelength of the laser signal.
22. The laser oscillator of claim 1 , wherein the intra-cavity mirror is movable along the common axis to cancel unwanted adjacent modes.
23. The method of claim 13 , wherein the intra-cavity mirror has a reflectivity between 30% and 40% at the wavelength of the laser signal.
24. The method of claim 13 , further comprising:
moving the intra-cavity mirror along the common axis to cancel unwanted adjacent modes.
25. The method of claim 13 , wherein the intra-cavity mirror has a reflectivity that permits an approximately equal distribution of laser energy between the first and second cavities.