Picosecond optical radiation systems and methods of use
Methods, systems and apparatus are disclosed for delivery of pulsed treatment radiation by employing a pump radiation source generating picosecond pulses at a first wavelength, and a frequency-shifting resonator having a lasing medium and resonant cavity configured to receive the picosecond pulses from the pump source at the first wavelength and to emit radiation at a second wavelength in response thereto, wherein the resonant cavity of the frequency-shifting resonator has a round trip time shorter than the duration of the picosecond pulses generated by the pump radiation source. Methods, systems and apparatus are also disclosed for providing beam uniformity and a sub-harmonic resonator.
1. An apparatus for delivery of pulsed treatment radiation comprising:
a pump radiation source generating picosecond pulses at a first wavelength, and
a wavelength-shifting resonator having a lasing medium and resonant cavity configured to receive the picosecond pulses from the pump radiation source at the first wavelength and to emit radiation at a second wavelength in response thereto,
wherein the resonant cavity of the wavelength-shifting resonator has a round trip time shorter than duration of the picosecond pulses generated by the pump radiation source, and the wavelength-shifting resonator operates without use of a modelocker or a Q-switch.
2. The apparatus of claim 1 , wherein the wavelength-shifting resonator has a round trip time at least 5 times shorter than the duration of the picosecond pulses generated by the pump radiation source.
3. The apparatus of claim 1 , wherein the wavelength-shifting resonator has a round trip time at least 10 times shorter than the duration of the picosecond pulses generated by the pump radiation source.
4. The apparatus of claim 1 , wherein the wavelength-shifting resonator has a cavity length less than 10 millimeters.
5. The apparatus of claim 1 , wherein the lasing medium of the wavelength-shifting resonator comprises a neodymium-doped crystal.
6. The apparatus of claim 5 , wherein the lasing medium of the wavelength-shifting resonator comprises a solid state crystal medium selected from the group consisting of neodymium-doped yttrium-aluminum garnet (Nd:YAG) crystals, neodymium-doped Perovskite (Nd:YAP or Nd:YAlO 3 ) crystals, neodymium-doped yttrium-lithium-fluoride (Nd:YAF) crystals, and neodymium-doped, vanadate (Nd:YVO 4 ) crystals.
7. The apparatus of claim 1 , further comprising a polarizer embedded within the resonant cavity of the wavelength-shifting resonator.
8. The apparatus of claim 1 , wherein the lasing medium of the wavelength-shifting resonator is a polarizing medium.
9. The apparatus of claim 1 , further comprising a frequency-doubling crystal.
10. The apparatus of claim 9 , wherein the frequency-doubling crystal comprises a second harmonic generating, nonlinear crystal material.
11. The apparatus of claim 9 , wherein the frequency-doubling crystal comprises one of a lithium triborate (LiB 3 O 5 ) material or a KTP material.
12. The apparatus of claim 1 , wherein the pump radiation source is a mode-locked laser.
13. The apparatus of claim 12 , wherein the mode-locked laser comprises an alexandrite laser.
14. The apparatus of claim 12 , wherein the mode-locked laser generates pulsed laser energy having at least about 100 mJ/pulse.
15. The apparatus of claim 12 , wherein the mode-locked laser generates pulsed laser energy has a pulse duration of less than 1000 picoseconds.
16. The apparatus of claim 1 , further comprising a treatment beam delivery system configured to apply a treatment beam to a patient's skin.
17. The apparatus of claim 16 , wherein the treatment beam comprises at least one of picosecond pulses from the pump radiation source at the first wavelength, picosecond pulses emitted by the wavelength-shifting resonator at the second wavelength, and picosecond pulses at a third wavelength, wherein the picosecond pulses at the third wavelength are output by a frequency-doubling crystal that receives the picosecond pulses at the second wavelength.
18. The apparatus of claim 17 , wherein the first wavelength is about 755 nm, the second wavelength is about 1064 nm, and the third wavelength is about 532 nm.
19. A method for shifting wavelength of a picosecond optical radiation pulse, the method comprising:
generating a pulse of optical radiation at a first wavelength and having a duration less than 1000 picoseconds,
pumping a wavelength-shifting resonator, operating without use of a modelocker or a Q-switch, with the pulse of optical radiation at the first wavelength, the wavelength-shifting resonator comprising a laser crystal with a high absorption coefficient at the first wavelength,
wherein a round trip time of the wavelength-shifting resonator is shorter than pumping laser pulse duration; and
extracting a pulse of radiation at a second wavelength emitted by the wavelength-shifting resonator, wherein the pulse at the second wavelength also has a duration of less than 1000 picoseconds.
20. The method of claim 19 , wherein the wavelength-shifting resonator has a round trip time at least 5 times shorter than the duration of the pumping pulse.
21. The method of claim 19 , wherein the wavelength-shifting resonator has a round trip time at least 10 times shorter than the duration of the pumping pulse.
22. The method of claim 19 , wherein the wavelength-shifting resonator has a cavity length less than 10 millimeters.
23. The method of claim 19 , wherein the laser crystal comprises a neodymium-doped crystal.
24. The method of claim 23 , wherein the laser crystal comprises a solid state crystal medium selected from the group comprising neodymium-doped yttrium-aluminum garnet (Nd:YAG) crystals, neodymium-doped pervoskite (Nd:YAP or Nd:YAlO 3 ) crystals, neodymium-doped yttrium-lithium-fluoride (Nd:YAF) crystals, and neodymium-doped vanadate (Nd:YVO 4 ) crystals.
25. The method of claim 19 , further comprising transmitting the pulse of radiation at a second wavelength through a frequency doubling crystal.
26. A method for treating tattoos or skin pigmentation disorders using a picosecond optical radiation source, the method comprising:
employing a pump radiation source to generate a pulse of optical radiation at a first wavelength, wherein the pulse has a duration of less than 1000 picoseconds,
pumping a wavelength-shifting resonator, operating without use of a modelocker or a Q-switch, with the pulse of optical radiation at the first wavelength, the wavelength-shifting resonator comprising a laser crystal with high absorption coefficient at the first wavelength,
wherein a round trip time of the wavelength-shifting resonator is shorter than the pumping laser pulse duration;
extracting a pulse of radiation at a second wavelength emitted by the wavelength-shifting resonator, wherein the pulse at the second wavelength also has a duration of less than 1000 picoseconds;
delivering the pulse of radiation at the second wavelength to a frequency-doubling crystal so as to generate a pulse of radiation at a third wavelength, wherein the pulse at the third wavelength also has a duration of less than 1000 picoseconds; and
directing the pulse at the third wavelength to a tattoo pigment or a skin pigmentation target to disrupt the target and promote clearance thereof.
27. The apparatus of claim 1 , further comprising controlling a temperature of the wavelength-shifting resonator.
28. The method of claim 19 wherein the duration of each pulse is greater than 1 picosecond.
29. The method of claim 26 wherein the duration of each pulse is greater than 1 picosecond.