Inexpensive variable rep-rate source for high-energy, ultrafast lasers
System for converting relatively long pulses from rep-rate variable ultrafast optical sources to shorter, high-energy pulses suitable for sources in high-energy ultrafast lasers. Fibers with positive group velocity dispersion (GVD) and self phase modulation are advantageously employed with the optical sources. These systems take advantage of the need for higher pulse energies at lower repetition rates so that such sources can be cost effective.
1. A combination comprising:
a pulse source outputting pulses having a pulse width between 1 picosecond and approximately 10 nanoseconds in duration at a repetition rate in a range of from 1 kHz to less than 10 MHz;
an amplifier directly receiving an unstretched output of said pulse source; and
a fiber with net positive group-velocity dispersion (GVD) and self phase modulation receiving an output of said amplifier and spectrally broadening said pulses.
2. A combination comprising:
a pulse source outputting pulses having a pulse width between 1 picosecond and approximately 10 nanoseconds in duration at a variable repetition rate in a range of from 1 kHz to less than 10 MHz; and
a fiber amplifier which includes at least one fiber with net positive group-velocity dispersion (GVD) and self phase modulation receiving an unstretched output of said pulse source and spectrally broadening said pulses.
3. A combination comprising:
a pulse source outputting pulses having a pulse width between 1 picosecond and approximately 10 nanoseconds in duration at a variable repetition rate in a range of from 1 kHz to less than 10 MHz; and
a fiber amplifier with net positive group-velocity dispersion (GVD) and self phase modulation receiving said pulses directly, as output by said pulse source, said fiber amplifier amplifying and spectrally broadening said pulses.
4. A combination comprising:
a pulse source outputting pulses having a pulse width between 1 picosecond and approximately 10 nanoseconds in duration at a variable repetition rate in a range of from 1 kHz to less than 10 MHz; and
a fiber with net positive group-velocity dispersion (GVD) and self phase modulation receiving an unstretched output of said pulse source and spectrally broadening said pulses,
wherein said fiber is arranged in a double pass configuration.
5. A system comprising:
a pulse source outputting pulses havina a pulse width between 1 picosecond and approximately 10 nanoseconds in duration at a repetition rate in a range of from 1 kHz to less than 10 MHz, said pulse source comprising a light source; and
a net positive group-velocity dispersion (GVD) fiber receiveng an unstretched output of said light source, and causing spectral generation by self phase modulation in said fiber.
6. A system comprising:
a pulse source outputting pulses, said pulse source comprising a light source;
a net positive group-velocity dispersion (GVD) fiber receiving an unstretched output of said light source, and causing spectral generation by self phase modulation in said fiber; and
an amplifier receiving an output of said positive GVD fiber, said amplifier being a parabolic amplifier.
7. The combination as claimed in claim 1 , wherein said source includes a laser diode.
8. The combination as claimed in claim 1 , wherein said source is internally modulated.
9. The combination as claimed in claim 1 , further comprising means for removing a pedestal from pulses output from said fiber with positive GVD.
10. The combination as claimed in claim 7 , wherein a pulse shape output from said diode is sufficiently parabolic for amplification in a parabolic pulse amplifier.
11. The combination as claimed in claim 2 , wherein said fiber is a multimode fiber in single mode operation for self phase modulation, and pulse energy is greater than 500 nJ.
12. The combination as claimed in claim 2 , wherein said fiber is a single mode fiber having a length of approximately 2 meters for a compression ratio of approximately 50.
13. The combination as claimed in claim 1 , wherein said amplifier is one of a multimode fiber and a holey fiber amplifier.
14. The combination as claimed in claim 2 , wherein pulse energies are greater than 1 μJ, said fiber is a multimode fiber, and said pulses are stretched.
15. A high power nonlinear fiber amplification system comprising: a seed source producing pulses with a pulse width shorter than 1 ns and longer than 1 ps, a nonlinear fiber amplifier, said amplifier being configured to spectrally broaden said seed pulses in the presence of positive dispersion, gain, and self-phase modulation, and to generate substantially linearly chirped pulses with a spectral bandwidth up to approximately 50 times larger than a spectral bandwidth of said seed pulses and wherein the chirp is substantially generated during or after the amplification process.
16. A high power nonlinear fiber amplification system according to claim 15 , further comprising a pulse compressor following said nonlinear amplifier recompressing the pulses to substantially shorter duration than the seed source pulses.
17. The combination according to claim 1 , wherein said seed source comprises a modulated semiconductor laser.
18. The combination according to claim 4 , wherein said semiconductor laser is gain switched.
19. The combination according to claim 4 , wherein said semiconductor laser is externally modulated.