Downchirped pulse amplification

• US 7,072,101 B2
• Filed: 05/10/2003
• Issued: 07/04/2006
• Est. Priority Date: 05/10/2002
• Status: Active Grant

• Current Assignee: The Board of Regents of the University of Colorado (University of Colorado System)
• Original Assignee: The Board of Regents of the University of Colorado (University of Colorado System)
• Inventors: Backus, Sterling J., Kapteyn, Henry C.
• Primary Examiner(s): Hughes, Deandra M.
• Application Number:
  US10/436,579
• Publication Number:
  US 20040000942A1
• Time in Patent Office: 1,151 Days
• Field of Search: 359/337.5
• US Class Current: 359/337.5
• CPC Class Codes: H01S 3/0057 Temporal shaping, e.g. pulse compression, frequency chirping soliton generation and propagation G02F1/3513, H01S3/063 and H01S3/108
• CPC Class Codes: H01S 3/2308 Amplifier arrangements, e.g. MOPA

Abstract

An ultrashort pulse amplifier produces high-power ultrafast laser pulses. Pulses first have net negative (i.e. blue to red) chirp applied, and are then amplified in a laser amplifier. After amplification, the pulses are compressed using propagation through a block of material or other convenient optical system with a positive sign of chromatic dispersion. High-order dispersion correction may also be included.

Claims

1. A pulse amplifier for generating high-power ultra-short pulses from moderate-power ultra-short pulses comprising:

a subsystem configured for applying negative group velocity dispersion to the moderate-power ultra-short pulses to generate moderate power, longer-duration pulses having negative chirp;

an amplifier configured for amplifying the moderate power, long pulses to generate high power long pulses; and

a compressor configured for de-chirping the moderate power, long pulses by applying positive group velocity dispersion to generate ultra-short, high power pulses;

wherein the negative dispersion subsystem is configured to apply sufficient negative dispersion to result in pulses having negative chirp after the amplifier amplifies the pulse; and

wherein the negative dispersion subsystem is configured to result in sufficient pulse stretching to avoid nonlinear distortion within the amplifier or damage to the amplifier.

2. The pulse amplifier of claim 1, further comprising high-order dispersion correction apparatus.

3. The pulse amplifier of claim 1, wherein the amplifier comprises one of either a free-space, multi-pass amplifier, a single pass amplifier, or a regenerative amplifier.

4. The pulse amplifier of claim 3, wherein the amplifier comprises a free-space, multi-pass ti:

sapphire amplifier.

5. The pulse amplifier of claim 3 operating in the range of wavelengths shorter than about 1.3 microns.

6. The pulse amplifier of claim 1 wherein the ultra-short pulses are about 10–

200 femtoseconds in duration and the longer-duration pulses are about 1 to 100 picoseconds in duration.

7. The pulse amplifier of claim 1, further including a beam expander after amplifier for expanding the beam diameter of the high power long pulses.

8. The pulse amplifier of claim 1, further including a spatial filter.

9. The pulse amplifier of claim 1, further including a pulse shaper.

10. The pulse amplifier of claim 1 wherein the compressor comprises a block of transparent material.

20. The pulse amplifier of claim 1 wherein the subsystem for applying negative chirp includes at least one of the following combinations:

a pair of double-pass diffraction gratings;

pair of double-pass prisms;

dispersive mirrors.

21. The pulse amplifier of claim 1, wherein the compressor comprises a bulk material that is non-resonant near the spectral region of the pulses and has positive dispersion characteristics.

22. The pulse amplifier of claim 21 wherein the compressor bulk material operates in a free space geometry.

23. The pulse amplifier of claim 1, wherein the negative chirp subsystem stretches the pulses on the order of at least 100 times.

24. The pulse amplifier of claim 1 wherein a high-power ultra-short pulse generated from a moderate-power ultra-short pulse has energy between 10⁻

7 and 10⁶ Joules and said energy is at least 5 orders of magnitude higher than energy of the moderate-power ultra-short pulse.

25. The pulse amplifier of claim 1, wherein the compressor applies positive dispersion in a free space geometry.

11. A pulse amplifying subsystem for generating high-power longer duration pulses from moderate-power ultra-short pulses comprising:

a subsystem configured for applying negative group velocity dispersion to the moderate-power ultra-short pulses to generate moderate power, longer-duration pulses having chirp; and

an amplifier configured for amplifying the moderate power, long pulses to generate high power long pulses;

wherein the negative dispersion subsystem is configured to apply sufficient negative dispersion to result in pulses with negative chirp after the amplifier amplifies the pulses; and

wherein the negative dispersion subsystem is configured to result in sufficient pulse stretching to avoid nonlinear distortion within the amplifier or damage to the amplifier.

12. The subsystem of claim 11, further including a compressor configured for de-chirping the moderate power, long pulses by applying positive group velocity dispersion to generate ultra-short, high power pulses.

13. The pulse amplifier of claim 12 wherein the compressor comprises a block of solid or liquid transparent material.

14. The pulse amplifier of claim 11, further comprising high-order dispersion correction apparatus.

26. The pulse amplifier of claim 14, wherein the compressor comprises a bulk material that is non-resonant near the spectral region of the pulses and has positive dispersion characteristics.

15. The method of generating high-power ultra-short pulses from moderate-power ultra-short pulses comprising the steps of:

applying negative group velocity dispersion to the moderate-power ultra-short pulses to generate moderate power, longer-duration pulses having negative chirp;

amplifying the moderate power, long pulses to generate high power long pulses; and

compressing and de-chirping the moderate power, long pulses by applying positive group velocity dispersion to generate ultra-short, high power pulses;

wherein the step of applying negative dispersion applies sufficient negative dispersion to result in pulses with negative chirp after the amplifier amplifies the pulses; and

wherein the step of applying negative dispersion results in sufficient pulse stretching to avoid nonlinear distortion within the amplifier or damage to the amplifier.

16. The method of claim 15, further comprising the step of correcting high-order dispersion.

17. The method of claim 15, further comprising the step of expanding the beam diameter of the high power long pulses.

18. The method of claim 15, further comprising the step of spatially filtering the pulses.

19. The method of claim 15, further comprising the step of shaping the pulses.

27. The method of claim 16 wherein the compressing step is accomplished using a bulk material that is non-resonant near the spectral region of the pulses and has positive dispersion characteristics.

28. The method of claim 27 wherein the compressing step occurs in a free space geometry.

29. The method of claim 16 wherein the step of applying negative dispersion stretches the pulse on the order of at least 100 times.

30. A pulse amplifier configured for generating high-power ultra-short pulses from moderate-power ultra-short pulses comprising:

a subsystem configured for applying negative group velocity dispersion to the moderate-power ultra-short pulses to generate moderate power, longer-duration pulses having negative chirp;

an amplifier configured for amplifying the moderate power, long pulses to generate high power long pulses; and

a compressor configured for de-chirping the moderate power, long pulses by applying positive group velocity dispersion to generate ultra-short, high power pulses;

wherein the amplifier is configured to operate in saturated gain mode; and

wherein the negative dispersion subsystem is configured to result in sufficient pulse stretching to avoid nonlinear distortion within the amplifier or damage to the amplifier.

31. The pulse amplifier of claim 30 operating in the range of wavelengths shorter than about 1.3 microns.

32. The pulse amplifier of claim 30 wherein the ultra-short pulses are about 10–

200 femtoseconds in duration and the longer-duration pulses are about 1 to 100 picoseconds in duration.

33. The pulse amplifier of claim 30, wherein the compressor comprises a bulk material that is non-resonant near the spectral region of the pulses and has positive dispersion characteristics.

34. The pulse amplifier of claim 30, wherein the compressor applies positive dispersion in a free space geometry.

35. The pulse amplifier of claim 30, wherein the negative chirp subsystem stretches the pulses on the order of at least 100 times.

36. The pulse amplifier of claim 30 wherein a high-power ultra-short pulse generated from a moderate-power ultra-short pulse has energy between 10⁻

7 and 10⁶ Joules and said energy is at least 5 orders of magnitude higher than energy of the moderate-power ultra-short pulse.