Apparatus and method for delivery of dispersion compensated ultrashort optical pulses with high peak power

• US 5,862,287 A
• Filed: 12/13/1996
• Issued: 01/19/1999
• Est. Priority Date: 12/13/1996
• Status: Expired due to Term

• Current Assignee: IMRA America Incorporated (Aisin Corp.)
• Original Assignee: IMRA America Incorporated (Aisin Corp.)
• Inventors: Bendett, Mark P., Galvanauskas, Almantas, Harter, Donald J., Sucha, Gregg D., Stock, Michelle L.
• Primary Examiner(s): Lee, John D.
• Application Number:
  US08/763,381
• Time in Patent Office: 767 Days
• Field of Search: 385/123, 385/124, 372/22, 372/25, 372/29, 372/30, 372/6, 359/154, 359/161, 359/173, 359/326, 359/332, 359/333, 359/341
• US Class Current: 385/123
• CPC Class Codes: G02B 6/29394 Compensating wavelength dispersion G02B6/29376 takes precedence; dispersion compensated optical transmission systems H04B10/2507
• 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: H04B 10/25133 including a lumped electrical or optical dispersion compensator H04B10/2519, H04B10/2525 takes precedence
• CPC Class Codes: H04B 2210/252 after the transmission line, i.e. post-compensation
• CPC Class Codes: H04B 2210/254 before the transmission line, i.e. pre-compensation

Abstract

An apparatus and method for delivery of high peak power pulse through an optical fiber to an optical device included an ultrashort pulsed laser source which produce ultrashort optical pluses having high peak power. Prior to transmittng the optical pulses through a delivery optical fiber, the pulse width of the optical pulses is streched, forming chirped optical pulses having a lower peak power. The stretched pulse are transmitted through an optical fiber which delivers the pulse to an optical device requiring ultrashort, high peak power optical pulses. The optical fiber and/or an output unit coupled to the end of the optical fiber introduces a dispersion which compensates for the dispersion introduced by the pulsed laser source and the stretcher, and delivers a recompressed optical pulse to an optical device. The optical fiber delivery system preferably pre-compensates for the dispersion introduced by optical components within the optical device, so that the optical pulses are fully recompressed at a point of interest within the optical device, such as at a specimen of at a detector. The optical fiber delivery system may include a frequency converter either before or after the delivery optical fiber. The frequency converter allows optical pulses having frequencies other than that generated by the laser source to be delivered to the optical device in an efficient manner.

Claims

1. An apparatus for delivering ultrashort optical pulses with high peak power to an optical device, comprising:

an optical pulse source;

a pulse stretcher which receives ultrashort optical pulses having high peak power from said optical pulse source and which expands a pulse width of the optical pulses; and

an optical fiber which transmits the expanded optical pulses over a desired length, said optical fiber having a dispersion that compensates for other dispersions in the apparatus and the optical device, such that the optical pulses are fully recompressed at a desired point in the optical device.

2. The apparatus according to claim 1, wherein the pulse stretcher is one of:

a chirped optical fiber Bragg grating, a diffraction grating pair, and a prism pair.

3. The apparatus according to claim 1, wherein the optical fiber is a single-mode optical fiber.

4. The apparatus according to claim 1, wherein the optical fiber is an amplifying optical fiber.

5. The apparatus according to claim 1, wherein said optical fiber compresses the pulse width of the optical pulses transmitted therethrough to provide high peak power optical pulses to the optical device, such that the optical pulses are fully recompressed at a desired point in the optical device.

6. The apparatus according to claim 1, wherein the optical device is a a two-photon laser scanning microscope used to analyze a sample.

7. The apparatus according to claim 6, wherein the optical fiber compensates for dispersion caused by said microscope, such that the optical pulses are fully recompressed at the sample.

8. The apparatus according to claim 1, further comprising a frequency converter disposed downstream of said optical pulse source, said frequency converter converting a frequency of the optical pulses generated by said optical pulse source to a frequency required by the optical device.

9. An apparatus for delivering ultrashort optical pulses with high peak power to an optical device, comprising:

a pulse stretcher which receives ultrashort optical pulses having high peak power and which expands a pulse width of the optical pulses;

an optical fiber which transmits the expanded optical pulses over a desired length;

a pulse compressor which compresses the pulse width of the optical pulses transmitted through the optical fiber, and which introduces a dispersion that compensates for other dispersions in the apparatus and the optical device, such that the optical pulses are fully recompressed at a desired point in the optical device.

10. The apparatus according to claim 9, wherein the pulse compressor is one of:

a chirped optical fiber Bragg grating, a diffraction grating pair, and a prism pair.

11. An apparatus for delivering ultrashort optical pulses with high peak power to an optical device, comprising:

a periodically poled non-linear frequency converter which receives ultrashort optical pulses having high peak power, said periodically poled non-linear frequency converter expanding a pulse width of the optical pulses and changing a frequency of said optical pulses; and

an optical fiber which transmits the optical pulses over a desired length, said optical fiber having a dispersion that compensates for other dispersions in the apparatus affecting the optical pulses, such that the optical pulses are fully recompressed at a desired point in the optical device.

12. The apparatus according to claim 11, wherein the optical fiber is a single-mode optical fiber.

13. The apparatus according to claim 11, wherein the optical fiber is an amplifying optical fiber.

14. The apparatus according to claim 11, wherein said optical fiber compresses the pulse width of the optical pulses transmitted therethrough to provide high peak power optical pulses to the optical device, such that the optical pulses are fully recompressed at a desired point in the optical device.

15. The apparatus according to claim 11, further comprising a pulse compressor which compresses the pulse width of the optical pulses transmitted through said optical fiber, such that the optical pulses are fully recompressed at a desired point in the optical device.

16. The apparatus according to claim 15, wherein the pulse compressor is one of:

a chirped optical fiber Bragg grating, a diffraction grating pair, and a prism pair.

17. The apparatus according to claim 11, wherein the optical device is a two-photon laser scanning microscope used to analyze a sample.

18. The apparatus according to claim 17, wherein the optical fiber compensates for dispersion caused by said microscope, such that the optical pulses are fully recompressed at the sample.

19. The apparatus according to claim 11, wherein said periodically poled non-linear frequency converter is a periodically-poled lithium niobate (PPLN) crystal.

20. An apparatus for producing ultrashort optical pulses with high peak power, comprising:

a pulse stretcher which receives ultrashort optical pulses and which expands a pulse width of the optical pulses;

an amplifying medium which amplifies the optical pulses, said amplifying medium having a dispersion that compensates for other dispersions in the apparatus affecting the optical pulses; and

a pulse compressor including a periodically poled non-linear frequency converter which compresses a pulse width of said optical pulses and which changes a frequency of said optical pulses.

21. An apparatus for delivering ultrashort optical pulses with high peak power to an optical device, comprising:

an optical fiber which receives chirped optical pulses and which transmits the optical pulses over a desired length; and

a periodically poled non-linear frequency converter which receives the optical pulses from said optical fiber, said periodically poled non-linear frequency converter compressing a pulse width of the optical pulses and changing a frequency of said optical pulses,

said optical fiber having a dispersion that compensates for other dispersions in the apparatus affecting the optical pulses, such that the optical pulses are fully recompressed at a desired point in the optical device.

22. The apparatus according to claim 21, wherein the optical fiber is an amplifying optical fiber.

23. The apparatus according to claim 21, wherein the optical fiber is a single-mode optical fiber.

24. The apparatus according to claim 21, wherein said optical fiber compresses the pulse width of the optical pulses transmitted therethrough to provide high peak power optical pulses to the optical device, such that the optical pulses are fully recompressed at a desired point in the optical device.

25. The apparatus according to claim 21, wherein the optical device is a two-photon laser scanning microscope used to analyze a sample.

26. The apparatus according to claim 25, wherein the optical fiber compensates for dispersion caused by said microscope, such that the optical pulses are fully recompressed at the sample.

27. The apparatus according to claim 21, wherein said periodically poled non-linear frequency converter is a periodically-poled lithium niobate (PPLN) crystal.

28. A method for delivering ultrashort optical pulses with high peak power to an optical device, comprising the steps of:

generating ultrashort optical pulses having high peak power;

stretching a pulse width of the optical pulses;

transmitting the optical pulses over an optical fiber;

compressing the pulse width of the optical pulses transmitted through said optical fiber by compensating for dispersion, including dispersion caused by said optical device; and

delivering the optical pulses to the optical device.

29. The method according to claim 28, further comprising the step of frequency converting a frequency of the optical pulses generated in said generating step to a frequency required by the optical device.

30. The method according to claim 29, wherein the frequency converting step is performed prior to the transmitting step.

31. The method according to claim 29, wherein the frequency converting step is performed after the transmitting step.

32. An apparatus for delivering ultrashort optical pulses with high peak power to an optical device, comprising:

a pulse stretcher which receives ultrashort optical pulses having high peak power and which expands a pulse width of the optical pulses;

an optical fiber which transmits the expanded optical pulses over a desired length and which introduces a dispersion that compensates for other dispersions in the apparatus and the optical device, such that the optical pulses are fully recompressed at a desired point in the optical device.

33. An apparatus for delivering ultrashort optical pulses with high peak power to an optical device, comprising:

a source of chirped optical pulse;

a dispersion compensator for compensating the chirp of said pulses, and including at leastone jof a compressor and an optical fiber which introduces a dispersion that compensates for other dispersions in the apparatus and the optical device, such that the optical pulses are fully recompressed at a desired point in the optical device.