Nonlinear chirped pulse fiber amplifier with pulse compression

• US 8,154,793 B2
• Filed: 05/27/2008
• Issued: 04/10/2012
• Est. Priority Date: 05/25/2007
• Status: Expired due to Fees

• Current Assignee: Cornell University
• Original Assignee: Cornell University
• Inventors: Wise, Frank W., Kuznetsova, Lyuba, Chong, Chin Yu
• Primary Examiner(s): BOLDA, ERIC L
• Application Number:
  US12/127,725
• Publication Number:
  US 20090002808A1
• Time in Patent Office: 1,414 Days
• Field of Search: 359/333, 359/341.1, 359/341.5, 372/25
• US Class Current: 359/341.1
• 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 3/06725 Fibre characterized by a specific dispersion, e.g. for pulse shaping in soliton lasers or for dispersion compensating [DCF]
• CPC Class Codes: H01S 3/06754 Fibre amplifiers H01S3/06708 takes precedence
• CPC Class Codes: H01S 3/1618 ytterbium
• CPC Class Codes: H04B 10/291 in which processing or amplification is carried out without conversion of the main signal from optical form
• CPC Class Codes: H04B 10/508 Pulse generation, e.g. generation of solitons

Abstract

A chirped-pulse fiber amplification method and system operates with large nonlinear phase shifts (as large as ˜20π or more). In this regime, the pulse spectrum is modified by strong self-phase modulation and gain shaping. With large-enough nonlinear phase shift, substantial spectral broadening occurs. The amplified spectrum can therefore be much broader than the spectrum that is obtained with small nonlinear phase shifts. The broader spectrum enables the formation of a shorter pulse, and the bandwidth generated in nonlinear chirped-pulse amplification can in fact be exploited to generate shorter pulses. Ultimately, this allows the generation of pulses shorter than the gain-narrowing limit of a fiber amplifier.

Claims

1. A method for generating high power ultrashort-pulses using a chirped pulse fiber amplifier, comprising the steps of:

chirping an input pulse to be amplified by passing said pulse through a pulse stretcher, thereby creating a chirped pulse that is broadened in time;

modifying said chirped pulse by increasing the power of said pulse with a fiber amplifier to induce an amount of nonlinear phase shift in said pulse which substantiality changes a shape of a power spectrum of said pulse and is sufficient to broaden the power spectrum of said pulse beyond a gain bandwidth of the fiber amplifier; and

dechirping said pulse by passing said pulse through a pulse compressor to generate a narrowed output pulse having a duration below a gain narrowing limit of said fiber amplifier, wherein said pulse stretcher and said pulse compressor have mismatched dispersion characteristics that combine to induce an amount of third order dispersion in said pulse that is sufficient to compensate for the amount of nonlinear phase shift induced in said pulse by said fiber amplifier.

2. The method of claim 1, wherein said fiber amplifier is formed from ytterbium doped fiber and said output pulse is dechirped to a duration of less than 120 femtoseconds.

3. The method of claim 2, wherein said output pulse has a duration of less than 100 femtoseconds.

4. The method of claim 1, wherein said output pulse has a duration that is shorter than the duration of said input pulse.

5. The method of claim 1, wherein a nonlinear phase shift of 12π

or more is induced in said chirped pulse to thereby broaden the power spectrum of said chirped pulse.

7. The chirped pulse fiber amplifier system of claim 1, wherein said fiber amplifier is formed from ytterbium doped fiber and said output pulse is dechirped to a duration of less than 120 femtoseconds.

8. The chirped pulse fiber amplifier system of claim 7, wherein said output pulse has a duration of less than 100 femtoseconds.

6. A chirped pulse fiber amplifier system for generating high power ultrashort-pulses comprising:

a pulse stretcher for chirping an input pulse to be compressed, thereby creating a chirped pulse that is broadened in time;

a fiber amplifier for modifying said chirped pulse by increasing the power of said pulse, said amplifier having a gain that is selected to induce an amount of nonlinear phase shift in said pulse which substantiality changes a shape of a power spectrum of said pulse and is sufficient to broaden the power spectrum of said pulse beyond a gain bandwidth of the fiber amplifier; and

a compressor for dechirping said pulse to generate a narrowed output pulse having a duration below a gain narrowing limit of said fiber amplifier;

wherein said pulse stretcher and said pulse compressor have mismatched dispersion characteristics that combine to induce an amount of third order dispersion in said pulse that is sufficient to compensate for the amount of nonlinear phase shift induced in said pulse by said fiber amplifier.

9. The chirped pulse fiber amplifier system of claim 6, wherein said output pulse has a duration that is shorter than the duration of said input pulse.

10. The chirped pulse fiber amplifier system of claim 6, wherein said fiber amplifier is selected to induce a nonlinear phase shift of 12π

or more in said chirped pulse to thereby broaden the power spectrum of said chirped pulse.

11. The chirped pulse fiber amplifier system of claim 6, wherein said pulse stretcher is formed from a length of single mode fiber, said fiber amplifier is formed from a length of doped single mode fiber and said compressor is formed from a plurality of gratings.