Chirped pulse fiber amplifier

• US 8,107,161 B2
• Filed: 04/14/2006
• Issued: 01/31/2012
• Est. Priority Date: 04/14/2005
• Status: Active Grant

• Current Assignee: Cornell University
• Original Assignee: Cornell University
• Inventors: Wise, Frank W., Zhou, Shian, Kuznetsova, Lyuba, Chong, Chin Yu
• Primary Examiner(s): BOLDA, ERIC L
• Application Number:
  US11/911,410
• Publication Number:
  US 20090128892A1
• Time in Patent Office: 2,118 Days
• Field of Search: 372/25, 359/341.1
• 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 3/06791 Fibre ring lasers fibre laser gyrometers G01C19/72
• CPC Class Codes: H01S 3/1618 ytterbium

Abstract

A short-pulse fiber amplifier system (10) is designed so that nonlinear phase shifts and third-order dispersion are purposely introduced that compensate each other. In particular, the nonlinear phase shift accumulated in the amplifier is compensated by the third-order dispersion of the combination of a fiber stretcher (12) and a grating compressor (16). In the presence of third-order dispersion, an optimal nonlinear phase shift reduces the pulse duration, and enhances the peak power and pulse contrast compared to the pulse produced in linear propagation.

Claims

1. A fiber amplifier system, comprising:

a source of optical pulses;

a pulse stretcher connected to said source for receiving said pulses and generating a plurality of broadened optical pulses;

a fiber amplifier connected to said pulse stretcher for receiving said broadened optical pulses from said pulse stretcher and generating a plurality of amplified pulses, said fiber amplifier having a gain that is adjustable to introduce a controllable amount of nonlinear phase shift to said amplified pulses; and

,

a pulse compressor connected to said fiber amplifier for receiving said amplified pulses received from said fiber amplifier and generating a plurality of compressed amplified pulses;

wherein, said pulse stretcher and said pulse compressor are selected to have dispersion characteristics that are mismatched with one another to thereby introduce an amount of third order dispersion into the system and said gain of said fiber amplifier is selected to introduce an amount of nonlinear phase shift having a magnitude of at least π

to said amplified pulses which compensates for said amount of third order dispersion to thereby produce pulses of short duration and high peak power.

2. The system of claim 1, wherein said stretcher is a segment of optical fiber.

3. The system of claim 2, wherein said compressor is a dispersive delay line.

4. The system of claim 3, wherein said dispersive delay line comprises a pair of diffraction gratings.

5. The system of claim 1, wherein said amounts of third order dispersion and said nonlinear phase shift are selected to minimize the width of said output pulses and thereby maximize a value of peak power in said pulses.

6. The system of claim 1, wherein said system is designed such that the relationship of the magnitude of nonlinear phase shift, Φ

^NL, is related to the third order dispersion (TOD) approximately by the formula;

|TOD|=|T·

GVD−

0.14Φ

^NL·

T³| where GVD is the net group velocity dispersion of the system and T is the interval of the pulse.

7. A fiber amplifier system, comprising:

a source of optical pulses;

a pulse stretcher connected to said source for receiving said pulses and generating a plurality of broadened optical pulses;

a fiber amplifier connected to said pulse stretcher for receiving said broadened optical pulses from said pulse stretcher and generating a plurality of amplified pulses, said fiber amplifier including a first section of fiber that is doped to produce gain and a second section of single mode fiber that provides an amount of nonlinear phase shift in said system, said gain being adjustable to introduce a controllable amount of nonlinear phase shift to said amplified pulses; and

,

a pulse compressor connected to said fiber amplifier for receiving said amplified pulses received from said fiber amplifier and generating a plurality of compressed amplified pulses;

wherein, said pulse stretcher and said pulse compressor are selected to have dispersion characteristics that are mismatched with one another to thereby introduce an amount of third order dispersion into the system and said gain of said fiber amplifier is selected to introduce an amount of nonlinear phase shift to said amplified pulses which compensates for said amount of third order dispersion to thereby produce pulses of short duration and high peak power.

8. A method of compensating for nonlinear phase shifts in short-pulse fiber amplifiers, comprising:

providing a pulse fiber amplifier system including a source of optical pulses, a pulse stretcher connected to said source, a pulse fiber amplifier connected to pulse stretcher and a pulse compressor connected to said pulse fiber amplifier;

selecting said pulse stretcher and said pulse compressor to have dispersion characteristics that are mismatched to one another and thereby introduce an amount of third order dispersion into said system; and

adjusting a gain of said pulse fiber amplifier to introduce a selected amount of nonlinear phase shift having a magnitude of at least π

into said system that is sufficient to compensate for said third order dispersion to produce pulses of short duration and high peak power.

9. The method of claim 8, wherein said stretcher is selected to be a segment of optical fiber.

10. The method of claim 9, wherein said compressor is selected to be a dispersive delay line.

11. The method of claim 10, wherein said dispersive delay line is selected to be a pair of diffraction gratings.

12. The method of claim 8, wherein said amount of nonlinear phase shift introduced by said fiber amplifier is adjusted to minimize the width of said output pulses and thereby maximize a value of peak power in said pulses.

13. The method of claim 12, where said phase shift is adjusted by adjusting an amount of pump power applied to said amplifier.

14. The method of claim 8, wherein said system is designed such that the relationship of the magnitude of nonlinear phase shift, Φ

^NL, is related to the third order dispersion (TOD) approximately by the formula;

|TOD|=T·

GVD−

0.14Φ

^NL·

T³|, where GVD is the net group velocity dispersion of the system and T is the interval of the pulse.

15. A method of compensating for nonlinear phase shifts in short-pulse fiber amplifiers, comprising:

providing a pulse fiber amplifier system including a source of optical pulses, a pulse stretcher connected to said source, a pulse fiber amplifier connected to pulse stretcher and a pulse compressor connected to said pulse fiber amplifier, said fiber amplifier being selected to include a first section of fiber that is doped to produce gain and a second section of single mode fiber that introduces an amount of nonlinear phase shift in said system;

selecting said pulse stretcher and said pulse compressor to have dispersion characteristics that are mismatched to one another and thereby introduce an amount of third order dispersion into said system; and

adjusting a gain of said pulse fiber amplifier to introduce a selected amount of nonlinear phase shift into said system that is sufficient to compensate for said third order dispersion to produce pulses of short duration and high peak power.