Method for amplifying an ultrashort laser pulse and method for designing an amplification system

Patent metadata

Field	Value
Publication number	US-12418154-B2
Application number	US-202217881711-A
Country	US
Kind code	B2
Filing date	Aug 5, 2022
Priority date	Feb 11, 2020
Publication date	Sep 16, 2025
Grant date	Sep 16, 2025

Abstract

A method for amplifying an ultrashort laser pulse includes: a) stretching the ultrashort laser pulse in time, b) amplifying the time-stretched laser pulse, c) compressing the amplified time-stretched laser pulse, with at least one gain phase contribution selected from a group consisting of a gain dynamics phase contribution of the laser pulse that emerges as a change in a nonlinear phase on account of gain dynamics in step b), a gain bandwidth phase contribution of the laser pulse that emerges as a change in the nonlinear phase on account of a gain bandwidth in step b), and a combination thereof, being compensated by virtue of d) an additional phase contribution being imparted on the laser pulse prior to step c) and/or e) a spectrum of the laser pulse being changed, in such a way that the at least one gain phase contribution is compensated after step c).

First claim

The invention claimed is:

1. A method for amplifying an ultrashort laser pulse, comprising the following steps:
a) stretching the ultrashort laser pulse in time and obtaining a time-stretched laser pulse;
b) amplifying the time-stretched laser pulse and obtaining an amplified time-stretched laser pulse;
c) compressing the amplified time-stretched laser pulse and obtaining an amplified ultrashort laser pulse, with
at least one gain phase contribution selected from a group consisting of a gain dynamics phase contribution of the laser pulse that emerges as a change in a nonlinear phase on account of gain dynamics in step b), a gain bandwidth phase contribution of the laser pulse that emerges as a change in the nonlinear phase on account of a gain bandwidth in step b), and a combination of the gain dynamics phase contribution and the gain bandwidth phase contribution, being compensated by virtue of
d) an additional phase contribution being imparted on the laser pulse prior to step c) and/or
e) a spectrum of the laser pulse being changed,
in such a way that the at least one gain phase contribution is compensated after step c).

2. The method as claimed in claim 1 , wherein at least one step, selected from steps d) and e),
is carried out when the ultrashort laser pulse is stretched according to step a), and/or
is carried out before the ultrashort laser pulse is stretched according to step a), and/or
is carried out after the ultrashort laser pulse has been stretched according to step a) and before the time-stretched laser pulse is amplified according to step b), and/or
is carried out when the time-stretched laser pulse is amplified according to step b).

3. The method as claimed in claim 1 , wherein step d) is carried out by virtue of a stretcher for stretching the ultrashort laser pulse being used in step a), and a suitably adapted time-of-flight profile being written into or impressed onto the stretcher on the basis of a wavelength for the ultrashort laser pulse.

4. The method as claimed in claim 3 , wherein the suitably adapted time-of-flight profile is statically written into or dynamically impressed onto the stretcher on the basis of the wavelength.

5. The method as claimed in claim 1 , wherein step e) is carried out by virtue of
a stretcher for stretching the ultrashort laser pulse being used in step a), a spectral filter being written therein or impressed thereon, and/or
the laser pulse being filtered by way of a spectral filter upstream or downstream of the stretcher, and/or
the laser pulse being guided through a fiber upstream or downstream of the stretcher, a spectral filter being written into the fiber, and/or
the laser pulse being filtered and/or spectrally shaped before or while it passes through an amplifier, in which or downstream of which self-phase modulation occurs.

6. The method as claimed in claim 1 , wherein the time-stretched laser pulse is amplified in step b) by an amplifier chain, the amplifier chain comprising a plurality of amplifiers, with step e) being carried out by virtue of the laser pulse passing through at least one amplifier of the plurality of amplifiers within the amplifier chain, the gain bandwidth of the amplifier being suitably adapted in order to at least partly compensate the at least one gain phase contribution.

7. The method as claimed in claim 6 , wherein at least one amplifier of the plurality of amplifiers is used for step e), the gain bandwidth of the amplifier being suitably adapted by virtue of the at least one amplifier having
a suitably adapted doping, and/or
a suitably adapted path length for the laser pulse within the amplifier.

8. The method as claimed in claim 1 , wherein at least 30% of the energy stored in an amplifier, by means of which the time-stretched laser pulse is amplified, is retrieved in step b).

9. The method as claimed in claim 1 , wherein a B-integral for the laser pulse is greater than 3 rad following the amplification in step b).

10. The method as claimed in claim 1 , wherein at least one property of a compressor used in step c) for compressing the amplified time-stretched laser pulse is altered in order to at least partly compensate the at least one gain phase contribution.

11. A method for designing an amplification system for amplifying an ultrashort laser pulse, the method comprising the following steps:
determining at least one gain phase contribution which is selected from a group consisting of a gain dynamics phase contribution that arises in the amplification system for an ultrashort laser pulse passing through the amplification system as a change in the nonlinear phase on account of gain dynamics of the amplification system, a gain bandwidth phase contribution that arises in the amplification system for the ultrashort laser pulse passing through the amplification system as a change in the nonlinear phase on account of a gain bandwidth of the amplification system, and a combination of the gain dynamics phase contribution and the gain bandwidth phase contribution, and
providing at least one compensation element which is configured to compensate the at least one gain phase contribution by way of the method as claimed in claim 1 .

12. The method as claimed in claim 11 , wherein the at least one gain phase contribution arising in the amplification system
is determined by phase measurement, and/or
is calculated from a spectrometric measurement, and/or
is calculated from a time measurement, and/or
is determined by simulation.

13. The method as claimed in claim 11 , wherein the compensation element is designed by virtue of
f) at least an additional phase contribution for the laser pulse and/or a spectrum of the laser pulse being set dynamically, by means of a controllable spatial light modulator and/or a controllable stretcher, with at least one measured variable being determined on the amplified ultrashort laser pulse, with
g) step f) being repeated with changes to the additional phase contribution and/or the spectrum of the laser pulse, with the at least one measured variable being optimized on the basis of the additional phase contribution for the laser pulse and/or the spectrum of the laser pulse, with
h) an optical design for the compensation element being determined by optimizing the at least one measured variable in step g).

14. The method as claimed in claim 13 , wherein the compensation element is provided by virtue of the optical design for the compensation element determined in step h) being transferred to a permanent optical structure.

15. The method as claimed in claim 11 , wherein use is made of a compensation element selected from a group consisting of a stretcher for stretching the laser pulse in time, a fiber for conducting the laser pulse, a spectral filter, a mirror, a grating, an amplifier for amplifying the laser pulse, an electro-optic modulator, a Pockels cell, an acousto-optic modulator, and a combination of at least two of the aforementioned elements.

16. The method as claimed in claim 15 , wherein the spectral filter comprises a reflection filter or a transmission filter.

17. The method as claimed in claim 15 , wherein the grating comprises a volume Bragg grating.

18. The method as claimed in claim 15 , wherein the amplifier comprises a preamplifier or main amplifier.

19. The method as claimed in claim 11 , wherein an amplifier is used as a compensation element, a gain bandwidth of which is adapted in order to at least partly compensate the at least one gain phase contribution.

20. The method as c

Assignees

• Trumpf Laser Gmbh

Inventors

• Budnicki Aleksander
• Scelle Raphael

Classifications

• H01S2301/08

  Generation of pulses with special temporal shape or frequency spectrum · CPC title

• H01S3/06758

  Tandem amplifiers · CPC title

• H01S3/0085

  Modulating the output, i.e. the laser beam is modulated outside the laser cavity · CPC title

• H01S3/06754

  Fibre amplifiers (H01S3/06708 takes precedence) · CPC title

• H01S3/0092

  Nonlinear frequency conversion, e.g. second harmonic generation [SHG] or sum- or difference-frequency generation outside the laser cavity (nonlinear frequency conversion per se G02F1/35) · CPC title