Method for generating ultrashort pulses

Patent metadata

Field	Value
Publication number	US-12003071-B2
Application number	US-201917048921-A
Country	US
Kind code	B2
Filing date	Apr 19, 2019
Priority date	Apr 20, 2018
Publication date	Jun 4, 2024
Grant date	Jun 4, 2024

Abstract

A method for generating ultrashort pulses includes directing a master beam having ultrashort pulses and at least one slave beam through an optical gate material. The intensity of the slave beam upstream of the optical gate material is lower than that of the master beam upstream of the optical gate material. The optical gate material and the pulses of the master beam are chosen to induce a Kerr effect when the master beam passes through the optical gate material, the Kerr effect producing a modulation of the phase of the slave beam in association with pulses of the master beam when the slave beam passes through the optical gate material. The modulation of the phase of the slave beam is transformed into a modulation of the amplitude thereof using a complementary optical device to generate a slave beam downstream of the optical gate material having ultrashort pulses.

First claim

The invention claimed is:

1. A method for generating ultrashort pulses, comprising:
directing a master beam having ultrashort pulses and at least one slave beam through an optical gate material, the intensity of the slave beam upstream of the optical gate material being lower than that of the master beam upstream of the optical gate material, the optical gate material and the pulses of the master beam being chosen so as to induce a Kerr effect when the master beam passes through the optical gate material, the Kerr effect producing a modulation of the phase of the slave beam in association with the pulses of the master beam when the slave beam passes through the optical gate material; and
transforming the modulation of the phase of the slave beam into a modulation of an amplitude thereof using a complementary optical device, so as to generate a slave beam downstream of the optical gate material having ultrashort pulses, so that the ultrashort pulses of the slave beam generated downstream of the optical gate material and the pulses of the master beam downstream of the optical gate material are superimposed temporally; and
using the pulses of the master beam downstream of the optical gate material as a signal beam of an Optical Parametric Chirped-Pulse Amplification (OPCPA) amplifier and using the pulses of the slave beam downstream of the optical gate material as a pump beam of the OPCPA amplifier.

2. The method as claimed in claim 1 , the slave beam upstream of the optical gate material being continuous or pulsed.

3. The method as claimed in claim 1 , the pulses of the master and slave beams upstream of the optical gate material being superimposed temporally.

4. The method as claimed in claim 1 , the master and slave beams having different central wavelengths.

5. The method as claimed in claim 1 , the master beam having a central wavelength centered on 800 nm.

6. The method as claimed in claim 1 , the slave beam having a central wavelength centered on 1064 nm.

7. The method as claimed in claim 1 , the modulation of the phase of the slave beam by the pulses of the master beam when the slave beam passes through the optical gate material being instantaneous or being performed with a delay less than or equal to 20 fs.

8. The method as claimed in claim 1 , the modulation of the phase of the slave beam by Kerr effect being accompanied by a modulation of its polarization when the slave beam passes through the optical gate material when the master and slave beams at the input of the optical gate material are polarized differently, the complementary optical device comprising means for adjusting the state of polarization of the slave beam upstream of the optical gate material and a downstream polarizer downstream of the optical gate material, crossed with the polarization of the save beam at the input of the optical gate material, to block the part of the slave beam that is not polarization-modulated.

9. The method as claimed in claim 1 , the complementary optical device comprising an interferometer configured to make at least one slave beam having passed through the optical gate material interfere with at least one other beam from the same source as the slave beam in order to produce the amplitude modulation of the slave beam.

10. The method as claimed in claim 9 , the interferometer being a Sagnac interferometer in which the slave beam is split into two beams that are propagated in opposite directions through the optical gate material and recombined after having passed through the latter.

11. The method as claimed in claim 1 , the modulation of the phase of the slave beam by Kerr effect being accompanied by a modulation of its divergence when the slave beam passes through the optical gate material in the presence of a spatial gradient of intensity of the master beam within the optical gate material, the complementary optical device comprising a spatial filter downstream of the optical gate material to block the part of the slave beam that is not divergence-modulated.

12. The method as claimed in claim 1 , wherein the slave beam, after having passed through the optical gate material, is amplified within a laser amplifier.

13. A system for generating ultrashort pulses, comprising:
a first laser source generating a master beam having ultrashort pulses;
at least one second laser source generating at least one slave beam;
an optical gate material disposed on the path of the master and slave beams, the intensity of the slave beam upstream of the optical gate material being lower than that of the master beam upstream of the optical gate material, the optical gate material and the pulses of the master beam being chosen so as to induce a Kerr effect when the master beam passes through the optical gate material, the Kerr effect producing a modulation of the phase of the slave beam in association with the pulses of the master beam when the slave beam passes through the optical gate material; and
a complementary optical device for transforming the modulation of the phase of the slave beam into a modulation of an amplitude thereof, so that the ultrashort pulses of the slave beam generated downstream of the optical gate material and the pulses of the master beam downstream of the optical gate material are superimposed temporally; and
an Optical Parametric Chirped-Pulse Amplification (OPCPA) amplifier, wherein the pulses of the master beam downstream of the optical gate material is used as a signal beam of the OPCPA amplifier and the pulses of the slave beam downstream of the optical gate material is used as a pump beam of the OPCPA amplifier.

14. The system as claimed in claim 13 , the second laser source being of SLM type.

15. The system as claimed in claim 13 , comprising optical amplification means for amplifying the slave beam downstream of the optical gate material.

16. The system as claimed in claim 13 , the modulation of the phase of the slave beam by Kerr effect being accompanied by a modulation of its polarization when the slave beam passes through the optical gate material when the master and slave beams at the input of the optical gate material are polarized differently, the complementary optical device comprising means for adjusting the state of polarization of the slave beam upstream of the optical gate material and a downstream polarizer downstream of the optical gate material, crossed with the polarization of the slave beam at the input of the optical gate material, to block the part of the slave beam that is not polarization-modulated.

17. The system as claimed in claim 13 , the complementary optical device comprising an interferometer configured to make at least one slave beam having passed through the optical gate material interfere with at least one other beam from the same source as the slave beam in order to produce the amplitude modulation of the slave beam.

18. The system as claimed in claim 17 , the complementary optical device comprising a Sagnac interferometer in which the slave beam is split into two beams that are propagated in opposite directions through the optical gate material and recombined after having passed through the latter.

19. The system as claimed in claim 13 , the modulation of the phase of the slave beam by Kerr effect being accompanied by a modulation of its divergence when the slave beam passes through the optical gate material in the presence of a spatial gradient of intensity of the master beam within the optical gate material, the complementary optical device comprising a spatial filter downstream of the optical gate mater

Assignees

• Ecole Polytech
• Centre Nat Rech Scient
• Univ Paris Saclay

Inventors

• Papadopoulos Dimitrios
• Delen Xavier
• Druon Frederic

Classifications

• H01S3/0057 Primary

  Temporal shaping, e.g. pulse compression, frequency chirping (soliton generation and propagation G02F1/3513, H01S3/063 and H01S3/108) · CPC title

• G02F1/3511

  Self-focusing or self-trapping of light; Light-induced birefringence; Induced optical Kerr-effect · CPC title

• G02F1/3515

  All-optical modulation, gating, switching, e.g. control of a light beam by another light beam (G02F1/353, G02F1/37, G02F1/39 take precedence) · CPC title

• G02F1/3519

  of Sagnac type, i.e. nonlinear optical loop mirror [NOLM] · CPC title

• G02F1/392

  Parametric amplification · CPC title