IP Library Granted Patent US 10,879,667
Granted Patent B2
US 10,879,667 · App. 16/487,792 · Granted Dec 29, 2020

Laser source for emitting a group of pulses

Inventors: Ammar Hideur (Le Petit Quevilly, FR); Adil Haboucha (Saint-Etienne-du-Rouvray, FR); Arnaud Bultel (Rouen, FR); Said Idlahcen (Sotteville-lès-Rouen, FR); Thomas Godin (Le Petit Quevilly, FR)
Assignees: CENTRE NATIONAL DE LA RECHERCHE SCIENTIFIQUE; INSTITUT NATIONAL DES SCIENCES APPLIQUEES-ROUEN; UNIVERSITE DE ROUEN NORMANDIE
H01S3/10046H01S3/0057H01S3/06754H01S3/094003H01S3/094053H01S3/10015H01S3/10023H01S3/10084H01S3/2308
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Quick Facts
Patent No.
US 10,879,667
App. No.
16/487,792
Granted
Dec 29, 2020
Kind
B2
Abstract

A laser source for emitting a group of pulses, includes a primary laser source suitable for emitting at least one primary laser pulse; at least one interferometer suitable for forming, from the primary laser pulse, a plurality of secondary laser pulses, each interferometer comprising at least one delay line allowing two secondary laser pulses to be temporally separated, by a delay comprised between 50 ps and 10 ns; and a single-mode amplifying optical fiber intended to receive the secondary laser pulses, in order to form as output a group of spatially superposed pulses.

Claims (28)

1. A laser source for emitting a group of pulses, comprising: a primary laser source suitable for emitting at least one primary laser pulse,

one or more interferometers suitable for forming, from said primary laser pulse, a plurality of secondary laser pulses, each interferometer comprising at least one delay line allowing two secondary laser pulses to be temporally separated by a delay (Δt, Δt′) comprised between 50 ps and 10 ns, said one or more interferometers comprising means for spectrally and/or temporally forming at least one of the secondary laser pulses

a single-mode amplifying optical fiber intended to receive said plurality of secondary laser pulses, in order to form as output a group of spatially superposed pulses.

2. The laser source as claimed in claim 1 , wherein at least one of said interferometers comprises means for controlling the relative optical power of the secondary laser pulses.

3. The laser source as claimed in claim 1 , furthermore comprising:

a stretcher placed upstream of the single-mode amplifying optical fiber such that the primary laser pulse is stretched to a pulse duration longer than 50 ps, and

a compressor downstream of the single-mode amplifying optical fiber in order to temporally compress the pulses of the group of pulses such that the pulses of the group of pulses have a pulse duration shorter than 500 fs.

4. The laser source as claimed in claim 1 , furthermore comprising:

at least one optical preamplifier placed upstream of the amplifying optical fiber.

5. The laser source as claimed in claim 1 , comprising:

a laser diode for optically pumping the single-mode amplifying optical fiber.

6. The laser source as claimed in claim 1 , wherein the single-mode amplifying optical fiber is intended to operate in saturated-gain regime.

7. The laser source as claimed in claim 1 , wherein the path of said at least one primary laser pulse and of the secondary laser pulses between the primary laser source and the entrance of the single-mode amplifying optical fiber is all-fiber.

8. The laser source as claimed in claim 1 , wherein the primary laser source is suitable for emitting a train of primary laser pulses that are temporally separated by a delay of at least 2 μs.

9. The laser source as claimed in claim 1 , wherein said one or more interferometers comprise at least one Mach-Zehnder interferometer, the delay line being formed by one arm of the interferometer.

10. A laser-induced-breakdown-spectroscopy (LIBS) analysis system, comprising:

a laser source for emitting a group of pulses, as claimed in claim 1 ,

a collector for collecting a beam resulting from the interaction between an object to be analyzed and the group of pulses emitted by the laser source; and

a spectrometer that allows, on the basis of the spectral analysis of the collected beam, the LIBS spectrum of the object to be analyzed to be obtained.

11. A method for generating a group of pulses, comprising the following steps:

emitting at least one primary laser pulse,

generating, from said primary pulse, a plurality of secondary laser pulses that are temporally separated by a delay comprised between 50 ps and 10 ns, by means of one or more interferometers, said generating step furthermore comprising the step of spectrally and/or temporally forming at least one of the secondary laser pulses,

injecting the secondary laser pulses into a single-mode amplifying optical fiber in order to form a group of spatially superposed pulses.

12. The method for generating a group of pulses as claimed in claim 11 , furthermore comprising the following steps:

temporally stretching the primary laser pulse such that the primary laser pulse is stretched to a pulse duration longer than 50 ps, and

temporally compressing the pulses of the group of spatially superposed pulses such that the pulses of the group of spatially superposed pulses have a pulse duration shorter than 500 fs.

13. The method for generating a group of pulses as claimed in claim 11 , furthermore comprising saturating the gain of the single-mode amplifying optical fiber.

14. The method for generating a group of pulses as claimed in claim 11 , furthermore comprising an adjustment of the delay between the secondary laser pulses.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Sep 30, 2019
From: HIDEUR, AMMAR; HABOUCHA, ADIL; BULTEL, ARNAUD; IDLAHCEN, SAID; GODIN, THOMAS
To: CENTRE NATIONAL DE LA RECHERCHE SCIENTIFIQUE; INSTITUT NATIONAL DES SCIENCES APPLIQUÉES - ROUEN; UNIVERSITÉ DE ROUEN NORMANDIE
Reel/Frame 050570/0430 →
Priority Claims (1)
FR 17 51653 · Feb 28, 2017 · national
Continuity (1)
Related Publication 20200028316A1 · Jan 23, 2020