IP Library Granted Patent US 12,249,802
Granted Patent B2
US 12,249,802 · App. 17/489,537 · Granted Mar 11, 2025

Laser device and method for operating laser device

Inventor: Tetsushi Takano (Yokohama, JP)
Assignee: Nichia Corporation
H01S3/08059H01S3/08013H01S3/091H01S3/0973H01S3/0816H01S3/094038
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Quick Facts
Patent No.
US 12,249,802
App. No.
17/489,537
Granted
Mar 11, 2025
Kind
B2
Abstract

A laser device includes: a traveling wave type resonator comprising a first mirror and a second mirror; and a laser medium disposed between the first mirror and the second mirror. The first mirror and the second mirror are disposed such that round-trip light that travels in round trips in the resonator has a focus inside the laser medium. The laser device is configured such that: excitation light incident on the resonator is superimposed on the round-trip light at the focus and narrowed to be thinner than the round-trip light, Z R ×α<0.5 is satisfied, where Z R is a Rayleigh length of the excitation light and α is an absorption coefficient of the laser medium with respect to the excitation light, and a round-trip Gouy phase shift of the resonator has a value excluding 2π×n/m where m is an integer of less than 15 and n is an integer of equal to or less than m.

Claims (39)

1. A laser device comprising:

a traveling wave type resonator comprising a first mirror and a second mirror; and

a laser medium disposed between the first mirror and the second mirror, wherein:

the first mirror and the second mirror are disposed such that round-trip light that travels in round trips in the resonator has a focus inside the laser medium;

the laser device is configured such that:

excitation light incident on the resonator is superimposed on the round-trip light at the focus and narrowed to be thinner than the round-trip light,

Z R ×α<0.5 is satisfied, where Z R is a Rayleigh length of the excitation light and a is an absorption coefficient of the laser medium with respect to the excitation light, and

a round-trip Gouy phase shift of the resonator has a value excluding 2π×n/m where m is an integer of less than 15 and n is an integer of equal to or less than m.

2. The laser device according to claim 1 , wherein:

L×α>1.89 is satisfied where L is an effective length of the laser medium with respect to the excitation light.

3. The laser device according to claim 1 , wherein:

the laser device comprises a temperature control mechanism configured to control a temperature of the laser medium.

4. The laser device according to claim 3 , wherein:

the temperature control mechanism includes a holder configured to hold the laser medium, and a temperature adjuster configured to adjust a temperature of the holder.

5. The laser device according to claim 3 , wherein:

the temperature control mechanism is configured to cause, by absorption of the excitation light, recovery of a multi-mode of the round-trip light that passes through the laser medium.

6. The laser device according to claim 1 , wherein:

the laser device further comprises

a seed light source configured to cause seed light to be incident on the resonator; and

a longitudinal mode adjustment circuit configured to control a resonator length of the resonator to be integer times a wavelength of the seed light.

7. The laser device according to claim 1 , wherein:

a slope efficiency of the laser device, represented by a ratio of an output light power increment with respect to an excitation light power increment, is higher in a second power region in which an excitation light power is higher than a predetermined level compared to a first power region in which the excitation light power is equal to or less than the predetermined level.

8. The laser device according to claim 7 , wherein:

the slope efficiency in the first power region is equal to or greater than 30% and less than 40%.

9. The laser device according to claim 7 , wherein:

the slope efficiency in the second power region is in a range of 45% to 60%.

10. A method for operating a laser device, the method comprising:

providing a traveling wave type resonator comprising a first mirror and a second mirror, and a laser medium between the first mirror and the second mirror, wherein the first mirror and the second mirror are disposed such that round-trip light that travels in round trips in the resonator has a focus inside the laser medium;

causing excitation light to be incident on the resonator such that the excitation light is superimposed on the round-trip light at the focus and narrowed to be thinner than the round-trip light; and

performing control such that:

a round-trip Gouy phase shift of the resonator has a value excluding 2π×n/m, where m is an integer of less than 15 and n is an integer of equal to or less than m, and

Z R ×α<0.5 is satisfied where a Rayleigh length of the excitation light is Z R and an absorption coefficient of the laser medium with respect to the excitation light is α.

11. The method for operating a laser device according to claim 10 , wherein:

the laser device operates under a condition of L×α>1.89, where L is an effective length of the laser medium with respect to the excitation light.

12. The method for operating a laser device according to claim 10 , further comprising:

condensing the excitation light by a thermal lens generated in the laser medium.

13. The method for operating a laser device according to claim 12 , further comprising:

increasing power of the excitation light, shortening a focal length of the thermal lens, and setting a round-trip Gouy phase shift of the resonator closer to 3π/2; and

further increasing the power of the excitation light, shortening the focal length of the thermal lens, and further increasing the round-trip Gouy phase shift from 3π/2.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Sep 29, 2021
From: TAKANO, TETSUSHI
To: NICHIA CORPORATION
Reel/Frame 057646/0354 →
Priority Claims (1)
JP 2020-165045 · Sep 30, 2020 · national
Continuity (1)
Related Publication 20220102931A1 · Mar 31, 2022
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