Cascaded optical harmonic generation
US-2016291443-A1 · Oct 6, 2016 · US
US11435646B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11435646-B2 |
| Application number | US-202117486917-A |
| Country | US |
| Kind code | B2 |
| Filing date | Sep 28, 2021 |
| Priority date | Oct 16, 2020 |
| Publication date | Sep 6, 2022 |
| Grant date | Sep 6, 2022 |
A practical reading order for non-experts. Skip the full description unless you need deep technical detail.
What the patent document calls the invention.
A short plain-language summary of the technical disclosure.
Who owns or filed the patent and who is credited as inventor.
Filing, priority, publication, and grant dates set the timeline.
The legal scope of protection — read this for what is actually claimed.
Technology tags used to group this patent with similar filings.
Prior art links and similar publications in this corpus.
Official abstract text for this publication.
A laser device includes a light source configured to emit a laser light, a first mirror and a second mirror constituting a resonator where a laser light emitted from the light source enters, a nonlinear optical medium located between the first mirror and the second mirror, and a dispersive medium of adjustable effective optical thickness located between the nonlinear optical medium and at least one of the first mirror and the second mirror.
Opening claim text (preview).
What is claimed is: 1. A laser device comprising: a light source configured to emit a laser light; a first mirror and a second mirror constituting a resonator where the laser light emitted from the light source enters; a nonlinear optical medium located between the first mirror and the second mirror; and a dispersive medium of adjustable effective optical thickness located between the nonlinear optical medium and at least one of the first mirror and the second mirror, wherein the laser light passes through the nonlinear optical medium along different optical paths between the first mirror and the second mirror, and is output from the resonator without returning to the different optical paths. 2. The laser device according to claim 1 , wherein the laser light contains a plurality of frequency components, and the plurality of frequency components are different from one another by 10 THz or greater. 3. The laser device according to claim 2 , wherein the non-linear optical medium is a gaseous medium or a liquid medium, the laser device further comprises a container configured to house the non-linear optical medium, the container comprises a first light-transmissive part located at a first mirror side, and a second light-transmissive part located at a second mirror side, and the laser light propagates: through the first light-transmissive part, through the nonlinear optical medium, and then through the second light-transmissive part, and through the second light-transmissive part, through the nonlinear optical medium, and then through the first light-transmissive part. 4. The laser device according to claim 3 , wherein the effective optical thickness of the dispersive medium can be adjusted to satisfy a relative phase relationship between the frequency components generated in the nonlinear optical medium, including effects of dispersion caused by the first light-transmissive part and the second light-transmissive part. 5. The laser device according to claim 3 , wherein the laser light is folded N times between the first mirror and the second mirror while the laser light propagates through the nonlinear optical medium before being outputted from the resonator, and N is an integer of 1 or greater. 6. The laser device according to claim 3 , wherein at least one of the first mirror and the second mirror is positionally adjustable to adjust a distance between the first mirror and the second mirror to adjust a beam waist diameter or a Rayleigh length of the laser light propagating through the nonlinear optical medium. 7. The laser device according to claim 3 , wherein the first mirror and the second mirror are convex mirrors. 8. The laser device according to claim 3 , further comprising a first optical system configured to align a beam waist diameter and a Rayleigh length of the laser light entering into the resonator to a beam waist diameter and a Rayleigh length determined by a configuration of the resonator. 9. The laser device according to claim 8 , further comprising a second optical system configured to adjust an incident angle of the laser light entering into the resonator. 10. The laser device according to claim 2 , wherein the laser light is folded N times between the first mirror and the second mirror while the laser light propagates through the nonlinear optical medium before being outputted from the resonator, and N is an integer of 1 or greater. 11. The laser device according to claim 2 , wherein at least one of the first mirror and the second mirror is positionally adjustable to adjust a distance between the first mirror and the second mirror to adjust a beam waist diameter or a Rayleigh length of the laser light propagating through the nonlinear optical medium. 12. The laser device according to claim 2 , wherein the first mirror and the second mirror are convex mirrors. 13. The laser device according to claim 2 , further comprising a first optical system configured to align a beam waist diameter and a Rayleigh length of the laser light entering into the resonator to a beam waist diameter and a Rayleigh length determined by a configuration of the resonator. 14. The laser device according to claim 13 , further comprising a second optical system configured to adjust an incident angle of the laser light entering into the resonator. 15. The laser device according to claim 1 , wherein the laser light is folded N times between the first mirror and the second mirror while the laser light propagates through the nonlinear optical medium before being outputted from the resonator, and N is an integer of 1 or greater. 16. The laser device according to claim 1 , wherein at least one of the first mirror and the second mirror is positionally adjustable to adjust a distance between the first mirror and the second mirror to adjust a beam waist diameter or a Rayleigh length of the laser light propagating through the nonlinear optical medium. 17. The laser device according to claim 1 , wherein the first mirror and the second mirror are convex mirrors. 18. The laser device according to claim 1 , further comprising a first optical system configured to align a beam waist diameter and a Rayleigh length of the laser light entering into the resonator to a beam waist diameter and a Rayleigh length determined by a configuration of the resonator. 19. The laser device according to claim 18 , further comprising a second optical system configured to adjust an incident angle of the laser light entering into the resonator. 20. The laser device according to claim 1 , further comprising a an optical system configured to adjust an incident angle of the laser light entering into the resonator.
Structural association of optical elements, e.g. lenses, with the non-linear optical device · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.