Beam shaping for ultra-small vertical cavity surface emitting laser (vcsel) arrays
US-2018301874-A1 · Oct 18, 2018 · US
US10084287B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10084287-B2 |
| Application number | US-201715783152-A |
| Country | US |
| Kind code | B2 |
| Filing date | Oct 13, 2017 |
| Priority date | Oct 14, 2016 |
| Publication date | Sep 25, 2018 |
| Grant date | Sep 25, 2018 |
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.
The mid-infrared laser system has an amplifier including at least one pump laser adapted to generate a pump laser beam and a length of fiber made of a low phonon energy glass and having at least one laser-active doped region between a first end and a second end, and a seed laser to generate a seed laser beam having a seed optical spectrum in the mid-infrared. The seed laser beam is launched into the first end to generate a mid-infrared laser beam outputted from the second end via stimulated emission upon pumping of the at least one laser-active doped region with the pump laser beam. When the power of the pump laser exceeds a spectrum modification threshold, the mid-infrared laser beam has an output optical spectrum being broadened relative to the seed optical spectrum.
Opening claim text (preview).
What is claimed is: 1. A mid-infrared laser system comprising: an amplifier including at least one pump laser adapted to generate a pump laser beam; and a length of fiber made of a low phonon energy glass and having at least one laser-active doped region between a first end and a second end; a seed laser adapted to generate a seed laser beam having a seed optical spectrum in a mid-infrared portion of an electromagnetic spectrum, the seed laser beam being launched into the first end to generate a mid-infrared laser beam outputted from the second end via stimulated emission upon pumping of the at least one laser-active doped region with the pump laser beam; and a spectrum modification threshold above which a power of the pump laser beam causes the mid-infrared laser beam to have an output optical spectrum being at least one of broadened and shifted relative to the seed optical spectrum. 2. The mid-infrared laser system of claim 1 wherein the seed laser beam has a seed wavelength equal or above 2.5 μm. 3. The mid-infrared laser system of claim 2 wherein the output optical spectrum of the mid-infrared laser beam includes at least 80% of its optical power at wavelengths longer than 3.0 μm. 4. The mid-infrared laser system of claim 1 wherein at least one of the first end and the second end of the length of fiber has an endcap, the endcap including a cylindrical waveguide having a first face serially connected to the at least one of the first end and the second end and being made of a low phonon energy glass being less permeable to OH— ions than the low phonon energy glass of the length of fiber. 5. The mid-infrared laser system of claim 4 wherein the endcap has a second face opposite to the first face, the second face being non perpendicular to a longitudinal axis of the cylindrical waveguide. 6. The mid-infrared laser system of claim 4 wherein the cylindrical waveguide is an optical fiber having at least one of no core and a core larger than a core of the length of fiber. 7. The mid-infrared laser system of claim 1 further comprising a bandwidth gain reflector at the second end of the length of fiber, the bandwidth gain reflector reflecting, away from the length of fiber, optical power at wavelengths within a gain bandwidth of the laser-active doped region. 8. The mid-infrared laser system of claim 7 wherein the bandwidth gain reflector is provided in the form of an tilted Bragg grating inscribed proximate to the second end of the length of fiber. 9. The mid-infrared laser system of claim 1 wherein the length of fiber includes an active fiber segment and a passive fiber segment serially connected to one another, the active fiber segment having the first end and the passive fiber segment having the second end. 10. The mid-infrared laser system of claim 9 wherein the active fiber segment is made of a first low phonon energy glass having a first transmittance window and the passive fiber segment is made of a second low phonon energy glass having a second transmittance window ranging at longer wavelengths than the first transmittance window of the first low phonon energy glass. 11. The mid-infrared laser system of claim 9 wherein the length of fiber includes a pump stripper for flushing out the pump laser beam away from the length of fiber, the pump stripper dividing the length of fiber into the active fiber segment and the passive fiber segment. 12. The mid-infrared laser system of claim 1 wherein the length of fiber includes a pump stripper for flushing the pump laser beam away from the length of fiber. 13. The mid-infrared laser system of claim 1 wherein the length of fiber includes at least a first active fiber segment and a second active fiber segment optically coupled to one another, the at least one pump laser including at least a first pump laser and a second pump laser optically coupled to the length of fiber and operable to simultaneously pump a respective one of the first and second active fiber segments, the first active fiber segment providing a first gain bandwidth and the second active fiber segment providing a second gain bandwidth ranging at longer wavelengths than the first gain bandwidth. 14. The mid-infrared laser system of claim 13 wherein the first active fiber segment is made of a first low phonon energy glass having a first transmittance window and the second active fiber segment is made of a second low phonon energy glass having a second transmittance window ranging at longer wavelengths than the first transmittance window of the first low phonon energy glass. 15. A mid-infrared optical amplifier for amplifying a seed laser beam in a mid-infrared portion of an electromagnetic spectrum, the mid-infrared optical amplifier comprising: at least one pump laser adapted to generate a pump laser beam; a length of fiber made of a low phonon energy glass and having at least one laser-active doped region between a first end and a second end, the seed laser beam being launchable into the first end to generate a mid-infrared laser beam outputted from the second end via stimulated emission upon pumping of the at least one laser-active doped region with the pump laser beam; and a spectrum modification threshold above which a power of the pump laser beam causes the mid-infrared laser beam to have an output optical spectrum being at least one of broadened and shifted relative to the seed optical spectrum. 16. The mid-infrared optical amplifier of claim 15 wherein at least one of the first end and the second end of the length of fiber has an endcap, the endcap including a cylindrical waveguide having a first face serially connected to the at least one of the first end and the second end and being made of a low phonon energy glass being less permeable to OH— ions than the low phonon energy glass of the length of fiber. 17. The mid-infrared optical amplifier of claim 16 wherein the endcap has a second face opposite to the first face, the second face being non perpendicular to a longitudinal axis of the cylindrical waveguide. 18. The mid-infrared optical amplifier of claim 16 wherein the cylindrical waveguide is an optical fiber having at least one of no core and a core larger than a core of the length of fiber. 19. The mid-infrared optical amplifier of claim 15 further comprising a bandwidth gain reflector at the second end of the length of fiber, the bandwidth gain reflector reflecting, away from the length of fiber, optical power at wavelengths within a gain bandwidth of the laser-active doped region. 20. The mid-infrared optical amplifier of claim 19 wherein the bandwidth gain reflector is provided in the form of a tilted Bragg grating inscribed proximate to the second end of the length of fiber. 21. The mid-infrared optical amplifier of claim 15 wherein the length of fiber includes an active fiber segment and an additional fiber segment serially connected to one another, the active fiber segment having the first end and the additional fiber segment having the second end, the active fiber segment being made of a first low phonon energy glass having a first transmittance window and the additional fiber segment being made of a second low phonon energy glass having a second transmittance window ranging at longer wavelengths than the first transmittance window of the first low phonon energy glass. 22. A method of operating a mid-infrared laser system having a seed laser adapted to generate a seed laser beam having a seed optical spectrum in a mid-infrared portion of an el
having special electric properties · CPC title
Frequency filtering · CPC title
Waveguide having a modified shape along the axis, e.g. branched, curved, tapered, voids · CPC title
Intensity modulators (intra-cavity modulators H01S5/0625) · CPC title
Tandem amplifiers · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.