Mode-locked multi-mode fiber laser pulse source
US-2016352063-A1 · Dec 1, 2016 · US
US10505335B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10505335-B2 |
| Application number | US-201615552061-A |
| Country | US |
| Kind code | B2 |
| Filing date | Mar 15, 2016 |
| Priority date | Mar 19, 2015 |
| Publication date | Dec 10, 2019 |
| Grant date | Dec 10, 2019 |
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A method and a system for pulsed excitation of a nonlinear medium for photon pair generation, he method comprising exciting a single narrow resonance of a nonlinear resonant element with a pulsed laser field, comprising embedding a nonlinear resonant element directly into an external laser cavity and locking the cavity modes.
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The invention claimed is: 1. A method for a pulsed bandwidth-matched excitation of a single narrow resonance of a nonlinear resonant element with a pulsed laser field, comprising embedding a nonlinear resonant element directly into an external laser cavity, selecting one single resonance of the nonlinear resonant element and locking external cavity resonances within the selected resonance of the nonlinear resonant element. 2. A method for a pulsed bandwidth-matched excitation of a nonlinear resonant element for the generation of photon pairs, comprising embedding a nonlinear resonant element directly into an external laser cavity, selecting one single resonance of the nonlinear resonant element and locking external cavity resonances within the selected resonance of the nonlinear resonant element, the photon pairs being generated by a spontaneous nonlinear effect in the nonlinear resonant element. 3. The method of claim 1 , comprising selecting a resonant nonlinear element among one of: a nonlinear optical guided loop, a micro-toroid resonator, a micro-sphere resonator, a nonlinear Fabry-Perot cavity, a nonlinear Ikeda cavity, and a whispering gallery mode resonator. 4. The method of claim 1 , wherein said locking the cavity modes comprises passive mode-locking the cavity modes. 5. The method of claim 1 , wherein said locking the cavity modes comprises using one of: saturable absorbers, nonlinear loop mirrors, nonlinear polarization rotation, additive pulse-mode-locking and nonlinear Kerr lenses. 6. The method of claim 1 , comprising placing the nonlinear resonant element inside a nonlinear amplifying loop mirror section of a figure-8 optical cavity and selecting a single nonlinear cavity resonance in a nonlinear amplifying loop mirror configuration. 7. The method of claim 1 , wherein said locking the cavity modes comprises active mode-locking the cavity modes. 8. The method of claim 1 , wherein said locking the cavity modes comprises using an active intensity or phase modulator and selecting a modulation amplitude at a frequency matching a free spectral range of the external cavity. 9. A system for pulsed bandwidth-matched excitation of a single narrow resonance pulsed excitation with a pulsed laser field, comprising an external laser cavity and a nonlinear resonant element, said nonlinear resonant element being directly embedded within said external laser cavity, wherein one single resonance of the nonlinear resonant element is selected and external cavity resonances are locked within the selected resonance of the nonlinear resonant element. 10. The system of claim 9 , wherein the resonant nonlinear element is one of: a nonlinear optical guided loop, a micro-toroid resonator, a micro-sphere resonator, a nonlinear Fabry-Perot cavity, a nonlinear Ikeda cavity, and a whispering gallery mode resonator. 11. The system of claim 9 , further comprising a mode-locking section. 12. The system of claim 9 , comprising one of: saturable absorbers, nonlinear loop mirrors, nonlinear polarization rotation, additive pulse-mode-locking and nonlinear Kerr lenses. 13. The system of claim 9 , comprising a modulator. 14. An intra-cavity pulsed pumped optical parametric oscillator, comprising an external laser cavity and a nonlinear resonant element, said nonlinear resonant element being directly embedded within said external laser cavity, wherein one single resonance of the nonlinear resonant element is selected and external cavity resonances are locked within the selected resonance of the nonlinear resonant element. 15. The method of claim 2 , comprising selecting a resonant nonlinear element among one of: a nonlinear optical guided loop, a micro-toroid resonator, a micro-sphere resonator, a nonlinear Fabry-Perot cavity, a nonlinear Ikeda cavity, and a whispering gallery mode resonator. 16. The method of claim 2 , wherein said locking the cavity modes comprises passive mode-locking the cavity modes. 17. The method of claim 2 , wherein said locking the cavity modes comprises using one of: saturable absorbers, nonlinear loop mirrors, nonlinear polarization rotation, additive pulse-mode-locking and nonlinear Kerr lenses. 18. The method of claim 2 , comprising placing the nonlinear resonant element inside a nonlinear amplifying loop mirror section of a figure-8 optical cavity and selecting a single nonlinear cavity resonance in a nonlinear amplifying loop mirror configuration. 19. The method of claim 2 , wherein said locking the cavity modes comprises active mode-locking the cavity modes. 20. The method of claim 2 , wherein said locking the cavity modes comprises using an active intensity or phase modulator and selecting a modulation amplitude at a frequency matching a free spectral range of the external cavity.
Passive mode locking · CPC title
Fibre amplifiers (H01S3/06708 takes precedence) · CPC title
using non-linear optical devices, e.g. exhibiting Brillouin or Raman scattering {(mode locking using a non-linear element H01S3/1112)} · CPC title
Loop resonators · CPC title
Frequency filtering · CPC title
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