High-brightness picosecond laser system
US-2024283209-A1 · Aug 22, 2024 · US
US2016164240A1 · US · A1
| Field | Value |
|---|---|
| Publication number | US-2016164240-A1 |
| Application number | US-201414251512-A |
| Country | US |
| Kind code | A1 |
| Filing date | Apr 11, 2014 |
| Priority date | Apr 11, 2014 |
| Publication date | Jun 9, 2016 |
| Grant date | — |
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 system for generating an optical signal having a preselected waveform includes: a laser source; a first waveform generator configured to apply a first signal to the laser source to create a laser output; an intensity modulator configured to receive the laser output; a second waveform generator configured to apply a second signal to the intensity modulator, the intensity modulator being configured to generate a pre-distorted laser signal based on the second signal and the laser output.
Opening claim text (preview).
What is claimed is: 1 . A system for generating an optical signal having a pre-selected waveform, the system comprising: a laser source; a first waveform generator configured to apply a first signal to the laser source to create a laser output; an intensity modulator configured to receive the laser output; and a second waveform generator configured to apply a second signal to the intensity modulator, the intensity modulator being configured to generate a pre-distorted laser signal based on the second signal and the laser output. 2 . The system of claim 1 , further comprising an amplifier coupled to the intensity modulator and configured to amplify the pre-distorted laser signal for generating the optical signal having the pre-selected waveform. 3 . The system of claim 2 , wherein the pre-distorted laser signal compensates for distortion caused by the amplifier and frequency converter. 4 . The system of claim 2 , wherein the amplifier comprises a plurality of stages including at least one broadband laser amplifier followed by at least one narrowband laser amplifier to reduce gain clamping. 5 . The system of claim 4 , wherein the amplifier comprises an optical gate between the stages to reduce gain clamping. 6 . The system of claim 1 , further comprising a frequency converter coupled to the intensity modulator and configured to convert a frequency of the pre-distorted laser signal for generating the optical signal having the pre-selected waveform. 7 . The system of claim 1 , wherein the first waveform generator is configured to apply the first signal to the laser source through a laser source driver configured to directly modulate a current applied to the laser source. 8 . The system of claim 7 , wherein the laser source driver is configured to directly modulate the current applied to the laser source by ramping the current applied to the laser source to generate a frequency chirp in the pre-selected waveform to mitigate stimulated Brillouin scattering. 9 . The system of claim 8 , wherein ramping the current applied to the laser source operates to improve a pulse contrast ratio at an output of the intensity modulator. 10 . The system of claim 1 , wherein the second waveform generator is configured to apply the second signal to the intensity modulator through a radio frequency amplifier configured to amplify the second signal. 11 . The system of claim 10 , wherein the intensity modulator is configured to generate the pre-distorted laser signal as a product of the laser signal and the second signal. 12 . The system of claim 1 , wherein the intensity modulator is an electro-optical intensity modulator. 13 . A method of generating an optical signal having a pre-selected waveform, the method comprising: applying a first signal from a first waveform generator to a laser source to create a laser output; transmitting the laser output to an intensity modulator, applying a second signal from a second waveform generator to the intensity modulator to generate a pre-distorted laser signal based on the second signal and the laser output; and amplifying and converting a frequency of the pre-distorted laser signal to generate the optical signal having the pre-selected waveform. 14 . The method of claim 13 , wherein pre-distorted laser signal compensates for distortion caused by amplification and frequency conversion. 15 . The method of claim 13 , wherein amplifying the pre-distorted laser signal comprises transmitting the pre-distorted laser signal through a plurality of stages including at least one broadband laser amplifier followed by at least one narrowband laser amplifier to reduce gain clamping. 16 . The method of claim 15 , wherein amplifying the pre-distorted laser signal comprises transmitting the pre-distorted laser signal through an optical gate between the stages to reduce gain clamping. 17 . The method of claim 13 , further comprising directly modulating a current applied to the laser source by applying the first signal from the first waveform generator through a laser source driver to the laser source. 18 . The method of claim 13 , further comprising ramping a current applied to the laser source to create a frequency chirp in the pre-selected waveform. 19 . The method of claim 13 , further comprising applying the second signal to the intensity modulator through a radio frequency amplifier configured to amplify the second signal. 20 . The method of claim 19 , further comprising creating the laser output as a product of the laser signal and the amplified second signal.
for second-harmonic generation {(G02F1/3532 takes precedence)} · CPC title
Controlling the frequency of the radiation · CPC title
Suppression of nonlinear conversion, e.g. specific design to suppress for example stimulated brillouin scattering [SBS], mainly in optical fibres in combination with multimode pumping · CPC title
Anti-reflection devices, e.g. optical isolaters (absorbing layers for marking or protecting purposes in laser working B23K26/50; magneto-optical non-reciprocal devices G02F1/093, G02F1/0955) · CPC title
Cascaded amplifiers · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.