Apparatus and methods for controlling carrier envelope phase of low repetition rate pulses
US-9225137-B2 · Dec 29, 2015 · US
US9711927B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9711927-B2 |
| Application number | US-201414780361-A |
| Country | US |
| Kind code | B2 |
| Filing date | Mar 27, 2014 |
| Priority date | Mar 27, 2013 |
| Publication date | Jul 18, 2017 |
| Grant date | Jul 18, 2017 |
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A laser device includes an apparatus for producing amplified laser pulses, using a plurality of amplifying optical fibers, and groups the basic amplified pulses into an overall amplified pulse, as well as a target, onto which the overall amplified pulse is directed such as to generate a predetermined physical process thereon, which causes a change of state in the target. The laser device is configured to measure at least one distinctive parameter of the generated physical process; adjust at least one characteristic for adjusting the basic amplified laser pulses; and analyze a plurality of measurements for different adjustments. The device analyzes the measurements many times in loops for different laser pulse adjustment characteristics, enabling an optimization by a heuristic method. Also provided is a heuristic optimization method implemented by the laser device.
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The invention claimed is: 1. A laser device comprising: an apparatus configured to produce amplified laser pulses at a frequency higher than 100 Hz, using a plurality of amplifier optical fibers in which an initial laser pulse is distributed in order to be amplified therein, and to gather together elementary pulses amplified by said amplifier optical fibers into an overall amplified pulse, and a target on to which said overall amplified pulse is directed, to generate therein, after impact, a predetermined physical process leading to a change in state of said target, means for measuring at least one characteristic parameter of said physical process generated after impact by said overall amplified pulse on said target, means for setting at least one setting characteristic of said amplified elementary laser pulses, said at least one characteristic being predetermined as a function of the use of said amplified elementary laser pulses; means for analyzing a plurality of measurements delivered by said means for measuring, for different settings made by said means for setting, during which said apparatus, said means for measuring and said means for setting are implemented at least twice, determining an optimal setting of said setting characteristic or characteristics to obtain an optimal value of said characteristic parameter or parameters of the physical process. 2. The laser device according to claim 1 , wherein said means for setting comprise means for adjusting a phase of the amplified laser pulses in each of the amplifier fibers. 3. The laser device according to claim 1 , wherein said means for setting comprise means for adjusting power of the laser pulses amplified in each of the amplifier fibers. 4. The laser device according to claim 1 , wherein the physical process generated by the interaction of the laser pulse on the target is an emission of a particle beam. 5. The laser device according to claim 4 , wherein the physical process generated by interaction of said laser pulse on the target is an emission of a proton beam. 6. The laser device according to claim 1 , wherein said means for setting enable modifying at least one of the following characteristics of the overall laser pulse: shape of the wave front of the pulse; power of the pulse; spatial distribution of amplitude of the pulse; spectral amplitude or spread of the pulse; spatial or temporal spread of the spectral components of the pulse; spatial or temporal distribution of amplitude of the pulse; duration of the pulse. 7. The laser device according to claim 1 , wherein said apparatus enables production of laser pulses at a frequency higher than 1 kHz. 8. The laser device according to claim 1 , wherein said means for setting modify the characteristics of the overall laser pulses produced at a frequency higher than 100 Hz. 9. A method for optimizing a predetermined physical process generated on a target by a laser pulse, said method comprising: producing an amplified laser pulse, amplified at a frequency higher than 100 Hz by a plurality of amplifier optical fibers over which an initial laser pulse is distributed in order to be amplified therein, said elementary pulses amplified by said amplifier optical fibers being gathered together into an overall amplified pulse, impacting said overall amplified pulse on a target to generate therein a predetermined physical process leading to a change in state of said target; measuring at least one characteristic parameter of said physical process generated during the impact of said overall amplified pulse on said target, setting at least one setting characteristic of said amplified elementary laser pulses, said at least one characteristic being predetermined as a function of the use of said amplified elementary laser pulses; repeating said producing a pulse, impacting, measuring and setting at least twice delivering a plurality of measurements for different settings, determining an optimal setting characteristic or characteristics to obtain an optimal value of said characteristic parameter or parameters of the physical process from said plurality of measurements delivered for different settings. 10. The method according to claim 9 , wherein setting at least one setting characteristics of said amplified elementary laser pulses comprises setting a phase of the pulse passing through each amplifier optical fiber. 11. The method according to claim 9 , wherein setting at least one setting characteristics of said amplified elementary laser pulses comprises setting a power of the amplified pulse in each amplifier optical fiber. 12. The laser device according to claim 1 , wherein said means for setting enable modifying duration the overall laser pulse. 13. The method according to claim 9 , wherein said setting modifies a duration the overall laser pulse.
Systems in which incident light is modified in accordance with the properties of the material investigated (where the material investigated is optically excited causing a change in wavelength of the incident light G01N21/63) · CPC title
Parallel arrangements · CPC title
using photo-ionisation, e.g. using laser beam · CPC title
Temporal shaping, e.g. pulse compression, frequency chirping (soliton generation and propagation G02F1/3513, H01S3/063 and H01S3/108) · CPC title
Tandem amplifiers · CPC title
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