Compact tunable x-ray source based on laser-plasma driven betatron emission
US-2020085388-A1 · Mar 19, 2020 · US
US11523489B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11523489-B2 |
| Application number | US-202117170851-A |
| Country | US |
| Kind code | B2 |
| Filing date | Feb 8, 2021 |
| Priority date | Mar 4, 2020 |
| Publication date | Dec 6, 2022 |
| Grant date | Dec 6, 2022 |
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Laser plasma optical device comprising a laser system for outputting driving light pulses and signal light pulses, a vacuum target chamber, a gas target generating device for generating gas and forming a required plasma channel target through high voltage capillary discharge ionization (or through laser picosecond pre-pulse ablation) of gas, and a focusing element. The driving light pulse is focused on the generated plasma channel target through the focusing element to generate a density-modulated plasma wake; and after a predetermined delay time T, the signal light pulse is focused onto a leading edge region of a second plasma density cavitation bubble of the plasma wake through the focusing element, so that the frequency of the signal light pulse is red-shifted to generate an ultra-intense near-single-cycle mid-infrared pulse.
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We claim: 1. A laser plasma optical device, comprising: a laser system for outputting driving light pulses and signal light pulses; a vacuum target chamber for providing a vacuum environment for interaction of laser and matter; a gas target generating device disposed in the vacuum target chamber, the gas target generating device being used for generating gas and forming a plasma channel target along a propagation direction of a driving light pulse by a laser pre-pulse irradiation or by a high-pressure ionized gas; and a focusing element disposed in the vacuum target chamber, wherein the driving light pulse is focused onto the plasma channel target by the focusing element to generate a density-modulated plasma wake; after a predetermined delay time T, the signal light pulse is focused onto a leading edge region of a second plasma density cavitation bubble of the density-modulated plasma wake through the focusing element, so that frequency of the signal light pulse is red-shifted to generate a near-single-cycle mid-infrared pulse with relativistic intensity and single-pulse energy up to multi-millijoule. 2. The laser plasma optical device of claim 1 , wherein the plasma channel target has a density rising radial density gradient distribution in a radial direction of a channel and a substantially uniform axial density distribution in an axial direction of the channel. 3. The laser plasma optical device of claim 1 , wherein the leading edge region is within most front end or a first half region of the second plasma cavitation bubble of the plasma wake. 4. The laser plasma optical device of claim 1 , wherein a beam waist radius where the driving light pulse and the signal light pulse are focused on the plasma target is 5-30 micrometers. 5. The laser plasma optical device of claim 1 , wherein the predetermined delay time T is adjusted in a range of tens of femtoseconds. 6. The laser plasma optical device of claim 1 , wherein the peak power of the driving light pulse is 1-20 terawatts. 7. The laser plasma optical device of claim 1 , wherein the peak power of the signal light pulse is 0.1-15 terawatts. 8. The laser plasma optical device of claim 1 , wherein the gas target generating device is a controllable high pressure gas nozzle device or capillary channel device. 9. The laser plasma optical device of claim 1 , wherein the mid-infrared pulse comprises one or more characteristics selected from the group consisting of (a) a peak intensity exceeding 10 17 watts/cm 2 ; (b) a pulse width being short to near a single optical cycle at the half-height full width position of the light intensity; (c) total energy up to dozens of millijoules; (d) a central wavelength up to 5 micrometer, and the maximum cut-off wavelength up to 10 micrometer; and (e) a controllable carrier phase. 10. A method for generating a near-single-cycle mid-infrared pulse with relativistic intensity and single-pulse energy up to multi-millijoule, comprising (a) providing a gas target to generate a plasma channel target through laser pre-pulse irradiation or high-pressure ionization of the gas target; (b) providing a driving light pulse to focus onto the gas target or the plasma channel target formed by the gas target in step (a) to generate a density-modulated plasma wake; and (c) after a predetermined delay time T, providing a signal light pulse to focus onto a leading edge region of a second plasma density cavitation bubble of the plasma wake in step (b) to red-shift a frequency of the signal light pulse to generate a near-single-cycle mid-infrared pulse with relativistic intensity and single-pulse energy up to multi-millijoule.
Nonlinear frequency conversion, e.g. second harmonic generation [SHG] or sum- or difference-frequency generation outside the laser cavity (nonlinear frequency conversion per se G02F1/35) · CPC title
Q-switching, i.e. in which the quality factor of the optical resonator is rapidly changed · CPC title
Modulating the output, i.e. the laser beam is modulated outside the laser cavity · CPC title
Non-linear optics · CPC title
for modulating the output, i.e. the laser beam is modulated outside the laser cavity · CPC title
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