2022
DOI: 10.1103/physrevx.12.011036
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Waveform Control of Relativistic Electron Dynamics in Laser-Plasma Acceleration

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Cited by 17 publications
(25 citation statements)
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“…where v φ is the laser phase velocity, v g the laser group velocity, c the light velocity, and λ 0 the laser central wavelength. This slippage of the CEP causes the wake (or bubble) to oscillate transversally during the propagation on the length scale L 2π , which has been shown to trigger periodic offaxis injection of electron bunches in simulations [13][14][15] and in our recent experiment [16]. Our previous work demonstrated clear variations of the experimental beam pointing in the polarization direction with the CEP, attributed to the bubble transverse oscillation injection.…”
Section: Introductionmentioning
confidence: 58%
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“…where v φ is the laser phase velocity, v g the laser group velocity, c the light velocity, and λ 0 the laser central wavelength. This slippage of the CEP causes the wake (or bubble) to oscillate transversally during the propagation on the length scale L 2π , which has been shown to trigger periodic offaxis injection of electron bunches in simulations [13][14][15] and in our recent experiment [16]. Our previous work demonstrated clear variations of the experimental beam pointing in the polarization direction with the CEP, attributed to the bubble transverse oscillation injection.…”
Section: Introductionmentioning
confidence: 58%
“…In our previous experiment [16], a slight beam charge variation depending on the CEP could be inferred, but it was dominated by higher amplitude CEP-independent charge variations during the scan. Moreover, the measured electron energy spectrum oscillated moderately with CEP, but the spectrometer geometry where the moving beam was sampled by a fixed pinhole did not allow to discriminate between an actual effect of the CEP on the spectrum, or just a difference of energy depending on the position sampled in the electron beam.…”
Section: Polarization Control In Nitrogenmentioning
confidence: 73%
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