2019
DOI: 10.3389/fphy.2019.00002
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A Simple Model for the Fields of a Chirped Laser Pulse With Application to Electron Laser Acceleration

Abstract: A simple model is introduced for the fields of a chirped laser pulse. As an application, dynamics of laser-acceleration of a single electron by the fields of a pulse, with a sin 4 envelope, is investigated. Multi-GeV energy gains from interaction with pulses of peak intensity I 0 ∼ 10 20 W/cm 2 , are reported.

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Cited by 14 publications
(4 citation statements)
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“…So polarization, magnetic field and chirp are the key characteristics for enhancing high energy gain. Different laser profile envelopes give us different electron scenario [31,[33][34]. By a comparative study between Trapezoidal Pulse Shape (TPS), Half-Sine Pulse Shape (HSPS), and Gaussian Pulse Shape (GPS) it has been shown that at high intensity the wakefield amplitude follows the pattern: TPS > GPS > HSPS but for lower intensity it will be reversed [35].…”
Section: Introductionmentioning
confidence: 99%
“…So polarization, magnetic field and chirp are the key characteristics for enhancing high energy gain. Different laser profile envelopes give us different electron scenario [31,[33][34]. By a comparative study between Trapezoidal Pulse Shape (TPS), Half-Sine Pulse Shape (HSPS), and Gaussian Pulse Shape (GPS) it has been shown that at high intensity the wakefield amplitude follows the pattern: TPS > GPS > HSPS but for lower intensity it will be reversed [35].…”
Section: Introductionmentioning
confidence: 99%
“…In recent years, with the development of high-peak intensity laser technology [1][2][3][4], the interaction between laser and film materials has become an important topic for scholars [5][6][7][8][9][10]. On the one hand, the diffraction gratings are an important pulse compression element in the high-peak power laser system [11][12][13], and its laser-induced damage threshold (LIDT) limits the laser energy output and affects the operational cost of refurbishment or replacement of the optics.…”
Section: Introductionmentioning
confidence: 99%
“…With lasers operating in the femtosecond and attosecond regimes becoming increasingly prevalent, precisely controlling the offset of the underlying electric field with respect to the envelope of the pulse, known as the carrier envelope offset phase (CEP), will continue to rise in importance. Myriads of applications including optical frequency metrology [1, 2], high harmonic generation [3,4], coherent synthesis of distributed fiber-laser arrays [5,6], and laser-based [7][8][9] and on-chip accelerators [10,11] rely on stabilizing and controlling the CEP. Achieving this stabilization and control over practically long durations is just as important if it is to be used in real-world applications.…”
Section: Introductionmentioning
confidence: 99%