1992
DOI: 10.1103/physreva.46.6640
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Acceleration of particles by an asymmetric Hermite-Gaussian laser beam

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Cited by 69 publications
(27 citation statements)
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“…This has become known as the Lawson-Woodward ͑LW͒ theorem. [2][3][4][5][6][7][8] The LW theorem assumes 2,3 ͑i͒ the region of interaction is infinite, ͑ii͒ the laser fields are in vacuum with no walls or boundaries present, ͑iii͒ the electron is highly relativistic (vӍc) along the acceleration path, ͑iv͒ no static electric or magnetic fields are present, and ͑v͒ nonlinear effects ͑e.g., ponderomotive, vϫB, and radiation reaction forces͒ are neglected. One or more of the assumptions of LW theorem must be violated in order to achieve a nonzero net energy gain.…”
Section: Laser Acceleration In Vacuummentioning
confidence: 99%
See 1 more Smart Citation
“…This has become known as the Lawson-Woodward ͑LW͒ theorem. [2][3][4][5][6][7][8] The LW theorem assumes 2,3 ͑i͒ the region of interaction is infinite, ͑ii͒ the laser fields are in vacuum with no walls or boundaries present, ͑iii͒ the electron is highly relativistic (vӍc) along the acceleration path, ͑iv͒ no static electric or magnetic fields are present, and ͑v͒ nonlinear effects ͑e.g., ponderomotive, vϫB, and radiation reaction forces͒ are neglected. One or more of the assumptions of LW theorem must be violated in order to achieve a nonzero net energy gain.…”
Section: Laser Acceleration In Vacuummentioning
confidence: 99%
“…[5][6][7][8] By properly choosing the electron injection point, net acceleration is possible. Consider a radiallypolarized higher-order Gaussian mode propagating along the z axis in the positive z direction, after having been reflected off a mirror located at some negative z position, as shown in Fig.…”
Section: A Acceleration Using Higher-order Gaussian Beamsmentioning
confidence: 99%
“…The basic idea of the application of the axial electric field of a focused laser beam to accelerate electrons was proposed by Scully et al (Bochove et al 1992;Scully and Zubairy 1991), i.e., when a high-power laser beam is focused, according the Maxwell equations it develops a longitudinal component large enough, which can be used to accelerate electrons along the axis in vacuum, if the electrons are injected with a high enough initial energy. Thus, the difficulties associated with the plasma can be avoided.…”
Section: Introductionmentioning
confidence: 99%
“…The simplest such laser accelerator configuration, proposed by Pantell and Piestrup [6], is a single laser beam oriented at a shallow angle to the electron beam and terminated by a downstream boundary. This initial conceptual geometry was followed by the proposal of more refined arrangements employing crossed Gaussian beam configurations [7] and eventually conceptual staged-interaction laser accelerator structures that could in principle sustain very large continuous gradients [8][9][10][11].…”
Section: Introductionmentioning
confidence: 99%