2018
DOI: 10.1016/j.physleta.2018.04.041
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Electron dynamics in the laser and quasi-static electric and magnetic fields

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Cited by 10 publications
(12 citation statements)
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“…Ref. 41) where the laser field in the ion channel has a planar structure with superluminal phase velocity. As a result, the laser can be described by For both cases, we would start with general 3/2D Hamiltonians for arbitrarily polarized laser with superluminal phase velocity and quasi-static electric and magnetic fields but the impacts of the electric and magnetic field are discussed separately.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…Ref. 41) where the laser field in the ion channel has a planar structure with superluminal phase velocity. As a result, the laser can be described by For both cases, we would start with general 3/2D Hamiltonians for arbitrarily polarized laser with superluminal phase velocity and quasi-static electric and magnetic fields but the impacts of the electric and magnetic field are discussed separately.…”
Section: Introductionmentioning
confidence: 99%
“…Ref 41,. the electron dynamics in such system with magnetic field depending on z and directing in x can be described by the following Hamiltonian equations z…”
mentioning
confidence: 99%
“…The actual description is complicated by the fact that the ω D = ω β relationship is only satisfied on average [48,58] because of the rapid nonlinear variation of v z during one betatron period T β = 2π/ω β . The result of such relativistic nonlinearity of the laser-particle interaction is an irregular (stochastic) motion of the accelerated electrons [59] and high sensitivity of the gained energy to the spatial-temporal resolution [41].…”
Section: A Bubble Driven By a Beam Driver With Large Chargementioning
confidence: 99%
“…3: (a) Relationship between the relativistic factor and the longitudinal work performed by the laser wave at different laser-plasma parameters. Dashed line corresponds to the scaling law (18). (b) Dependence W ⊥ on W || at different R and the same laser intensity and plasma frequency: the ratio |W || /W ⊥ | increases with decrease of the channel radius.…”
Section: B Scaling Lawmentioning
confidence: 99%
“…The resonant interaction of electrons with high-intensity laser wave is complicated by the fact that the Doppler shifted frequency of the wave ω D = ω L (1 − v x /v ph ), where L is the wave frequency, v ph is its phase velocity and v x is the longitudinal particle velocity, only in average equals to the betatron fre-quency ω β = ω p / √ 2γ of the electron oscillations in the channel [17]. Strong non-linearity of the laser-particle interaction leads to an irregular (stochastic) motion of electrons in the ion channel [18] and high sensitivity of the gained energy to the initial conditions.…”
Section: Introductionmentioning
confidence: 99%