2019
DOI: 10.1103/physreve.100.043202
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Polarized electron acceleration in beam-driven plasma wakefield based on density down-ramp injection

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Cited by 41 publications
(29 citation statements)
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“…Such field distributions are also seen in our simulations ( Fig.1 (a)). As already stated in previous works [27][28][29]45], the spin is preserved during steady acceleration but precesses dramatically during the injection phase. That is why we focus on the spin dynamics during injection, where typically one has γ<<1/a e [42,46] and the second term of Eq.…”
Section: Resultssupporting
confidence: 66%
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“…Such field distributions are also seen in our simulations ( Fig.1 (a)). As already stated in previous works [27][28][29]45], the spin is preserved during steady acceleration but precesses dramatically during the injection phase. That is why we focus on the spin dynamics during injection, where typically one has γ<<1/a e [42,46] and the second term of Eq.…”
Section: Resultssupporting
confidence: 66%
“…Taking <β x >~1/2, γ~1, <n(x)>~(α+1)n 0 /2 and <r>~r i /2 during the injection phase, one obtains <Ω>≈-5e<B ϕ >/4m≈-5e 2 (α+1)n 0 r i /64mε 0 , thus Δθ s~< Ω>~ΔT~-ηr i |r i | with η=5e 2 (α+1)n 0 /16mc 2 ε 0 . For simplicity, we assume a homogeneous electron distribution within the cylindrical injection volume of |r i |≤r b (x p ) [27][28][29], where r b (x p ) is the bubble radius at the density peak, satisfying r b 2 (x p )~4σ l σ r (n b0 /αn 0 ) 1/2 for PWFA [42,44] and r b 2 (x p )~4amc 2 ε 0 /αe 2 n 0 for LWFA [51]. Therefore, combining with the fact that ϕ~ϕ p , the polarization at certain ϕ p becomes…”
Section: Resultsmentioning
confidence: 99%
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“…Despite many advances mostly on the theoretical side, several principal issues need to be addressed, for example: (i) is it possible to alter the polarization of an initially unpolarized target through interaction with relativistic laser pulses [31][32][33][34][35]? or (ii) are the spins so inert during the short acceleration period that a pre-polarized target is required [13,14,[36][37][38]? Following the work by Hützen et al [39], Wen et al [13] have proposed to generate highcurrent polarized electron beams in the interaction of an ultraintense laser pulse with a pre-polarized gas plasma, which is produced through photo-dissociation by a circularly polarized ultra-violet (UV) laser pulse [40].…”
Section: Introductionmentioning
confidence: 99%
“…Simulations regarding shock-assisted injection have overwhelmingly been particle-in-cell simulations of the narrow region in which the laser interacts with the gas density transition [39][40][41][42]47 . Results can conveniently be compared to interferograms of the same field of view 27,37 .…”
Section: Introductionmentioning
confidence: 99%