2017
DOI: 10.1103/physreva.96.043407
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Spin polarization of electrons by ultraintense lasers

Abstract: In a strong magnetic field, ultra-relativistic electrons or positrons undergo spin flip transitions as they radiate, preferentially spin polarizing in one direction -- the Sokolov-Ternov effect. Here we show that this effect could occur very rapidly (in less than 10 fs) in high intensity ($I\gtrsim10^{23}$ W/cm$^{2}$) laser-matter interactions, resulting in a high degree of electron spin polarization (70%-90%)

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Cited by 110 publications
(98 citation statements)
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“…where E and B are the electric and magnetic fields, p the momentum, γ the Lorentz factor, e the electron charge, m the electron mass and = »-a 1.16 10 e g 2 2 3 e the anomalous magnetic moment of electron [21]. The QED-based photon emission process including electron spin is correlated to the radiation spectrum of the electron for the spin-paralleled/-anti-paralleled case, similar to the Sokolov-Ternov effect [11] (see also [22]) under the locally constant field approximation (LCFA):…”
Section: Qed Spin-dependent Radiation-reaction Modelmentioning
confidence: 90%
“…where E and B are the electric and magnetic fields, p the momentum, γ the Lorentz factor, e the electron charge, m the electron mass and = »-a 1.16 10 e g 2 2 3 e the anomalous magnetic moment of electron [21]. The QED-based photon emission process including electron spin is correlated to the radiation spectrum of the electron for the spin-paralleled/-anti-paralleled case, similar to the Sokolov-Ternov effect [11] (see also [22]) under the locally constant field approximation (LCFA):…”
Section: Qed Spin-dependent Radiation-reaction Modelmentioning
confidence: 90%
“…Typically the polarization time for 17]. The S-T like effect could be significant in the strong-field QED regime and lead to certain degree of beam polarization [37,38], relying on the collision of multi-GeV electrons with a laser pulse of focal intensity >5×10 22 W cm −2 . However, in LWFA the typical relativistic factor of electrons and field strength are γ e ∼10 3 and F∼10 16 V m −1 , respectively.…”
Section: Spin Dynamics and Simulation Parametersmentioning
confidence: 99%
“…Simulations are performed with the PIC code EPOCH [39], which includes both plasma physics and nonlinear QED interactions [40,41], the latter according to [42]. Spin polarization effects [7] are neglected. Figure 1 shows 3D simulation results of HB ion acceleration in the regime where QED effects are important, at time t=6T L (where T L ≈3.33 fs is the laser period).…”
Section: Quenching Of Hb Ion Acceleration By a Self-generated Pair-plmentioning
confidence: 99%
“…Next generation lasers, such as those comprising the soon to be completed Extreme Light Infrastructure [3], could accelerate ions to GeV energies with 100% efficiency in principle [4,5]. However, at the intensities expected to be reached in these laser-matter interactions (I>10 23 W cm −2 ), the laser very rapidly ionizes the target to form a plasma in which nonlinear quantum-electrodynamic (QED) effects play a crucial role [6][7][8]. Energetic electrons radiate MeV energy gamma-ray photons by nonlinear Compton scattering.…”
Section: Introductionmentioning
confidence: 99%