2010
DOI: 10.1103/physrevb.82.195316
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Non-Abelian gauge fields in the gradient expansion: Generalized Boltzmann and Eilenberger equations

Abstract: We present a microscopic derivation of the generalized Boltzmann and Eilenberger equations in the presence of non-Abelian gauges for the case of a nonrelativistic disordered Fermi gas. A unified and symmetric treatment of the charge ͓U͑1͔͒ and spin ͓SU͑2͔͒ degrees of freedom is achieved. Within this framework, just as the U͑1͒ Lorentz force generates the Hall effect, so does its SU͑2͒ counterpart gives rise to the spin Hall effect. Considering elastic and spin-independent disorder we obtain diffusion equations… Show more

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Cited by 84 publications
(166 citation statements)
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“…(46) is that, under stationary conditions, S = χΩ, provided the spin Hall angle is nonzero. This implies that the spin polarization follows the total magnetic field and (for an energy-independent scattering time [43]) there can be no out-of-plane spin polarization since Ω lays in the xy plane. This is no longer the case when one considers the extrinsic SOC as will be shown in the following Section.…”
Section: The "Intrinsic" Bloch Equationsmentioning
confidence: 99%
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“…(46) is that, under stationary conditions, S = χΩ, provided the spin Hall angle is nonzero. This implies that the spin polarization follows the total magnetic field and (for an energy-independent scattering time [43]) there can be no out-of-plane spin polarization since Ω lays in the xy plane. This is no longer the case when one considers the extrinsic SOC as will be shown in the following Section.…”
Section: The "Intrinsic" Bloch Equationsmentioning
confidence: 99%
“…(1) is the SU (2) approach, where the SOC is described in terms of a spin-dependent gauge field [43]. This formalism, introduced in the context of quarkgluon kinetic theory [53,54], was recently also extended to superconducting structures with SOC [55,56].…”
Section: The Su(2) Approach For Intrinsic Socmentioning
confidence: 99%
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