TY - JOUR
T1 - Gauge field theory approach to spin transport in a 2D electron gas
AU - Berche, B.
AU - Bolívar, N.
AU - López, A.
AU - Medina, E.
PY - 2009
Y1 - 2009
N2 - We discuss the Pauli Hamiltonian including the spin-orbit interaction within an U(1) × SU(2) gauge theory interpretation, where the gauge symmetry appears to be broken. This interpretation offers new insight into the problem of spin currents in the condensed matter environment, and can be extended to Rashba and Dresselhaus spin-orbit interactions. We present a few outcomes of the present formulation: i) it automatically leads to zero spin conductivity, in contrast to predictions of Gauge symmetric treatments, ii) a topological quantization condition leading to voltage quantization follows, and iii) spin interferometers can be conceived in which, starting from an arbitrary incoming unpolarized spinor, it is always possible to construct a perfect spin filtering condition.
AB - We discuss the Pauli Hamiltonian including the spin-orbit interaction within an U(1) × SU(2) gauge theory interpretation, where the gauge symmetry appears to be broken. This interpretation offers new insight into the problem of spin currents in the condensed matter environment, and can be extended to Rashba and Dresselhaus spin-orbit interactions. We present a few outcomes of the present formulation: i) it automatically leads to zero spin conductivity, in contrast to predictions of Gauge symmetric treatments, ii) a topological quantization condition leading to voltage quantization follows, and iii) spin interferometers can be conceived in which, starting from an arbitrary incoming unpolarized spinor, it is always possible to construct a perfect spin filtering condition.
KW - Gauge field theory
KW - Spin Hall effect
KW - Spin transport
KW - Spin-orbit interaction
UR - http://www.scopus.com/inward/record.url?scp=77649119079&partnerID=8YFLogxK
U2 - 10.5488/CMP.12.4.707
DO - 10.5488/CMP.12.4.707
M3 - Artículo
AN - SCOPUS:77649119079
SN - 1607-324X
VL - 12
SP - 707
EP - 716
JO - Condensed Matter Physics
JF - Condensed Matter Physics
IS - 4
ER -