Dr. Yuli Lyanda-Geller
Purdue University
Spin-electric State
Spin-orbit interactions cause many remarkable phenomena in
many fields of physics. During the past decade, considerable effort was
devoted to spin Hall effect and related phenomena. In this talk I
will discuss a new state of matter, spin-electric state, that arises due to
spin currents. I will show that in the presence of electric
current, the electron spin polarization normal to the plane of the
two-dimensional (2D) semiconductor can reach its maximal possible value, making
all electrons polarized spin up or spin down. I will show that this
happens at the edges of the 2D sample if spin relaxation is weak. In the
spin-electric state, two stripes near the edges emerge with induced electric
fields directed perpendicular to flowing electric current caused by applied
external field. The directions of the induced fields at two edges are opposite
to each other. These electric fields and corresponding voltages represent
true Hall voltage and electric signal caused by spin current. In the central
stripe between the two edge stripes, the spin polarization and electric fields
change their sign in the middle, where their magnitude vanishes. The
spin-electric structure can be detected by measuring the potential drop between
the edge and the middle of the sample. I will describe microscopic theory
of the spin-electric state, and discuss self-consistent solution of the
two-dimensional electrostatic problem in the presence of spin currents. I will
show how to make spin-orbit interactions for electrons and holes being large
enough to generate the spin electric state but small enough to give weak spin
relaxation. I will describe microscopic theory of the spin-electric
state, and discuss self-consistent solution of the two-dimensional
electrostatic problem in the presence of spin currents. I will show how to make
spin-orbit interactions for electrons and holes being large enough to generate
the spin electric state but small enough to give weak spin relaxation.
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