12 research outputs found
Spin-charge separation in a strongly correlated spin-polarized chain
We combine the first-quantized path-integral formalism and bosonization to
develop a phenomenological theory for spin-charge coupled dynamics in
one-dimensional (1D) ferromagnetic systems with strong interparticle repulsion,
at low temperatures. We assume an effective spin-charge separation and retain
the standard Luttinger-liquid plasmon branch, which is explicitly coupled to a
ferromagnetic spin-wave texture with a quadratic dispersion. The dynamic spin
structure severely suppresses the plasmon peak in the single-particle
propagator, in both fermionic and bosonic systems. Our analysis provides an
effective theory for the new universality class of 1D ferromagnetic systems,
capturing both the trapped spin and propagating spin-wave regimes of the
long-time behavior.Comment: 5 pages, 1 figur
Spin-selective localization due to intrinsic spin-orbit coupling
We study spin-dependent diffusive transport in the presence of a tunable
spin-orbit (SO) interaction in a two-dimensional electron system. The spin
precession of an electron in the SO coupling field is expressed in terms of a
covariant curvature, affecting the quantum interference between different
electronic trajectories. Controlling this curvature field by modulating the SO
coupling strength and its gradients by, e.g., electric or elastic means, opens
intriguing possibilities for exploring spin-selective localization physics. In
particular, applying a weak magnetic field allows the control of the electron
localization independently for two spin directions, with the spin-quantization
axis that could be "engineered" by appropriate SO interaction gradients.Comment: 7 pages, 1 figur
Negative effective mass transition and anomalous transport in power-law hopping bands
We study the stability of spinless Fermions with power law hopping . It is shown that at precisely , the
dispersive inflection point coalesces with the band minimum and the charge
carriers exhibit a transition into negative effective mass regime, characterized by retarded transport in the presence of an electric field.
Moreover, bands with must be accompanied by counter-carriers with
, having a positive band curvature, thus stabilizing the system
in order to maintain equilibrium conditions and a proper electrical response.
We further examine the semi-classical transport and response properties,
finding an infrared divergent conductivity for 1/r hopping(). The
analysis is generalized to regular lattices in dimensions = 1, 2, and 3.Comment: 6 pages. 2 figure
Disorder induced transition into a one-dimensional Wigner glass
The destruction of quasi-long range crystalline order as a consequence of
strong disorder effects is shown to accompany the strict localization of all
classical plasma modes of one-dimensional Wigner crystals at T=0. We construct
a phase diagram that relates the structural phase properties of Wigner crystals
to a plasmon delocalization transition recently reported. Deep inside the
strictly localized phase of the strong disorder regime, we observe
``glass-like'' behavior. However, well into the critical phase with a plasmon
mobility edge, the system retains its crystalline composition. We predict that
a transition between the two phases occurs at a critical value of the relative
disorder strength. This transition has an experimental signature in the AC
conductivity as a local maximum of the largest spectral amplitude as a function
of the relative disorder strength.Comment: 5 pages, revtex. Typo regarding localization length exponent
corrected. Should read 1 / \delt
Anderson transition of the plasma oscillations of 1D disordered Wigner lattices
We report the existence of a localization-delocalization transition in the
classical plasma modes of a one dimensional Wigner Crystal with a white noise
potential environment at T=0. Finite size scaling analysis reveals a divergence
of the localization length at a critical eigenfrequency. Further scaling
analysis indicates power law behavior of the critical frequency in terms of the
relative interaction strength of the charges. A heuristic argument for this
scaling behavior is consistent with the numerical results. Additionally, we
explore a particular realization of random-bond disorder in a one dimensional
Wigner lattice in which all of the collective modes are observed to be
localized.Comment: 4 pages, 3 figures, Typo for the localization length corrected.
Should read 1 / \n