2,429 research outputs found
Incommensurate ground state of double-layer quantum Hall systems
Double-layer quantum Hall systems possess interlayer phase coherence at
sufficiently small layer separations, even without interlayer tunneling. When
interlayer tunneling is present, application of a sufficiently strong in-plane
magnetic field drives a commensurate-incommensurate (CI)
transition to an incommensurate soliton-lattice (SL) state. We calculate the
Hartree-Fock ground-state energy of the SL state for all values of
within a gradient approximation, and use it to obtain the
anisotropic SL stiffness, the Kosterlitz-Thouless melting temperature for the
SL, and the SL magnetization. The in-plane differential magnetic susceptibility
diverges as when the CI transition is approached
from the SL state.Comment: 12 pages, 7 figures, to be published in Physical Review
Pseudo-spin canting transition in bilayer quantum Hall ferromagnets: a self-charging capacitor
For sufficiently strong in-plane magnetic field a bilayer quantum
Hall pseudo-ferromagnet is expected to exhibit a soliton lattice. For
sufficiently close layers and large in-plane field, we predict this
incommensurate ``planar'' phase to undergo a reentrant pseudo-spin
canting transition to an incommensurate state , with a finite out-of-plane
pseudo-magnetization component, corresponding to an interlayer charge imbalance
in regions between solitons. At the transition is in the 2d compressible
Ising universality class, and at T=0, the quantum transition is in heretofore
unexplored universality class. The striking experimental signatures are the
universal nonlinear charge-voltage and in-plane field relations, and the
divergence of the differential bilayer capacitance at the transition, resulting
in a bilayer capacitor that spontaneously charges itself, even in the absence
of an applied interlayer voltage.Comment: 4 RevTeX pgs, 1 eps figures, submitted to PR
A sol-gel method for growing superconducting MgB2 films
In this paper we report a new sol-gel method for the fabrication of MgB2
films. Polycrystalline MgB2 films were prepared by spin-coating a precursor
solution of Mg(BH_4)_2 diethyl ether on (001)Al2O3 substrates followed with
annealing in Mg vapor. In comparison with the MgB2 films grown by other
techniques, our films show medium qualities including a superconducting
transition temperature of Tc ~ 37 K, a critical current density of Jc(5 K, 0 T)
~ 5 {\times} 10^6 A cm^{-2}, and a critical field of H_{c2}(0) ~ 19 T. Such a
sol-gel technique shows potential in the commercial fabrication of practically
used MgB2 films as well as MgB2 wires and tapes.Comment: 8 pages, 5 figure
Reentrant Melting of Soliton Lattice Phase in Bilayer Quantum Hall System
At large parallel magnetic field , the ground state of bilayer
quantum Hall system forms uniform soliton lattice phase. The soliton lattice
will melt due to the proliferation of unbound dislocations at certain finite
temperature leading to the Kosterlitz-Thouless (KT) melting. We calculate the
KT phase boundary by numerically solving the newly developed set of Bethe
ansatz equations, which fully take into account the thermal fluctuations of
soliton walls. We predict that within certain ranges of , the
soliton lattice will melt at . Interestingly enough, as temperature
decreases, it melts at certain temperature lower than exhibiting
the reentrant behaviour of the soliton liquid phase.Comment: 11 pages, 2 figure
Double-Layer Systems at Zero Magnetic Field
We investigate theoretically the effects of intralayer and interlayer
exchange in biased double-layer electron and hole systems, in the absence of a
magnetic field. We use a variational Hartree-Fock-like approximation to analyze
the effects of layer separation, layer density, tunneling, and applied gate
voltages on the layer densities and on interlayer phase coherence. In agreement
with earlier work, we find that for very small layer separations and low layer
densities, an interlayer-correlated ground state possessing spontaneous
interlayer coherence (SILC) is obtained, even in the absence of interlayer
tunneling. In contrast to earlier work, we find that as a function of total
density, there exist four, rather than three, distinct noncrystalline phases
for balanced double-layer systems without interlayer tunneling. The newly
identified phase exists for a narrow range of densities and has three
components and slightly unequal layer densities, with one layer being spin
polarized, and the other unpolarized. An additional two-component phase is also
possible in the presence of sufficiently strong bias or tunneling. The
lowest-density SILC phase is the fully spin- and pseudospin-polarized
``one-component'' phase discussed by Zheng {\it et al.} [Phys. Rev. B {\bf 55},
4506 (1997)]. We argue that this phase will produce a finite interlayer Coulomb
drag at zero temperature due to the SILC. We calculate the particle densities
in each layer as a function of the gate voltage and total particle density, and
find that interlayer exchange can reduce or prevent abrupt transfers of charge
between the two layers. We also calculate the effect of interlayer exchange on
the interlayer capacitance.Comment: 35 pages, 19 figures included. To appear in PR
Spontaneous coherence and the quantum Hall Effect in triple-layer electron systems
We investigate spontaneous interlayer phase coherence and the occurrence of
the quantum Hall effect in triple-layer electron systems. Our work is based on
a simple tight-binding model that greatly facilitates calculations and whose
accuracy is verified by comparison with recent experiments. By calculating the
ground state in an unrestricted Hartree-Fock approximation and the
collective-mode spectrum in a time-dependent Hartree-Fock approximation, we
construct a phase diagram delimiting regions in the parameter space of the
model where the integer quantum Hall effect occurs in the absence of interlayer
tunneling.Comment: To appear in Phys. Rev. B, 20 pages, 5 PostScript figures uuencoded
with TeX fil
Spin-flip scattering in the quantum Hall regime
We present a microscopic theory of spin-orbit coupling in the integer quantum
Hall regime. The spin-orbit scattering length is evaluated in the limit of
long-range random potential. The spin-flip rate is shown to be determined by
rare fluctuations of anomalously high electric field. A mechanism of strong
spin-orbit scattering associated with exchange-induced spontaneous
spin-polarization is suggested. Scaling of the spin-splitting of the
delocalization transition with the strength of spin-orbit and exchange
interactions is also discussed.Comment: References added, small additional comments, to appear in Phys. Rev.
B; 23 pages, RevTeX 3.
Persistent Spin Currents in Helimagnets
We demonstrate that weak external magnetic fields generate dissipationless
spin currents in the ground state of systems with spiral magnetic order. Our
conclusions are based on phenomenological considerations and on microscopic
mean-field theory calculations for an illustrative toy model. We speculate on
possible applications of this effect in spintronic devices.Comment: 9 pages, 6 figures, updated version as published, Journal referenc
Probing Interband Coulomb Interactions in Semiconductor Nanocrystals with 2D Double-Quantum Coherence Spectroscopy
Using previously developed exciton scattering model accounting for the
interband, i.e., exciton-biexciton, Coulomb interactions in semiconductor
nanocrystals (NCs), we derive a closed set of equations for 2D double-quantum
coherence signal. The signal depends on the Liouville space pathways which
include both the interband scattering processes and the inter- and intraband
optical transitions. These processes correspond to the formation of different
cross-peaks in the 2D spectra. We further report on our numerical calculations
of the 2D signal using reduced level scheme parameterized for PbSe NCs. Two
different NC excitation regimes considered and unique spectroscopic features
associated with the interband Coulomb interactions are identified.Comment: 11 pages, 5 figure
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