185 research outputs found
Quantized Thermal Transport in the Fractional Quantum Hall Effect
We analyze thermal transport in the fractional quantum Hall effect (FQHE),
employing a Luttinger liquid model of edge states. Impurity mediated
inter-channel scattering events are incorporated in a hydrodynamic description
of heat and charge transport. The thermal Hall conductance, , is shown to
provide a new and universal characterization of the FQHE state, and reveals
non-trivial information about the edge structure. The Lorenz ratio between
thermal and electrical Hall conductances {\it violates} the free-electron
Wiedemann-Franz law, and for some fractional states is predicted to be {\it
negative}. We argue that thermal transport may provide a unique way to detect
the presence of the elusive upstream propagating modes, predicted for fractions
such as and .Comment: 6 pages REVTeX, 2 postscript figures (uuencoded and compressed
Coulomb blockade of strongly coupled quantum dots studied via bosonization of a channel with a finite barrier
A pair of quantum dots, coupled through a point contact, can exhibit Coulomb
blockade effects that reflect an oscillatory term in the dots' total energy
whose value depends on whether the total number of electrons on the dots is
even or odd. The effective energy associated with this even-odd alternation is
reduced, relative to the bare Coulomb blockade energy for uncoupled dots, by a
factor (1-f) that decreases as the interdot coupling is increased. When the
transmission coefficient for interdot electronic motion is independent of
energy and the same for all channels within the point contact (which are
assumed uncoupled), the factor (1-f) takes on a universal value determined
solely by the number of channels and the dimensionless conductance g of each
individual channel.
This paper studies corrections to the universal value of (1-f) that result
when the transmission coefficent varies over energy scales of the size of the
bare Coulomb blockade energy. We consider a model in which the point contact is
described by a single orbital channel containing a parabolic barrier potential,
and we calculate the leading correction to (1-f) for one-channel (spin-split)
and two-channel (spin-degenerate) point contacts in the limit where the single
orbital channel is almost completely open. By generalizing a previously used
bosonization technique, we find that, for a given value of the dimensionless
conductance g, the value of (1-f) is increased relative to its value for a
zero-thickness barrier, but the absolute value of the increase is small in the
region where our calculations apply.Comment: 13 pages, 3 Postscript figure
Colossal anisotropy in diluted magnetic topological insulators
We consider dilute magnetic doping in the surface of a three dimensional
topological insulator where a two dimensional Dirac electron gas resides. We
find that exchange coupling between magnetic atoms and the Dirac electrons has
a strong and peculiar effect on both. First, the exchange-induced single ion
magnetic anisotropy is very large and favors off-plane orientation. In the case
of ferromagnetically ordered phase we find a colossal magnetic anisotropy
energy, of the order of the critical temperature. Second, a persistent
electronic current circulates around the magnetic atom and, in the case of a
ferromagnetic phase, around the edges of the surface.Comment: 4 pages, 3 figure
Electric Field Control of Shallow Donor Impurities in Silicon
We present a tight-binding study of donor impurities in Si, demonstrating the
adequacy of this approach for this problem by comparison with effective mass
theory and experimental results. We consider the response of the system to an
applied electric field: donors near a barrier material and in the presence of
an uniform electric field may undergo two different ionization regimes
according to the distance of the impurity to the Si/barrier interface. We show
that for impurities ~ 5 nm below the barrier, adiabatic ionization is possible
within switching times of the order of one picosecond, while for impurities ~
10 nm or more below the barrier, no adiabatic ionization may be carried out by
an external uniform electric field. Our results are discussed in connection
with proposed Si:P quantum computer architectures.Comment: 18 pages, 6 figures, submitted to PR
Orbital Polarons in the Metal-Insulator Transition of Manganites
The metal-insulator transition in manganites is strongly influenced by the
concentration of holes present in the system. Based upon an orbitally
degenerate Mott-Hubbard model we analyze two possible localization scenarios to
account for this doping dependence: First, we rule out that the transition is
initiated by a disorder-order crossover in the orbital sector, showing that its
effect on charge mobility is only small. Second, we introduce the idea of
orbital polarons originating from a strong polarization of orbitals in the
vicinity of holes. Considering this direct coupling between charge and orbital
degree of freedom in addition to lattice effects we are able to explain well
the phase diagram of manganites for low and intermediate hole concentrations
Reduction in risk-taking behaviors among MSM in Senegal between 2004 and 2007 and prevalence of HIV and others STIs
Electron Exchange Coupling for Single Donor Solid-State Qubits
Inter-valley interference between degenerate conduction band minima has been
shown to lead to oscillations in the exchange energy between neighbouring
phosphorus donor electron states in silicon \cite{Koiller02,Koiller02A}. These
same effects lead to an extreme sensitivity of the exchange energy on the
relative orientation of the donor atoms, an issue of crucial importance in the
construction silicon-based spin quantum computers. In this article we calculate
the donor electron exchange coupling as a function of donor position
incorporating the full Bloch structure of the Kohn-Luttinger electron
wavefunctions. It is found that due to the rapidly oscillating nature of the
terms they produce, the periodic part of the Bloch functions can be safely
ignored in the Heitler-London integrals as was done by Koiller et. al. [Phys.
Rev. Lett. 88,027903(2002),Phys. Rev. B. 66,115201(2002)], significantly
reducing the complexity of calculations.
We address issues of fabrication and calculate the expected exchange coupling
between neighbouring donors that have been implanted into the silicon substrate
using an 15keV ion beam in the so-called 'top down' fabrication scheme for a
Kane solid-state quantum computer. In addition we calculate the exchange
coupling as a function of the voltage bias on control gates used to manipulate
the electron wavefunctions and implement quantum logic operations in the Kane
proposal, and find that these gate biases can be used to both increase and
decrease the magnitude of the exchange coupling between neighbouring donor
electrons. The zero-bias results reconfirm those previously obtained by
Koiller.Comment: 10 Pages, 8 Figures. To appear in Physical Review
Voltage-tunable singlet-triplet transition in lateral quantum dots
Results of calculations and high source-drain transport measurements are
presented which demonstrate voltage-tunable entanglement of electron pairs in
lateral quantum dots. At a fixed magnetic field, the application of a
judiciously-chosen gate voltage alters the ground-state of an electron pair
from an entagled spin singlet to a spin triplet.Comment: 8.2 double-column pages, 10 eps figure
B --> Phi K_S and Supersymmetry
The rare decay B --> Phi K_S is a well-known probe of physics beyond the
Standard Model because it arises only through loop effects yet has the same
time-dependent CP asymmetry as B --> Psi K_S. Motivated by recent data
suggesting new physics in B --> Phi K_S, we look to supersymmetry for possible
explanations, including contributions mediated by gluino loops and by Higgs
bosons. Chirality-preserving LL and RR gluino contributions are generically
small, unless gluinos and squarks masses are close to the current lower bounds.
Higgs contributions are also too small to explain a large asymmetry if we
impose the current upper limit on B(B_s --> mu mu). On the other hand,
chirality-flipping LR and RL gluino contributions can provide sizable effects
and while remaining consistent with related results in B --> Psi K_S, Delta
M_s, B --> X_s gamma and other processes. We discuss how the LR and RL
insertions can be distinguished using other observables, and we provide a
string-based model and other estimates to show that the needed sizes of mass
insertions are reasonable.Comment: 33 pages, 32 figures, Updated version for PRD. Includes discussions
of other recent works on this topic. Added discussions & plots for gluino
mass dependence and effects of theoretical uncertaintie
Local perceptions of mental health in Iran, Semnan Province
Introduction: Understanding local perceptions of mental health in different cultures and contexts is crucial for designing and implementing appropriate mental healthcare services. Methods: This qualitative study was conducted to investigate local perceptions of mental health in two highly populated provincial districts in Iran. Data were collected using the free list technique and interviews. A two-phase training workshop was held with the research team at a local health center, followed by a pilot study with the participation of six subjects. All the interviews were audio-recorded, transcribed, and then analyzed by the third and fourth authors in DEDOOSE. Results: A total of 30 individuals (20 in the free list and 10 as key informants in the interviews) took part in the study. Based on the study findings and the key informants' ideas, mental health problems were categorized into three categories of depression, anxiety, and obsessive�compulsive disorder (OCD). Conclusions: Mental health problems appear to be expressed in different ways and with different symptoms in different cultures, and there is a distinct need for examining mental disorders in each culture and nationality separately using culturally appropriate tools for disease screening. © 2020 The Authors. Brain and Behavior published by Wiley Periodicals LL
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