32,724 research outputs found
A canonical Frobenius structure
We show that it makes sense to speak of THE Frobenius manifold attached to a
convenient and nondegenerate Laurent polynomialComment: 24 page
Universal amplitude ratios in the 3D Ising Universality Class
We compute a number of universal amplitude ratios in the three-dimensional
Ising universality class. To this end, we perform Monte Carlo simulations of
the improved Blume-Capel model on the simple cubic lattice. For example, we
obtain A_+/A_-=0.536(2) and C_+/C_-=4.713(7), where A_+- and C_+- are the
amplitudes of the specific heat and the magnetic susceptibility, respectively.
The subscripts + and - indicate the high and the low temperature phase,
respectively. We compare our results with those obtained from previous Monte
Carlo simulations, high and low temperature series expansions, field theoretic
methods and experiments.Comment: 18 pages, two figures, typos corrected, discussion on finite size
corrections extende
Quarks in Finite Nuclei
We describe the development of a theoretical description of the structure of
finite nuclei based on a relativistic quark model of the structure of the bound
nucleons which interact through the (self-consistent) exchange of scalar and
vector mesons.Comment: Invited talks presented at the Joint Japan-Australian Workshop on
"Quarks, Hadrons and Nuclei", Adelaide, November 1995, to appear in
Australian Jounal of Physic
Quark-Meson Coupling Model for a Nucleon
The quark-meson coupling model for a nucleon is considered. The model
describes a nucleon as an MIT bag, in which quarks are coupled to scalar and
vector mesons. A set of coupled equations for the quark and the meson fields
are obtained and are solved in a self-consistent way. It is shown that the mass
of a nucleon as a dressed MIT bag interacting with sigma- and omega-meson
fields significantly differs from the mass of a free MIT bag. A few sets of
model parameters are obtained so that the mass of a dressed MIT bag becomes the
nucleon mass. The results of our calculations imply that the self-energy of the
bag in the quark-meson coupling model is significant and needs to be considered
in doing the nuclear matter calculations.Comment: 3 figure
Finite-dimensional analogs of string s <-> t duality and pentagon equation
We put forward one of the forms of functional pentagon equation (FPE), known
from the theory of integrable models, as an algebraic explanation to the
phenomenon known in physics as st duality. We present two simple geometrical
examples of FPE solutions, one of them yielding in a particular case the
well-known Veneziano expression for 4-particle amplitude. Finally, we interpret
our solutions of FPE in terms of relations in Lie groups.Comment: LaTeX, 12 pages, 6 eps figure
Injection and detection of spin in a semiconductor by tunneling via interface states
Injection and detection of spin accumulation in a semiconductor having
localized states at the interface is evaluated. Spin transport from a
ferromagnetic contact by sequential, two-step tunneling via interface states is
treated not in itself, but in parallel with direct tunneling. The spin
accumulation induced in the semiconductor channel is not suppressed, as
previously argued, but genuinely enhanced by the additional spin current via
interface states. Spin detection with a ferromagnetic contact yields a weighted
average of the spin accumulation in the channel and in the localized states. In
the regime where the spin accumulation in the localized states is much larger
than that in the channel, the detected spin signal is insensitive to the spin
accumulation in the localized states and the ferromagnet probes the spin
accumulation in the semiconductor channel.Comment: 7 pages, 2 figures. Theory onl
Variations of Hadron Masses and Matter Properties in Dense Nuclear Matter
Using a self-consistent quark model for nuclear matter we investigate
variations of the masses of the non-strange vector mesons, the hyperons and the
nucleon in dense nuclear matter (up to four times the normal nuclear density).
We find that the changes in the hadron masses can be described in terms of the
value of the scalar mean-field in matter. The model is then used to calculate
the density dependence of the quark condensate in-medium, which turns out to be
well approximated by a linear function of the nuclear density. Some relations
among the hadron properties and the in-medium quark condensate are discussed.Comment: 22 pages, University of Adelaide preperint ADP-94-20/T160, submitted
to Physical Review
Thermal spin current and magnetothermopower by Seebeck spin tunneling
The recently observed Seebeck spin tunneling, the thermoelectric analog of
spin-polarized tunneling, is described. The fundamental origin is the spin
dependence of the Seebeck coefficient of a tunnel junction with at least one
ferromagnetic electrode. Seebeck spin tunneling creates a thermal flow of
spin-angular momentum across a tunnel barrier without a charge tunnel current.
In ferromagnet/insulator/semiconductor tunnel junctions this can be used to
induce a spin accumulation (\Delta \mu) in the semiconductor in response to a
temperature difference (\Delta T) between the electrodes. A phenomenological
framework is presented to describe the thermal spin transport in terms of
parameters that can be obtained from experiment or theory. Key ingredients are
a spin-polarized thermoelectric tunnel conductance and a tunnel spin
polarization with non-zero energy derivative, resulting in different Seebeck
tunnel coefficients for majority and minority spin electrons. We evaluate the
thermal spin current, the induced spin accumulation and \Delta\mu/\Delta T,
discuss limiting regimes, and compare thermal and electrical flow of spin
across a tunnel barrier. A salient feature is that the thermally-induced spin
accumulation is maximal for smaller tunnel resistance, in contrast to the
electrically-induced spin accumulation that suffers from the impedance mismatch
between a ferromagnetic metal and a semiconductor. The thermally-induced spin
accumulation produces an additional thermovoltage proportional to \Delta\mu,
which can significantly enhance the conventional charge thermopower. Owing to
the Hanle effect, the thermopower can also be manipulated with a magnetic
field, producing a Hanle magnetothermopower.Comment: 10 pages, 3 figures, 1 tabl
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