771 research outputs found
Density-functional theory for fermions in the unitary regime
In the unitary regime, fermions interact strongly via two-body potentials
that exhibit a zero range and a (negative) infinite scattering length. The
energy density is proportional to the free Fermi gas with a proportionality
constant . We use a simple density functional parametrized by an effective
mass and the universal constant , and employ Kohn-Sham density-functional
theory to obtain the parameters from fit to one exactly solvable two-body
problem. This yields and a rather large effective mass. Our approach
is checked by similar Kohn-Sham calculations for the exactly solvable Calogero
model.Comment: 5 pages, 2 figure
Octet Baryon Charge Radii, Chiral Symmetry and Decuplet Intermediate States
We compute the octet baryon charge radii to O(1/Heavy^3) in heavy baryon
chiral perturbation theory. We examine the effect of including the decuplet of
spin-3/2 baryons explicitly. We find that it does no t improve the level of
agreement between the HBchiPT and experimental values for the Sigma^- charge
radius.Comment: 9 pages, 2 figures. Uses axodraw.sty, include
Chiral Symmetry and the Parity-Violating Yukawa Coupling
We construct the complete SU(2) parity-violating (PV)
interaction Lagrangian with one derivative, and calculate the chiral
corrections to the PV Yukawa coupling constant through in the leading order of heavy baryon expansion. We
discuss the relationship between the renormalized \hpi, the measured value of
\hpi, and the corresponding quantity calculated microscopically from the
Standard Model four-quark PV interaction.Comment: RevTex, 26 pages + 5 PS figure
Subleading corrections to parity-violating pion photoproduction
We compute the photon asymmetry Bγ for near threshold parity-violating (PV) pion photoproduction through subleading order. We show that subleading contributions involve a new combination of PV couplings not included in previous analyses of hadronic PV. We argue that existing constraints on the leading order contribution to Bγ—obtained from the PV γ-decay of 18F—suggest that the impact of the subleading contributions may be more significant than expected from naturalness arguments
Anomalous Chiral Action from the Path-Integral
By generalizing the Fujikawa approach, we show in the path-integral
formalism: (1) how the infinitesimal variation of the fermion measure can be
integrated to obtain the full anomalous chiral action; (2) how the action
derived in this way can be identified as the Chern-Simons term in five
dimensions, if the anomaly is consistent; (3) how the regularization can be
carried out, so as to lead to the consistent anomaly and not to the covariant
anomaly. Our method uses Schwinger's ``proper-time'' representation of the
Green's function and the gauge invariant point-splitting technique. We find
that the consistency requirement and the point-splitting technique allow both
an anomalous and a non-anomalous action. In the end, the nature of the vacuum
determines whether we have an anomalous theory, or, a non-anomalous theoryComment: 28 page
Density Functional Theory: Methods and Problems
The application of density functional theory to nuclear structure is
discussed, highlighting the current status of the effective action approach
using effective field theory, and outlining future challenges.Comment: 10 pages, 14 figures, invited talk at INT workshop on Nuclear Forces
and the Quantum Many-Body Problem, Seattle, October 200
Recoil Order Chiral Corrections to Baryon Octet Axial Currents
We calculate chiral corrections to the octet axial currents through using baryon chiral perturbation theory (BCPT). The relativistic BCPT
framework allows one to sum an infinite series of recoil corrections at a given
order in the chiral expansion. We also include SU(3)-breaking operators
occuring at not previously considered. We determine the
corresponding low-energy constants (LEC's) from hyperon semileptonic decay data
using a variety of infrared regularization schemes. We find that the chiral
expansion of the axial currents does not display the proper convergence
behavior, regardless of which scheme is chosen. We explore the implications of
our analysis for determinations of the strange quark contribution to the
nucleon spin, .Comment: RevTex, 19 pages + 2 PS figure
Baryon magnetic moments and sigma terms in lattice-regularized chiral perturbation theory
An SU(3) chiral Lagrangian for the lightest decuplet of baryons is
constructed on a discrete lattice of spacetime points, and is added to an
existing lattice Lagrangian for the lightest octets of mesons and baryons. A
nonzero lattice spacing renders all loop integrations finite, and the continuum
limit of any physical observable is identical to the result obtained from
dimensional regularization. Chiral symmetry and gauge invariance are preserved
even at nonzero lattice spacing. Specific calculations discussed here include
the non-renormalization of a conserved vector current, the magnetic moments of
octet baryons, and the pi N and KN sigma terms that relate to the nucleon's
strangeness content. The quantitative difference between physics at a nonzero
lattice spacing and physics in the continuum limit is easily computed, and it
represents an expectation for the size of discretization errors in
corresponding lattice QCD simulations.Comment: 19 pages, 5 figures, one paragraph added to introduction, to appear
in Phys Rev
Superconductivity from a melted insulator
Quantum phase transitions typically result in a broadened critical or
crossover region at nonzero temperature. Josephson arrays are a model of this
phenomenon, exhibiting a superconductor-insulator transition at a critical wave
impedance, and a well-understood insulating phase. Yet high-impedance arrays
used in quantum computing and metrology apparently evade this transition,
displaying superconducting behavior deep into the nominally insulating regime.
The absence of critical behavior in such devices is not well understood. Here
we show that, unlike the typical quantum-critical broadening scenario, in
Josephson arrays temperature dramatically shifts the critical region. This
shift leads to a regime of superconductivity at high temperature, arising from
the melted zero-temperature insulator. Our results quantitatively explain the
low-temperature onset of superconductivity in nominally insulating regimes, and
the transition to the strongly insulating phase. We further present, to our
knowledge, the first understanding of the onset of anomalous-metallic
resistance saturation. This work demonstrates a non-trivial interplay between
thermal effects and quantum criticality. A practical consequence is that,
counterintuitively, the coherence of high-impedance quantum circuits is
expected to be stabilized by thermal fluctuations.Comment: 8+18 pages, 4+15 figure
- …