1,849 research outputs found
The Matsubara-Fradkin Thermodynamical Quantization of Podolsky Electrodynamics
In this work we apply the Matsubara-Fradkin formalism and the Nakanishi's
auxiliary field method to the quantization of the Podolsky electrodynamics in
thermodynamic equilibrium. This approach allows us to write consistently the
path integral representation for the partition function of gauge theories in a
simple manner. Furthermore, we find the Dyson-Schwinger-Fradkin equations and
the Ward-Fradkin-Takahashi identities for the Podolsky theory. We also write
the most general form for the polarization tensor in thermodynamic equilibrium.Comment: Submitted to Physical Review
Charge-Density-Wave and Superconductor Competition in Stripe Phases of High Temperature Superconductors
We discuss the problem of competition between a superconducting (SC) ordered
state with a charge density wave (CDW) state in stripe phases of high
superconductors. We consider an effective model for each stripe motivated by
studies of spin-gapped electronic ladder systems. We analyze the problem of
dimensional crossover arising from inter-stripe SC and CDW couplings using
non-Abelian bosonization and renormalization group (RG) arguments to derive an
effective -symmetric nonlinear -model in for the case of
when both inter-stripe couplings are of equal magnitude as well as equally RG
relevant. By studying the effects of various symmetry lowering perturbations,
we determine the structure of the phase diagram and show that, in general, it
has a broad regime in which both orders coexist. The quantum and thermal
critical behavior is discussed in detail, and the phase coexistence region is
found to end at associated as well as tetracritical points. The
possible role of hedgehog topological excitations of the theory is considered
and argued to be RG irrelevant at the spatially anisotropic higher dimensional
low-energy fixed point theory. Our results are also relevant to the case of
competing N\'eel and valence bond solid (VBS) orders in quantum magnets on 2D
isotropic square as well as rectangular lattices interacting via nearest
neighbor Heisenberg exchange interactions.Comment: 9 pages, 3 figures (one with 3 subfigures
Exact Transformation for Spin-Charge Separation of Spin-half Fermions without Constraints
We demonstrate an exact local transformation which maps a purely Fermionic
manybody system to a system of spinfull Bosons and spinless Fermions,
demonstrating a possible path to a non-Fermi liquid state. We apply this to the
half-filled Hubbard model and show how the transformation maps the ordinary
spin half Fermionic degrees of freedom exactly and without introducing Hilbert
space constraints to a charge-like ``quasicharge'' fermion and a spin-like
``quasispin'' Boson while preserving all the symmetries of the model. We
present approximate solutions with localized charge which emerge naturally from
the Hubbard model in this form. Our results strongly suggest that charge tends
to remain localized for large values of the Hubbard U
Geometric criticality between plaquette phases in integer-spin kagome XXZ antiferromagnets
The phase diagram of the uniaxially anisotropic antiferromagnet on the
kagom\'e lattice includes a critical line exactly described by the classical
three-color model. This line is distinct from the standard geometric classical
criticality that appears in the classical limit () of the 2D XY
model; the geometric T=0 critical line separates two unconventional
plaquette-ordered phases that survive to nonzero temperature. The
experimentally important correlations at finite temperature and the nature of
the transitions into these ordered phases are obtained using the mapping to the
three-color model and a combination of perturbation theory and a variational
ansatz for the ordered phases. The ordered phases show sixfold symmetry
breaking and are similar to phases proposed for the honeycomb lattice dimer
model and model. The same mapping and phase transition can be
realized also for integer spins but then require strong on-site
anisotropy in the Hamiltonian.Comment: 5 pages, 2 figure
Theory of the nodal nematic quantum phase transition in superconductors
We study the character of an Ising nematic quantum phase transition (QPT)
deep inside a d-wave superconducting state with nodal quasiparticles in a
two-dimensional tetragonal crystal. We find that, within a 1/N expansion, the
transition is continuous. To leading order in 1/N, quantum fluctuations enhance
the dispersion anisotropy of the nodal excitations, and cause strong scattering
which critically broadens the quasiparticle (qp) peaks in the spectral
function, except in a narrow wedge in momentum space near the Fermi surface
where the qp's remain sharp. We also consider the possible existence of a
nematic glass phase in the presence of weak disorder. Some possible
implications for cuprate physics are also discussed.Comment: 9 page, 4 figures, an error in one of expressions corrected and a new
author was added. New references and footnotes are added and this is the
version to appear in PR
3-point off-shell vertex in scalar QED in arbitrary gauge and dimension
We calculate the complete one-loop off-shell three-point scalar-photon vertex
in arbitrary gauge and dimension for Scalar Quantum Electrodynamics. Explicit
results are presented for the particular cases of dimensions 3 and 4 both for
massive and massless scalars. We then propose non-perturbative forms of this
vertex that coincide with the perturbative answer to order .Comment: Uses axodra
Surface pinning of fluctuating charge order: an "extraordinary" surface phase transition
We study the mean-field theory of charge-density wave (CDW) order in a
layered system, including the effect of the long-range Coulomb interaction and
of screening by uncondensed electrons. We particularly focus on the conditions
necessary for an ``extraordinary'' transition, in which the surface orders at a
higher temperature, and is more likely to be commensurate, than the bulk. We
interpret recent experiments on NaCCOC as indicating the presence of
commensurate CDW at the surface that is not present in the bulk. More
generally, we show that poor screening of the Coulomb interaction tends to
stabilize incommensurate order, possibly explaining why the CDW order in LSCO
and NbSe2 remains incommensurate to T -> 0, despite the small magnitude of the
incommensurability.Comment: 9 pages, no figures, 31 references; 1 new figure and minor editing of
the tex
On dilaton dependence of type II superstring action
The supersymmetric action of type IIA D=10 superstring in N=2a, D=10
supergravity background can be derived by double dimensional reduction of the
action of supermembrane coupled to D=11 supergravity. We demonstrate that the
background Ramond-Ramond fields appear in the resulting superstring action with
an extra factor of exponential of the dilaton.Comment: 6 pages, harvmac (references added
Nintendo Wii Free Run vs. Treadmill Running: A Comparison of Physiological and Metabolic Data
Please view abstract in the attached PDF file
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