986 research outputs found
Perturbative nonequilibrium dynamics of phase transitions in an expanding universe
A complete set of Feynman rules is derived, which permits a perturbative
description of the nonequilibrium dynamics of a symmetry-breaking phase
transition in theory in an expanding universe. In contrast to a
naive expansion in powers of the coupling constant, this approximation scheme
provides for (a) a description of the nonequilibrium state in terms of its own
finite-width quasiparticle excitations, thus correctly incorporating
dissipative effects in low-order calculations, and (b) the emergence from a
symmetric initial state of a final state exhibiting the properties of
spontaneous symmetry breaking, while maintaining the constraint . Earlier work on dissipative perturbation theory and spontaneous symmetry
breaking in Minkowski spacetime is reviewed. The central problem addressed is
the construction of a perturbative approximation scheme which treats the
initial symmetric state in terms of the field , while the state that
emerges at later times is treated in terms of a field , linearly related
to . The connection between early and late times involves an infinite
sequence of composite propagators. Explicit one-loop calculations are given of
the gap equations that determine quasiparticle masses and of the equation of
motion for and the renormalization of these equations is
described. The perturbation series needed to describe the symmetric and
broken-symmetry states are not equivalent, and this leads to ambiguities
intrinsic to any perturbative approach. These ambiguities are discussed in
detail and a systematic procedure for matching the two approximations is
described.Comment: 22 pages, using RevTeX. 6 figures. Submitted to Physical Review
Nonequilibrium perturbation theory for complex scalar fields
Real-time perturbation theory is formulated for complex scalar fields away
from thermal equilibrium in such a way that dissipative effects arising from
the absorptive parts of loop diagrams are approximately resummed into the
unperturbed propagators. Low order calculations of physical quantities then
involve quasiparticle occupation numbers which evolve with the changing state
of the field system, in contrast to standard perturbation theory, where these
occupation numbers are frozen at their initial values. The evolution equation
of the occupation numbers can be cast approximately in the form of a Boltzmann
equation. Particular attention is given to the effects of a non-zero chemical
potential, and it is found that the thermal masses and decay widths of
quasiparticle modes are different for particles and antiparticles.Comment: 15 pages using RevTeX; 2 figures in 1 Postscript file; Submitted to
Phys. Rev.
5d superconformal field theories and graphs
We propose graphs, the Combined Fiber Diagrams (CFD), to characterize all 5d superconformal field theories (SCFTs) that arise as S1-reductions of 6d SCFTs. Transitions between CFDs encode mass deformations that trigger RG-flows between SCFTs. They provide a combinatorial classification of all such 5d SCFTs and encode physical information about the strongly coupled theories, like the superconformal flavor symmetry and BPS states. We consistently reproduce known results, but more importantly predict new theories and strong coupling effects in 5d SCFTs
Nonequilibrium perturbation theory for spin-1/2 fields
A partial resummation of perturbation theory is described for field theories
containing spin-1/2 particles in states that may be far from thermal
equilibrium. This allows the nonequilibrium state to be characterized in terms
of quasiparticles that approximate its true elementary excitations. In
particular, the quasiparticles have dispersion relations that differ from those
of free particles, finite thermal widths and occupation numbers which, in
contrast to those of standard perturbation theory evolve with the changing
nonequilibrium environment. A description of this kind is essential for
estimating the evolution of the system over extended periods of time. In
contrast to the corresponding description of scalar particles, the structure of
nonequilibrium fermion propagators exhibits features which have no counterpart
in the equilibrium theory.Comment: 16 pages; no figures; submitted to Phys. Rev.
Component masses of young, wide, non-magnetic white dwarf binaries in the SDSS DR7
We present a spectroscopic component analysis of 18 candidate young, wide,
non-magnetic, double-degenerate binaries identified from a search of the Sloan
Digital Sky Survey Data Release 7 (DR7). All but two pairings are likely to be
physical systems. We show SDSS J084952.47+471247.7 + SDSS J084952.87+471249.4
to be a wide DA+DB binary, only the second identified to date. Combining our
measurements for the components of 16 new binaries with results for three
similar, previously known systems within the DR7, we have constructed a mass
distribution for the largest sample to date (38) of white dwarfs in young,
wide, non-magnetic, double-degenerate pairings. This is broadly similar in form
to that of the isolated field population with a substantial peak around M~0.6
Msun. We identify an excess of ultra-massive white dwarfs and attribute this to
the primordial separation distribution of their progenitor systems peaking at
relatively larger values and the greater expansion of their binary orbits
during the final stages of stellar evolution. We exploit this mass distribution
to probe the origins of unusual types of degenerates, confirming a mild
preference for the progenitor systems of high-field-magnetic white dwarfs, at
least within these binaries, to be associated with early-type stars.
Additionally, we consider the 19 systems in the context of the stellar initial
mass-final mass relation. None appear to be strongly discordant with current
understanding of this relationship.Comment: 20 pages, 5 Tables, 7 figures. accepted for publication in MNRA
Binary Reactive Adsorbate on a Random Catalytic Substrate
We study the equilibrium properties of a model for a binary mixture of
catalytically-reactive monomers adsorbed on a two-dimensional substrate
decorated by randomly placed catalytic bonds. The interacting and
monomer species undergo continuous exchanges with particle reservoirs and react
() as soon as a pair of unlike particles appears on sites
connected by a catalytic bond.
For the case of annealed disorder in the placement of the catalytic bonds
this model can be mapped onto a classical spin model with spin values , with effective couplings dependent on the temperature and on the mean
density of catalytic bonds. This allows us to exploit the mean-field theory
developed for the latter to determine the phase diagram as a function of in
the (symmetric) case in which the chemical potentials of the particle
reservoirs, as well as the and interactions are equal.Comment: 12 pages, 4 figure
Critical properties of the topological Ginzburg-Landau model
We consider a Ginzburg-Landau model for superconductivity with a Chern-Simons
term added. The flow diagram contains two charged fixed points corresponding to
the tricritical and infrared stable fixed points. The topological coupling
controls the fixed point structure and eventually the region of first order
transitions disappears. We compute the critical exponents as a function of the
topological coupling. We obtain that the value of the exponent does not
vary very much from the XY value, . This shows that the
Chern-Simons term does not affect considerably the XY scaling of
superconductors. We discuss briefly the possible phenomenological applications
of this model.Comment: RevTex, 7 pages, 8 figure
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