108 research outputs found
RG Fixed Points in Supergravity Duals of 4-d Field Theory and Asymptotically AdS Spaces
Recently, it has been conjectured that supergravity solutions with two asymptotically AdS regions describe the RG flow of a 4-d field theory from a UV fixed point to an interacting IR fixed point. In this paper we lend support to this conjecture by showing that, in the UV (IR) limit, the two-point function of a minimally-coupled scalar field depends only on the UV (IR) region of the metric, asymptotic to AdS_5. This result is consistent with the interpretation of the radial coordinate of Anti de Sitter space as an energy scale, and it may provide an analog of the Callan-Symanzik equation for supergravity duals of strongly coupled field theories
Holographic zero sound at finite temperature
We use gauge-gravity duality to study the temperature dependence of the zero
sound mode and the fundamental matter diffusion mode in the strongly coupled
{\cal N}=4 SU(N_c) supersymmetric Yang-Mills theory with N_f {\cal N}=2
hypermultiplets in the N_c>>1, N_c>>N_f limit, which is holographically
realized via the D3/D7 brane system. In the high density limit \mu>>T, three
regimes can be identified in the behavior of these modes, analogous to the
collisionless quantum, collisionless thermal and hydrodynamic regimes of a
Landau Fermi-liquid. The transitions between the three regimes are
characterized by the parameters T/\mu and (T/\mu)^2 respectively, and in each
of these regimes the modes have a distinctively different temperature and
momentum dependence. The collisionless-hydrodynamic transition occurs when the
zero sound poles of the density-density correlator in the complex frequency
plane collide on the imaginary axis to produce a hydrodynamic diffusion pole.
We observe that the properties characteristic of a Landau Fermi-liquid zero
sound mode are present in the D3/D7 system despite the atypical T^6/\mu^3
temperature scaling of the specific heat and an apparent lack of a directly
identifiable Fermi surface.Comment: 35 pages, 13 figures, 2 tables, 3 animation
The polarization tensor of neutral gluons in external fields at high temperature
The one-loop polarization operator of neutral gluons in the background
constant Abelian isotopic, , and hypercharge, , chromomagnetic
fields combined with electrostatic potential at high temperature is
calculated. The case when is investigated separately. The proper time
method is applied. It is found that neutral gluons do not acquire magnetic
masses in the background fields, in contrast to the charged ones. The
application of the results are discussed.Comment: 13 pages, 1 figur
Non-transversality of the gluon polarization tensor in a chromomagnetic background
We investigate the question about the transversality of the gluon
polarization tensor in a homogeneous chromomagnetic background field. We
re-derive the non transversality known from a pure one loop calculation using
the Slavnov-Taylor identities. In addition we generalize the procedure to
arbitrary gauge fixing parameter and calculate the -dependent part
of the polarization tensor.Comment: subm. to TM
Complete High Temperature Expansions for One-Loop Finite Temperature Effects
We develop exact, simple closed form expressions for partition functions
associated with relativistic bosons and fermions in odd spatial dimensions.
These expressions, valid at high temperature, include the effects of a
non-trivial Polyakov loop and generalize well-known high temperature
expansions. The key technical point is the proof of a set of Bessel function
identities which resum low temperature expansions into high temperature
expansions. The complete expressions for these partition functions can be used
to obtain one-loop finite temperature contributions to effective potentials,
and thus free energies and pressures.Comment: 9 pages, RevTeX, no figures. To be published in Phys. Rev D. v2 has
revised introduction and conclusions, plus a few typographical errors are
corrected; v3 corrects one typ
Hydrodynamics at RHIC -- how well does it work, where and how does it break down?
I review the successes and limitations of the ideal fluid dynamic model in
describing hadron emission spectra from Au+Au collisions at the Relativistic
Heavy Ion Collider (RHIC).Comment: 8 pages, 4 figures. Invited talk presented at Strange Quark Matter
2004 (Cape Town, Sep. 15-20, 2004). Proceedings to appear in Journal of
Physics
Free Energy of an SU(2) Model of (2+1)-dimensional QCD in the Constant Condensate Background
Gluon and quark contributions to the thermodynamic potential (free energy) of
a (2+1)-dimensional QCD model at finite temperature in the background of a
constant homogeneous chromomagnetic field H combined with A_0 condensate are
calculated. The role of the tachyonic mode in the gluon energy spectrum is
discussed. A possibility of the free energy global minimum generation at
nonzero values of H and A_0 condensates is investigated.Comment: LaTeX 2e, 14 pages, 6 eps figures, some miscalculations were
correcte
Ring diagrams and electroweak phase transition in a magnetic field
Electroweak phase transition in a magnetic field is investigated within the
one-loop and ring diagram contributions to the effective potential in the
minimal Standard Model. All fundamental fermions and bosons are included with
their actual values of masses and the Higgs boson mass is considered in the
range . The effective potential is real at
sufficiently high temperature. The important role of fermions and -bosons in
symmetry behaviour is observed. It is found that the phase transition for the
field strengths G is of first order but the baryogenesis
condition is not satisfied. The comparison with the hypermagnetic field case is
done.Comment: 16 pages, Latex, changed for a mistake in the numerical par
New Insights into Properties of Large-N Holographic Thermal QCD at Finite Gauge Coupling at (the Non-Conformal/Next-to) Leading Order in N
In the context of [1]'s string theoretic dual of large-N thermal QCD-like
theories at finite gauge/string coupling (as part of the `MQGP' limit of [2]),
we discuss the following. First, up to LO in N, using the results of [3], we
show that the local T^3 of [2] is the T^2-invariant sLag of [3] in a resolved
conifold. This, together with the results of [4], shows that for a
(predominantly resolved or deformed) resolved warped deformed conifold, the
local T^3 of [2] in the MQGP limit, is the T^2-invariant sLag of [3] justifying
the construction of the delocalized SYZ type IIA mirror of the type IIB
background of [1]. Then, using the prescription of [5], we obtain the
temperature dependence of the thermal (and electrical) conductivity working up
to leading order in N (the number of D3-branes), and upon comparison with [6]
show that the results mimic a 1+1-dimensional Luttinger liquid with impurities.
Further, including sub-leading non-conformal terms in the metric determined by
M (the number of fractional D-branes = the number of colors = 3 in the IR after
the end of a Seiberg duality cascade), by looking at respectively the scalar,
vector and tensor modes of metric perturbations and using [7]'s prescription of
constructing appropriate gauge-invariant perturbations, we obtain respectively
the speed of sound, the diffusion constant and the shear viscosity \eta (and
\eta/s) including the non-conformal O((g_s M^2) (g_s N_f)/N<<1)-corrections,
N_f being the number of flavor D7-branes.Comment: 1+75 pages, LaTeX; Some corrections in Tc-related calculations,
results unchange
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