14,544 research outputs found
Wilson-'t Hooft operators in four-dimensional gauge theories and S-duality
We study operators in four-dimensional gauge theories which are localized on
a straight line, create electric and magnetic flux, and in the UV limit break
the conformal invariance in the minimal possible way. We call them Wilson-'t
Hooft operators, since in the purely electric case they reduce to the
well-known Wilson loops, while in general they may carry 't Hooft magnetic
flux. We show that to any such operator one can associate a maximally symmetric
boundary condition for gauge fields on AdS^2\times S^2. We show that Wilson-'t
Hooft operators are classifed by a pair of weights (electric and magnetic) for
the gauge group and its magnetic dual, modulo the action of the Weyl group. If
the magnetic weight does not belong to the coroot lattice of the gauge group,
the corresponding operator is topologically nontrivial (carries nonvanishing 't
Hooft magnetic flux). We explain how the spectrum of Wilson-'t Hooft operators
transforms under the shift of the theta-angle by 2\pi. We show that, depending
on the gauge group, either SL(2,Z) or one of its congruence subgroups acts in a
natural way on the set of Wilson-'t Hooft operators. This can be regarded as
evidence for the S-duality of N=4 super-Yang-Mills theory. We also compute the
one-point function of the stress-energy tensor in the presence of a Wilson-'t
Hooft operator at weak coupling.Comment: 32 pages, latex. v2: references added. v3: numerical factors
corrected, other minor change
A new Determination of the Extragalactic Background of Diffuse Gamma Rays taking into account Dark Matter Annihilation
The extragalactic background (EGB) of diffuse gamma rays can be determined by
subtracting the Galactic contribution from the data. This requires a Galactic
model (GM) and we include for the first time the contribution of dark matter
annihilation (DMA), which was previously proposed as an explanation for the
EGRET excess of diffuse Galactic gamma rays above 1 GeV.
In this paper it is shown that the newly determined EGB shows a
characteristic high energy bump on top of a steeply falling soft contribution.
The bump is shown to be compatible with a contribution from an extragalactic
DMA signal from weakly interacting massive particles (WIMPs) with a mass
between 50 and 100 GeV in agreement with the EGRET excess of the Galactic
diffuse gamma rays and in disagreement with earlier analysis. The remaining
soft contribution of the EGB is shown to resemble the spectra of the observed
point sources in our Galaxy.Comment: 7 pages, 4 figures. Accepted by A&A, made Fig. 4 and table 1
consisten
The supersymmetric interpretation of the EGRET excess of diffuse Galactic gamma rays
Recently it was shown that the excess of diffuse Galactic gamma rays above 1
GeV traces the Dark Matter halo, as proven by reconstructing the peculiar shape
of the rotation curve of our Galaxy from the gamma ray excess. This can be
interpreted as a Dark Matter annihilation signal. In this paper we investigate
if this interpretation is consistent with Supersymmetry. It is found that the
EGRET excess combined with all electroweak constraints is fully consistent with
the minimal mSUGRA model for scalars in the TeV range and gauginos below 500
GeV.Comment: 11 pages, 6 figures, extended version with more figures, as accepted
for publication in Phys. Letters
Supersymmetry and LHC
The motivation for introduction of supersymmetry in high energy physics as
well as a possibility for supersymmetry discovery at LHC (Large Hadronic
Collider) are discussed. The main notions of the Minimal Supersymmetric
Standard Model (MSSM) are introduced. Different regions of parameter space are
analyzed and their phenomenological properties are compared. Discovery
potential of LHC for the planned luminosity is shown for different channels.
The properties of SUSY Higgs bosons are studied and perspectives of their
observation at LHC are briefly outlined.Comment: Lectures given at the 9th Moscow International School of Physics
(XXXIV ITEP Winter School of Physics
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