718 research outputs found
White dwarf axions, PAMELA data, and flipped-SU(5)
Recently, there are two hints arising from physics beyond the standard model.
One is a possible energy loss mechanism due to emission of very weakly
interacting light particles from white dwarf stars, with a coupling strength ~
0.7x10^{-13}, and another is the high energy positrons observed by the PAMELA
satellite experiment. We construct a supersymmetric flipped-SU(5) model,
SU(5)xU(1)_X with appropriate additional symmetries,
[U(1)_H]_{gauge}x[U(1)_RxU(1)_\Gamma]_{global}xZ_2, such that these are
explained by a very light electrophilic axion of mass 0.5 meV from the
spontaneously broken U(1)_\Gamma and two component cold dark matters from Z_2
parity. We show that in the flipped-SU(5) there exists a basic mechanism for
allowing excess positrons through the charged SU(2) singlet leptons, but not
allowing anti-proton excess due to the absence of the SU(2) singlet quarks. We
show the discovery potential of the charged SU(2) singlet E at the LHC
experiments by observing the electron and positron spectrum. With these
symmetries, we also comment on the mass hierarchy between the top and bottom
quarks.Comment: 13 pages and 2 figure
Gamma-ray and synchrotron emission from neutralino annihilation in the Large Magellanic Cloud
We calculate the expected flux of gamma-ray and radio emission from the LMC
due to neutralino annihilation. Using rotation curve data to probe the density
profile and assuming a minimum disk, we describe the dark matter halo of the
LMC using models predicted by N-body simulations. We consider a range of
density profiles including the NFW profile, a modified NFW profile proposed by
Hayashi et al.(2003) to account for the effects of tidal stripping, and an
isothermal sphere with a core. We find that the gamma-ray flux expected from
these models may be detectable by GLAST for a significant part of the
neutralino parameter space. The prospects for existing and upcoming Atmospheric
Cherenkov Telescopes are less optimistic, as unrealistically long exposures are
required for detection. However, the effects of adiabatic compression due to
the baryonic component may improve the chances for detection by ACTs. The
maximum flux we predict is well below EGRET's measurements and thus EGRET does
not constrain the parameter space. The expected synchrotron emission generally
lies below the observed radio emission from the LMC in the frequency range of
19.7 to 8550 MHz. As long as <2x 10^-26 cm^3 s^-1 for a neutralino
mass of 50 GeV, the observed radio emission is not primarily due to neutralinos
and is consistent with the assumption that the main source is cosmic rays. We
find that the predicted fluxes, obtained by integrating over the entire LMC,
are not very strongly dependent on the inner slope of the halo profile, varying
by less than an order of magnitude for the range of profiles we considered.Comment: 24 pages, 5 figures; detailed discussion of how the neutralino
induced signals compare with the cosmic-ray induced ones was added. Main
conclusions unchanged. Matches accepted version, to appear in Astroparticle
Physic
Dark Matter Evidence, Particle Physics Candidates and Detection Methods
The problem of the dark matter in the universe is reviewed. A short history
of the subject is given, and several of the most obvious particle candidates
for dark matter are identified. Particular focus is given to weakly
interacting, massive particles (WIMPs) of which the lightest supersymmetric
particle is an interesting special case and a usful template. The three
detection methods: in particle accelerators, by direct detection of scattering
in terrestrial detectors, and indirect detection of products from dark matter
particle annihilation in the galactic halo, are discussed and their
complementarity is explained. Direct detection experiments have revealed some
possible indications of a dark matter signal, but the situation is quite
confusing at the moment. Very recently, also indirect detection has entered a
sensitivity region where some particle candidates could be detectable. Indeed,
also here there are some (presently non-conclusive) indications of possible
dark matter signals, like an interesting structure at 130 GeV gamma-ray energy
found in publicly available data from the Fermi-LAT space detector. The future
of the field will depend on whether WIMPs are indeed the dark matter, something
that may realistically be probed in the next few years. If this exciting
scenario turns out to be true, we can expect a host of other, complementary
experiments in the coming decade. If it is not true, the time scale and methods
for detection will be much more uncertain.Comment: To be published in Annalen der Physik special issue DARK MATTER
edited by M. Bartelmann and V. Springel; Ann.Phys. (Berlin) 524, (2012
SNOC: a Monte-Carlo simulation package for high-z supernova observations
We present a Monte-Carlo package for simulation of high-redshift supernova
data, SNOC. Optical and near-infrared photons from supernovae are ray-traced
over cosmological distances from the simulated host galaxy to the observer at
Earth. The distances to the sources are calculated from user provided
cosmological parameters in a Friedmann-Lemaitre universe, allowing for
arbitrary forms of ``dark energy''. The code takes into account gravitational
interactions (lensing) and extinction by dust, both in the host galaxy and in
the line-of-sight. The user can also choose to include exotic effects like a
hypothetical attenuation due to photon-axion oscillations. SNOC is primarily
useful for estimations of cosmological parameter uncertainties from studies of
apparent brightness of Type Ia supernovae vs redshift, with special emphasis on
potential systematic effects. It can also be used to compute standard
cosmological quantities like luminosity distance, lookback time and age of the
universe in any Friedmann-Lemaitre model with or without quintessence.Comment: 16 pages, 3 figure
Particle Dark Matter Physics: An Update
This write--up gives a rather elementary introduction into particle physics
aspects of the cosmological Dark Matter puzzle. A fairly comprehensive list of
possible candidates is given; in each case the production mechanism and
possible ways to detect them (if any) are described. I then describe detection
of the in my view most promising candidates, weakly interacting massive
particles or WIMPs, in slightly more detail. The main emphasis will be on
recent developments.Comment: Invited talk at the 5th Workshop on Particle Physics Phenomenology,
Pune, India, January 1998; 21 pages, LaTeX with equation.st
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