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Related papers: Neutralino Annihilation to Gluons

200 papers

According to the helicity conservation (HCns) theorem, the sum of the helicities should be conserved, in any 2-to-2 processes in MSSM with R-parity conservation, at high energies; i.e. all amplitudes violating this rule, must vanish…

High Energy Physics - Phenomenology · Physics 2011-09-23 G. J. Gounaris , J. Layssac , F. M. Renard

Electron-positron annihilation into hadrons plus an energetic photon from initial state radiation allows the hadronic cross-section to be measured over a wide range of energies. The full next-to-leading order QED corrections for the…

High Energy Physics - Phenomenology · Physics 2011-09-13 G. Rodrigo , H. Czyz , J. H. Kuhn , M. Szopa

We investigate if the gamma ray halo, for which recent evidence has been found in EGRET data, can be explained by neutralino annihilations in a clumpy halo. We find that the measured excess gamma ray flux can be explained through a moderate…

Astrophysics · Physics 2009-10-30 L. Bergstrom , J. Edsjo , P. Ullio

We present the calculation at next-to-leading order (NLO) in alpha_s of the fragmentation function of a gluon into heavy quarkonium in the color-octet spin-singlet S-wave channel. To calculate the real NLO corrections, we adapt a…

High Energy Physics - Phenomenology · Physics 2019-02-20 Pierre Artoisenet , Eric Braaten

Recent advances in N-body simulations of cold dark matter halos point to a substantial density enhancement near the center. This means that, e.g., the $\gamma$ ray signals from neutralino dark matter annihilations would be significantly…

Astrophysics · Physics 2010-11-30 L. Bergstrom , P. Ullio , J. Buckley

Strange quark contributions to the neutrino (antineutrino) scattering are investigated on the elastic neutrino-nucleon scattering and the neutrino-nucleus scattering for 12C target in the quasi-elastic region on the incident energy of 500…

Nuclear Theory · Physics 2015-05-13 Myung-Ki Cheoun , K. S. Kim

Decays of the lightest neutralino are studied in R_p-violating models with operators lambda^{prime} L Q D^c and lambda L L E^c involving third-generation matter fields and with dominant lambda^{prime} and lambda couplings. Generalizations…

High Energy Physics - Phenomenology · Physics 2009-11-07 F. Borzumati , R. M. Godbole , J. L. Kneur , F. Takayama

In my diploma thesis I calculate a lower mass bound of the lightest nutralino assuming an additional supernova cooling mechanism. I consider elektron-positron annihilation and nucleon-nucleon bremsstrahlung as cooling processes. These…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ulrich Langenfeld

We calculate the supersymmetric QCD corrections in order $\alpha_s$ to the decays $\squark_i \to q' \chargino_j$ (i,j = 1,2) and $\squark_i \to q \neutralino_k$ (k = 1,...4) within the Minimal Supersymmetric Standard Model. In particular we…

High Energy Physics - Phenomenology · Physics 2011-01-27 S. Kraml , H. Eberl , A. Bartl , W. Majerotto , W. Porod

We analyze how the measurements of the low-energy spectrum of cosmic antiprotons can provide information on relic neutralinos. The analysis is focused on the light neutralinos which emerge in supersymmetric schemes where gaugino-mass…

High Energy Physics - Phenomenology · Physics 2009-11-11 A. Bottino , F. Donato , N. Fornengo , P. Salati

We compare the rate for elastic scattering of neutralinos from various nuclei with the flux of upward muons induced by energetic neutrinos from neutralino annihilation in the Sun and Earth. We consider both scalar and axial-vector…

High Energy Physics - Phenomenology · Physics 2008-11-26 Marc Kamionkowski , Kim Griest , Gerard Jungman , Bernard Sadoulet

One of the main channels which allows for a large rate of neutralino dark matter annihilation in the early Universe is via the pseudoscalar Higgs A-resonance. In this case, the measured dark matter abundance can be obtained in the minimal…

High Energy Physics - Phenomenology · Physics 2012-11-12 Howard Baer , Alexander Belyaev , Chung Kao , Patrik Svantesson

We calculate the NLO corrections for the gluon fragmentation functions to a heavy quark-antiquark pair in ${^{1}\hspace{-0.6mm}S_{0}^{[1]}}$ or ${^{1}\hspace{-0.6mm}S_{0}^{[8]}}$ state within NRQCD factorization. We use integration-by-parts…

High Energy Physics - Phenomenology · Physics 2019-05-22 Peng Zhang , Chen-Yu Wang , Xiao Liu , Yan-Qing Ma , Ce Meng , Kuang-Ta Chao

The determination of the full SUSY QCD corrections to the production of squarks and gluinos at hadron colliders is reviewed. The inclusion of the NLO corrections stabilizes the theoretical predictions of the various production cross…

High Energy Physics - Phenomenology · Physics 2007-05-23 Michael Spira

We consider a model for neutralino dark matter candidates arising in anomaly-mediated supersymmetry breaking schemes, and examine its testability through the search for exotic cosmic rays produced by neutralino pair annihilations in the…

High Energy Physics - Phenomenology · Physics 2010-02-03 Piero Ullio

We consider supersymmetric scenarios, compatible with all cosmological and phenomenological requirements, where the lightest SUSY particles (LSPs) are the neutralino and a quasi degenerate gluino. We study the neutralino relic abundance,…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. Profumo , C. E. Yaguna

We argue that high gluon density effects at small $x$ are important for the calculation of ultra-high energy neutrino nucleon cross sections due to the phenomenon of geometric scaling. We calculate the cross section for $\nu N \to \mu X$,…

High Energy Physics - Phenomenology · Physics 2014-11-17 Jamal Jalilian-Marian

We revisit the properties of positron cloud in quark nugget (QN) model of dark matter (DM). In this model, dark matter particles are represented by compact composite objects composed of a large number of quarks or antiquarks with total…

High Energy Physics - Phenomenology · Physics 2021-09-29 V. V. Flambaum , I. B. Samsonov

We calculate the cross sections for neutrino interactions with (isoscalar) nuclear targets in the energy domain all the way up to 10^12 GeV. Small x QCD effects are included by using a unified BFKL/DGLAP formalism which embodies non-leading…

Astrophysics · Physics 2009-10-31 J. Kwiecinski , A. D. Martin , A. Stasto

A sub-component of dark matter with a short collision length compared to a planetary size leads to efficient accumulation of dark matter in astrophysical bodies. We analyze possible neutrino signals from the annihilation of such dark matter…

High Energy Physics - Phenomenology · Physics 2024-01-15 Maxim Pospelov , Anupam Ray