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Neutralino annihilation toqq¯g

2006/08/31 by V. Barger, Vernon Barger, Wai-Yee Keung +2
Chemistry · Mathematics · Physics and Astronomy · #Annihilation #Chemistry #Combinatorics #Crystallography #Dark Matter and Cosmic Phenomena #Mathematics #Neutralino #Order (exchange) #Particle physics #Particle physics theoretical and experimental studies #Physics #Quantum Chromodynamics and Particle Interactions #Supersymmetry #hep-ph

paper · pdf · doi:10.1103/physrevd.74.075005

published as Phys.Rev.D74:075005,2006 · 13 pages, 1 figure; v2: refs added; v3: version to appear in PRD

arxiv created 2006/10/10 · openalex publication_date 2006/10/16 · arxiv updated 2009/12/01 · openalex created_date 2021/04/13 · openalex updated_date 2026/08/05

Abstract

We compute the cross section for \ensuremathχ\ensuremathχ\ensuremath→qqg at order \ensuremathαs2/M_\stackrel\texttildelowq6 arising from interference between the tree-level and loop-induced processes. This interference term is the same order in \ensuremathαs as \ensuremathχ\ensuremathχ\ensuremath→gg; for mass degenerate squarks M_\stackrel\texttildelowqR=M_\stackrel\texttildelowqL=M_\stackrel\texttildelowq we find vrel\ensuremathσint=[\ensuremath-2m_\ensuremathχ2/3M_\stackrel\texttildelowq2]vrel\ensuremathσ(\ensuremathχ\ensuremathχ\ensuremath→gg).

Citations