Constraining the Selectron Mass in the Process e^- + gamma --> neutralino_1 +selectron_{L/R}^- --> e^- + 2 neutralino_1

Details Constraining the Selectron Mass in the Process e^- + gamma --> neutralino_1 +selectron_{L/R}^- --> e^- + 2 neutralino_1 Constraining the Selectron Mass in the Process e^- + gamma --> neutralino_1 +selectron_{L/R}^- --> e^- + 2 neutralino_1

1999-10-28

arxiv.org/abs/hep-ph/9910528v1

Acta Phys.Polon.B30:3417-3421,1999

Physics

High Energy Physics

High Energy Physics - Phenomenology

5 pages, LaTeX, 4 ps figures, uses appolb.cls (included); talk presented at the XXIII School of Theoretical Physics, Ustron, P

Scientific paper

With the process $e^-\gamma \to \tilde{\chi}_1^0 \tilde{e}_{L/R}^- \to e^-
\tilde{\chi}_1^0 \tilde{\chi}_1^0$ it is possible to constrain selectron masses
above the kinematical limit of the pair production process in $e^+e^-$
colliders. We investigate these mass ranges and discuss the possibility to test
the renormalization group equations for the selectron masses.

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