Answers are grounded in this paper and cite their sources.
Recently it has been realized that the production and decay processes of charginos, neutralinos, and sleptons receive corrections which grow like logm_ ̃ \~q for large m_ ̃ \~q. In this paper we calculate the chargino pair production cross section at e⁺e^- colliders with quark-squark loop corrections. We introduce a novel formulation, where the one-loop amplitude is reorganized into two parts. One part is expressed in terms of the ``effective'' chargino coupling g_e ̃ \~ν ̃ \~W and mixing matrices UP,VP, and includes all O(logm_ ̃ \~q) corrections, while the other decouples for large m_ ̃ \~q. The form of the one-loop cross section then becomes physically transparent. Our formulation can be easily extended to other loops and processes. Numerically, we find significant corrections due to the effective t-channel coupling g_e ̃ \~ν ̃ \~W, for gaugino-like charginos. In the mixed region, where the chargino has large gaugino and Higgsino components, the corrections due to (UP,VP) are also significant. Our numerical results disagree with a previous calculation. We reexamine previous studies of the determination of g_e ̃ \~ν ̃ \~W through the measurement of the chargino production cross section. We point out that a previous study, which claimed that the measurement suffers large systematic errors, was performed at a ``pessimistic'' point in MSSM parameter space. We provide reasons why the systematic errors are not a limiting factor for generic parameter choices.
No takes yet. Share an insight, caveat, or question.
Kiyoura et al. (1998) studied this question.
Synapse has enriched 10 related papers. Consider them for comparative context: