Q Ball formation in the gravity mediated SUSY breaking scenario
By S. Kasuya, M. Kawasaki. 2000
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We study the formation of Q balls which are made of flat directions that appear in the supersymmetric extension of the standard model in the context of gravity-mediated supersymmetry breaking. The full nonlinear calculations for the dynamics of the complex scalar field are made. Since the scalar potential in this model is flatter than ${\ensuremath{\varphi}}^{2},$ we have found that fluctuations develop and go nonlinear to form nontopological solitons, Q balls. The size of a Q ball is determined by the most amplified mode, which is completely determined by the model parameters. On the other hand, the charge of Q balls depends linearly on the initial charge density of the Affleck-Dine (AD) field. Almost all the charges are absorbed into Q balls, and only a tiny fraction of the charges is carried by a relic AD field. It may lead to some constraints on the baryogenesis and/or parameters in the particle theory. The peculiarity of gravity mediation is the moving Q balls. This results in collisions between Q balls. It may increase the charge of the Q balls, and change its fate.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/463d91264d56720a8d8030aed21f91b583c8375a
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Citations in the corpus
- Origin of the matter-antimatter asymmetry (2003, methodology): “Numerical analyses (Kasuya and Kawasaki, 2000a, 2000b, 2001; Enqvist et al., 2001), which can trace the evolution of unstable modes beyond the linear regime, have shown that fragmentation of the condensate is a generic phenomenon (see Fig.”
- Analytic description of primordial black hole formation from scalar field fragmentation (2019, background): “the standard probability theory result for a collection of Niid variables with a Gaussian distribution. The field fragmentation process is stochastic, as supported by numerous simulation results (e.g. [40,64,65]). Hence, we can infer the soliton probability distribution within a given volume, P(N|V),”