Abstract

We discuss some interesting aspects of the Q\rm Q-ball formation during the early oscillations of the flat directions. These oscillations are triggered by the running of soft (mass)2({\rm mass})^2 stemming from the nonzero energy density of the Universe. However, this is quite different from the standard Q\rm Q-ball formation. The running in presence of gauge and Yukawa couplings becomes strong if m1/2/m0m_{1/2}/m_0 is sufficiently large. Moreover, the Q\rm Q-balls which are formed during the early oscillations constantly evolve, due to the redshift of the Hubble-induced soft mass, until the low-energy supersymmtery breaking becomes dominant. For smaller m1/2/m0m_{1/2}/m_0, Q\rm Q-balls are not formed during early oscillations because of the shrinking of the instability band due to the Hubble expansion. In this case the Q\rm Q-balls are formed only at the weak scale, but typically carry smaller charges, as a result of their amplitude redshift. Therefore, the Hubble-induced corrections to the flat directions give rise to a successful Q\rm Q-ball cosmology.Comment: 7 revtex pages, few references corrected and added, final version to appear in Phys. Rev.

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