For a U(1)-charged scalar, the Euclidean bounce for vacuum decay loses O(4) symmetry at finite charge, lowers the barrier and increases the rate, while charge rearrangement imposes a subluminal terminal velocity on the expanding bubble.
Non-Perturbative Production of Multi-Boson States and Quantum Bubbles
1 Pith paper cite this work. Polarity classification is still indexing.
abstract
The amplitude of production of $n$ on-mass-shell scalar bosons by a highly virtual field $\phi$ is considered in a $\lambda \phi^4$ theory with weak coupling $\lambda$ and spontaneously broken symmetry. The amplitude of this process is known to have an $n!$ growth when the produced bosons are exactly at rest. Here it is shown that for $n \gg 1/\lambda$ the process goes through `quantum bubbles', i.e. quantized droplets of a different vacuum phase, which are non-perturbative resonant states of the field $\phi$. The bubbles provide a form factor for the production amplitude, which rapidly decreases above the threshold. As a result the probability of the process may be heavily suppressed and may decrease with energy $E$ as $\exp (-const \cdot E^a)$, where the power $a$ depends on the number of space dimensions. Also discussed are the quantized states of bubbles and the amplitudes of their formation and decay.
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Globally Charged Vacuum Decay
For a U(1)-charged scalar, the Euclidean bounce for vacuum decay loses O(4) symmetry at finite charge, lowers the barrier and increases the rate, while charge rearrangement imposes a subluminal terminal velocity on the expanding bubble.