Nuclear fusion in a dense plasma
arXiv:1002.0872 · doi:10.1103/PhysRevLett.104.191103
Abstract
The standard theory of nuclear fusion rates in a strongly interacting plasma can be (correctly) derived only when the energy release, Q, is large compared to other energies in the problem. We exhibit a result for rates that provides a basis for calculating the finite Q corrections. Crude estimates indicate a significant defect in the conventional results for some regions of high density and strong plasma coupling. We also lay some groundwork for a path integral calculation of the new effects.
Final version to appear in Phys. Rev. Lett.
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