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A quantum system which can tunnel, at T=0, out of a metastable state and whose interaction with its environment is adequately described in the classically accessible region by a phenomenological friction coefficient, is considered. By only assuming that the environment response is linear, it is found that dissipation multiplies the tunneling probability by the factor exp-A{ () ^2}, where is the "distance under the barrier" and A is a numerical factor which is generally of order unity.
Caldeira et al. (Mon,) studied this question.