Abstract
An explicit formula is given relating the effective potential in a finite volumeP(φ)2 quantum field theory to the expected energy density under the constraint of a fixed average filed. In the one phase region, i.e., where the classical potential equals its convex hull and has nonvanishing second derivative, it is shown via a central limit theorem that in the infinite volume limit the effective potential is equal to the constrained energy density, provided ħ is sufficiently small.
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Communicated by K. Osterwalder
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Slade, G. The effective potential as an energy density: The one phase region. Commun.Math. Phys. 104, 573–580 (1986). https://doi.org/10.1007/BF01211065
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DOI: https://doi.org/10.1007/BF01211065