Abstract
LetH 0≧0 be a self-adjoint operator acting in a spaceL 2(M, μ). It is assumed thatH 0 e=0, wheree is strictly positive, and that exp(−tH 0) is positivity preserving fort≧0. LetV be a real function onM such that its positive part is inL 2(M,e 2μ) and its negative part is relatively small with respect toH 0. ThenH=H 0+V is essentially self-adjoint on the intersection of the domains ofH 0 andV. This result is applied to Schrödinger operators and to quantum field Hamiltonians.
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Faris, W.G. Essential self-adjointness of operators in ordered hilbert space. Commun.Math. Phys. 30, 23–34 (1973). https://doi.org/10.1007/BF01646685
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DOI: https://doi.org/10.1007/BF01646685