Tadahiro Miyao, Herbert Spohn
JOURNAL OF MATHEMATICAL PHYSICS 50 7 072103 2009年07月
[査読有り][通常論文] The retarded van der Waals potential, as first obtained by Casimir and Polder, is usually computed on the basis of nonrelativistic quantum electrodynamics . The Hamiltonian describes two infinitely heavy nuclei, charge e, separated by a distance R and two spinless electrons, charge -e, nonrelativistically coupled to the quantized radiation field. Casimir and Polder used the dipole approximation and small coupling to the Maxwell field. We employ here the full Hamiltonian and determine the asymptotic strength of the leading -R(-7) potential, which is valid for all e. Our computation is based on a path integral representation and expands in 1/R, rather than in e.