
arXiv: 1802.02883
The Pauli–Villars regularization procedure confirms and sharpens the conclusions reached previously by covariant point splitting. The divergences in the stress tensor of a quantized scalar field interacting with a static scalar potential are isolated into a three-parameter local, covariant functional of the background potential. These divergences can be naturally absorbed into coupling constants of the potential, regarded as a dynamical object in its own right; here, this is demonstrated in detail for two different models of the field-potential coupling. There is a residual dependence on the logarithm of the potential, reminiscent of the renormalization group in fully-interacting quantum field theories; these terms are finite, but numerically dependent on an arbitrary mass or length parameter, which is purely a matter of convention. This work is one step in a program to elucidate boundary divergences by replacing a sharp boundary by a steeply-rising smooth potential.
High Energy Physics - Theory, Quantum Physics, potential, FOS: Physical sciences, scalar field, General Relativity and Quantum Cosmology (gr-qc), Mathematical Physics (math-ph), Pauli-Villars, point splitting, General Relativity and Quantum Cosmology, vacuum energy; renormalization; Pauli–Villars; point splitting; boundary; potential; scalar field, renormalization, boundary, vacuum energy, High Energy Physics - Theory (hep-th), Quantum Physics (quant-ph), Mathematical Physics, Nonperturbative methods of renormalization applied to problems in quantum field theory
High Energy Physics - Theory, Quantum Physics, potential, FOS: Physical sciences, scalar field, General Relativity and Quantum Cosmology (gr-qc), Mathematical Physics (math-ph), Pauli-Villars, point splitting, General Relativity and Quantum Cosmology, vacuum energy; renormalization; Pauli–Villars; point splitting; boundary; potential; scalar field, renormalization, boundary, vacuum energy, High Energy Physics - Theory (hep-th), Quantum Physics (quant-ph), Mathematical Physics, Nonperturbative methods of renormalization applied to problems in quantum field theory
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