Chiral limit of nuclear physics

Aurel Bulgac, Gerald A. Miller, and Mark Strikman
Phys. Rev. C 56, 3307 – Published 1 December 1997
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Abstract

We study nuclear physics in the chiral limit (mu, md=0) in which the pion mass vanishes. We find that the deuteron mass is changed little, but that P-wave nucleon-nucleon scattering volumes are infinite. This motivates an investigation of the possibilities that there could be a two-nucleon 3P0 bound state, and that the nuclear matter ground state is likely to be a condensed state of nucleons paired to those quantum numbers. However, the short distance repulsion in the nucleon-nucleon potential is not affected by the chiral limit and prevents such new chiral possibilities. Thus the chiral limit physics of nuclei is very similar to that of nature. Using the chiral limit to simplify QCD sum rule calculations of nuclear matter properties seems to be a reasonable approximation.

  • Received 26 August 1997

DOI:https://doi.org/10.1103/PhysRevC.56.3307

©1997 American Physical Society

Authors & Affiliations

Aurel Bulgac1, Gerald A. Miller1,2,3, and Mark Strikman2,4,5

  • 1Department of Physics, P.O. Box 351560, University of Washington, Seattle, Washington 98195-1560
  • 2Institute for Nuclear Theory, P.O. Box 351550, University of Washington, Seattle, Washington 98195-1550
  • 3Stanford Linear Accelerator Center, Stanford University, Stanford, California 94309
  • 4Pennsylvania State University, University Park, Pennsylvania 16802
  • 5Institute for Nuclear Physics, St. Petersburg, Russia

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Vol. 56, Iss. 6 — December 1997

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