Abstract
Functional integral representation of the nuclear many-body grand partition function: A. K. Kerman, Center for Theoretical Physics, Laboratory for Nuclear Science and Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, and T. Troudet, Institute for Theoretical Physics, University of California at Santa Barbara, Santa Barbara, California 93106, and W. K. Kellogg Radiation Laboratory, California Institute of Technology, Pasadena,
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