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The structure of the “condensed” phase of a finite nucleus is investigated by a HF calculation with a HO-type potential, one-pion-exchange potential and one-rho-meson-exchange potential. The pion field expectation value is also calculated from this nuclear source wave function and compared with the pion field of the normal phase. The time-dependent Schroedinger equation is solved for a certain approximated model of a heavy-ion reaction to see the dynamical growth of the pion field expectation value and its behaviour on such a time scale. The growth of the pion field itself is also investigated to see whether it is a normal growth or that of the condensed phase.  相似文献   

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