Abstract

Relativistic nuclear response theory is formulated for the proton–neutron pairing, or deuteron transfer, channel. The approach is based on the meson–nucleon Lagrangian of Quantum Hadrodynamics (QHD) and advances the relativistic field theory to connect consistently the high-energy scale of heavy mesons, the medium-energy range of the pion and the low-energy domain of emergent collective vibrations (phonons) in a parameter-free way. Mesons and phonons build up the in-medium nucleon–nucleon interaction in spin–isospin transfer channels, in particular, the phonon-exchange part takes care of the leading-order retardation effects. In this framework, we explore Jπ=0+ and Jπ=1+ channels of the nuclear response to the proton–neutron pair removal and addition in 56Ni and 100Sn with a special focus on the lowest (soft) modes as precursors of deuteron condensate and candidates for being the mediators of the proton–neutron pairing interaction.

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