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Isoscalar Giant Resonances in the even-A Pd Isotopes

J. Arroyo, U. Garg, T. Furuno, M. Itoh, H. Shimojo, S. Adachi, H. Akimune, J. Cai, G. Colo, M. Dozono, F. Endo, M. Fujiwara, F. Furukawa, M. N. Harakeh, Y. Hijikata, Y. Honda, G. Hosoya, N. Itakura, K. Kawata, T. Kawabata, N. Kobayashi, Z. Z. Li, Y. Lin, Y. Matsuda, T. Morishita, K. Nakano, Y. F. Niu, T. Okamura, S. Ota, F. Saito, R. Saito, S. Sakajo, K. Sakanashi, H. Shibakita, R. Tsuji, G. Umemoto, A. Yamasaki, S. Yamazaki, T. Yano, K. Yasumura, S. Yonekura, J. Zenihiro

nucl-exarXiv:2608.22109

Abstract

Studies of the isoscalar giant monopole resonance (ISGMR) across the chart of nuclides provide insight into the incompressibility of nuclear matter near saturation density, K(infinity). Such studies had revealed a discrepancy between theoretical approaches: quasiparticle random phase approximation (QRPA) derived from Skyrme interactions reproduce the strength distributions of the ISGMR in the doubly-closed-shell nuclei 90Zr and 208Pb, but their descriptions of strength distributions in open-shell medium-heavy nuclei suggest higher centroid energies should be experimentally observed. The latter nuclei required a smaller K(infinity) and were thus deemed softer. The present work serves to add to this softness discourse by extracting ISGMR strength distributions for 104,106,108,110Pd via 386-MeV inelastic alpha-scattering. The extracted giant resonance strength distributions are consistent with expectations in this isotopic range. Additional Quasiparticle Vibration Coupling (QPVC) effects are included with the QRPA approach and compared to aforementioned ISGMR strength distributions.

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