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    Isoscalar giant resonances in the even-A Pd isotopes

    J. Arroyo1,*, U. Garg1,†, T. Furuno2,3, M. Itoh4, H. Shimojo2, S. Adachi4, H. Akimune5, J. Cai6, G. Colò7,8 et al.

    M. Dozono9, F. Endo6, M. Fujiwara6, F. Furukawa6, M. N. Harakeh10, Y. Hijikata9, Y. Honda2, G. Hosoya4, N. Itakura6, K. Kawata6, T. Kawabata2, N. Kobayashi6, Z. Z. Li (李征征)11,12, Y. Lin2, Y. Matsuda6, T. Morishita5, K. Nakano5, Y. F. Niu (牛一斐)13, T. Okamura2, S. Ota6, F. Saito5, R. Saito4, S. Sakajo2, K. Sakanashi2, H. Shibakita6, R. Tsuji9, G. Umemoto5, A. Yamasaki5, S. Yamazaki4, T. Yano9, K. Yasumura5, S. Yonekura4, and J. Zenihiro9

    • *Contact author: jarroyo1@nd.edu
    • †Contact author: garg@nd.edu

    Phys. Rev. C 114, 044306 – Published 5 October, 2026

    DOI: https://doi.org/10.1103/r21q-4789

    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∞. 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 Zr90 and Pb208, 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∞ and were thus deemed “softer.” The present work serves to add to this “softness” discourse by extracting ISGMR strength distributions for Pd104,106,108,110 via 386-MeV inelastic α 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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