In this study, the fully self-consistent Hartree–Fock (HF)-based random phase approximation (RPA) calculations were done for the 40Ca\documentclass[12pt]{minimal}
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\begin{document}$$^{40}\hbox {Ca}$$\end{document} and 48Ca\documentclass[12pt]{minimal}
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\begin{document}$$^{48}\hbox {Ca}$$\end{document} nuclei using 20 Skyrme-type interactions: KDE0, KDE0v1, SLy4, SLy5, SLy6, SK255, SKI2, SKI3, SKI5, SKM, SKMP, SKP, LNS, SGII, RAPT, SV-bas, SV-m56-O, SV-m64-O, SV-min and T6. Having a large number of Skyrme-force parameterisations requires a continuous search for the best for describing the experimental data. To examine our results, we compared the strength functions S(E), the charge density distribution and centroid energies ECEN\documentclass[12pt]{minimal}
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\begin{document}$$E_{\mathrm{CEN}}$$\end{document} of the isoscalar giant monopole resonance (ISGMR), Jπ=0+\documentclass[12pt]{minimal}
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\begin{document}$$J^{\pi } = 0^{+}$$\end{document}, T=0\documentclass[12pt]{minimal}
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\begin{document}$$T = 0$$\end{document}, the isovector giant dipole resonance (IVGDR), Jπ=1-\documentclass[12pt]{minimal}
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\begin{document}$$J^{\pi } = 1^{-}$$\end{document}, T=1\documentclass[12pt]{minimal}
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\begin{document}$$T = 1$$\end{document}, and isoscalar giant quadrupole resonance (ISGQR), Jπ=2+\documentclass[12pt]{minimal}
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\begin{document}$$J^{\pi } = 2^{+}$$\end{document}, T=0\documentclass[12pt]{minimal}
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\begin{document}$$T = 0$$\end{document} with the available experimental data. Moreover, we discussed the sensitivities of the centroid energy m1/m0\documentclass[12pt]{minimal}
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\begin{document}$$m_{1}/m_{0}$$\end{document} and moment m1\documentclass[12pt]{minimal}
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\begin{document}$$m_{1}$$\end{document} of the S(E) to the bulk properties of nuclear matter (NM), such as KNM\documentclass[12pt]{minimal}
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\begin{document}$$K_\mathrm{NM}$$\end{document}, the effective mass m* / m and the enhancement factor κ\documentclass[12pt]{minimal}
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\begin{document}$$\kappa $$\end{document} .
