Octupole deformation produces only modest changes to transition strengths in giant resonances, while M1 strength is more affected below 8 MeV and the isoscalar E3 response requires explicit removal of the rotational Nambu-Goldstone mode.
Roca-Maza and N
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Bayesian analysis of IVGDR properties in BUU transport simulations with Skyrme functionals constrains the neutron-proton effective mass splitting at saturation density to Δm*_1(ρ0)/m = 0.200 +0.101 -0.094.
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Impact of octupole deformation on the nuclear electromagnetic response
Octupole deformation produces only modest changes to transition strengths in giant resonances, while M1 strength is more affected below 8 MeV and the isoscalar E3 response requires explicit removal of the rotational Nambu-Goldstone mode.
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Constraining neutron-proton effective mass splitting through nuclear giant dipole resonance within transport approach
Bayesian analysis of IVGDR properties in BUU transport simulations with Skyrme functionals constrains the neutron-proton effective mass splitting at saturation density to Δm*_1(ρ0)/m = 0.200 +0.101 -0.094.