A low-energy calculation of 9Be photodisintegration cross section is presented within an ααn cluster approach. The αn and αα contact interactions are derived from cluster effective field theory. The two-body potentials defined in momentum space are regularized by a Gaussian cutoff. The associated low-energy constants are found by comparing the calculated low-energy T matrix with its effective range expansion. A three-body state-dependent potential is also introduced in the model. First, the 9Be three-body binding energy is studied within the nonsymmetrized hyperspherical harmonics method. Then, the low-energy cross section is calculated via the Lorentz integral transform method, focusing on the dominant electric dipole transitions. A twofold evaluation of the nuclear current matrix element is presented, employing both the electric dipole transition operator (Siegert theorem) and the one-body convection current operator. This approach is adopted to allow for a discussion of the effect of the many-body currents.
9Be photodisintegration cross section within cluster effective field theory / Capitani, Y.; Filandri, E.; Ji, C.; Leidemann, W.; Orlandini, G.. - In: PHYSICAL REVIEW C. - ISSN 2469-9985. - 112:6(2025), pp. 1-15. [10.1103/4492-hghr]
9Be photodisintegration cross section within cluster effective field theory
Capitani Y.
;Filandri E.;Leidemann W.;Orlandini G.
2025-01-01
Abstract
A low-energy calculation of 9Be photodisintegration cross section is presented within an ααn cluster approach. The αn and αα contact interactions are derived from cluster effective field theory. The two-body potentials defined in momentum space are regularized by a Gaussian cutoff. The associated low-energy constants are found by comparing the calculated low-energy T matrix with its effective range expansion. A three-body state-dependent potential is also introduced in the model. First, the 9Be three-body binding energy is studied within the nonsymmetrized hyperspherical harmonics method. Then, the low-energy cross section is calculated via the Lorentz integral transform method, focusing on the dominant electric dipole transitions. A twofold evaluation of the nuclear current matrix element is presented, employing both the electric dipole transition operator (Siegert theorem) and the one-body convection current operator. This approach is adopted to allow for a discussion of the effect of the many-body currents.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione



