Collective excitations of $\Lambda$ hypernuclei

Abstract

We discuss low-lying collective excitations of $\Lambda$ hypernuclei using the self-consistent mean-field approaches. We first discuss the deformation properties of $\Lambda$ hypernuclei in the $sd$-shell region. Based on the relativistic mean-field (RMF) approach, we show that the oblate deformation for ${}^{28}$Si nucleus may disappear when a $\Lambda$ particle is added to this nucleus. We then discuss the rotational excitations of ${}_{\Lambda }^{25}$Mg nucleus using the three-dimensional potential energy surface in the deformation plane obtained with the Skyrme-Hartree-Fock method. The deformation of ${}_{\Lambda }^{25}$Mg nucleus is predicted to be slightly reduced due to an addition of $\Lambda$ particle. We demonstrate that this leads to a reduction of electromagnetic transition probability, $B(E2)$, in the ground state rotational band. We also present an application of random phase approximation (RPA) to hypernuclei, and show that a new dipole mode, which we call a soft dipole $\Lambda$ mode, appears in hypernuclei, which can be interpreted as an oscillation of $\Lambda$ particle against the core nucleus.

Comments: 8 pages, 5 figures. A talk given at XI International Conference on Hypernuclear and Strange Particle Physics (HYP2012), Oct. 1-5, 2012, Barcelona, Spain