paper

Polarization of the C cage by the photoelectron, interior static polarization of C by the ion-remainder and atomic-core relaxation in @C photoionization

arXiv:1809.02898

Abstract

Photoionization cross sections, photoelectron angular-asymmetry parameters and photoionization time delays for @C endohedral atoms are studied with account for both the individual and combined effects of dipole static polarization (DSP) of C by the outgoing photoelectron, interior static polarization (ISP) of C by the ion-remainder, , and atomic-core relaxation of the encapsulated atom upon its ionization. It is unraveled that the DSP effect is weak; it changes the phase of confinement-resonant oscillations in , and without generally noticeable changes in their magnitudes, unless concentrates a relatively large part of oscillator strength of the continuum spectrum near threshold. This is counter-intuitive in view of a large dipole static polarizability of C, . Furthermore, it is demonstrated that the DSP effect results in the transmission of a part of oscillator strength of the continuum spectrum of @C into its discrete spectrum. It is shown that the DSP effect is counteracted by ISP. Possible reasons behind the made findings are provided. Photoionization of Xe@C, Ne@C, H@C and some hypothetical C fullerene anions is chosen as a case study. For Xe@C, the role of atomic-core relaxation of the ionized encapsuled Xe-ion-remainder on the photoionization of Xe@C is revealed to be of utter significance, as in free Xe. The random phase approximation with exchange (RPAE) and generalized RPAE were used in the study. The C cage is modelled by a spherical attractive potential of a certain inner radius, thickness and depth. Its dipole static polarization potential is approximated by the Bates dipole static potential.

16 pages, 19 figures, regular paper