The C K-edge photoabsorption and 1s core-level photoemission of pentacene (C22H14) free molecules are experimentally measured, and calculated by self-consistent-field and static-exchange approximation ab initio methods. Six nonequivalent C atoms present in the molecule contribute to the C 1s photoemission spectrum. The complex near-edge structures of the carbon K-edge absorption spectrum present two main groups of discrete transitions between 283 and 288?eV photon energy, due to absorption to ?* virtual orbitals, and broader structures at higher energy, involving ?* virtual orbitals. The sharp absorption structures to the ?* empty orbitals lay well below the thresholds for the C 1s ionizations, caused by strong excitonic and localization effects. We can definitely explain the C K-edge absorption spectrum as due to both final (virtual) and initial (core) orbital effects, mainly involving excitations to the two lowest-unoccupied molecular orbitals of ?* symmetry, from the six chemically shifted C 1s core orbitals.
Core-shell photoabsorption and photoelectron spectra of gas-phase pentacene: Experiment and theory / Alagia, M; C., Baldacchini; Betti, Maria Grazia; Bussolotti, F; Carravetta, V; Ekström, U; Mariani, Carlo; Stranges, Stefano. - In: THE JOURNAL OF CHEMICAL PHYSICS. - ISSN 0021-9606. - 122:(2005), pp. 124305-1-124305-6. [10.1063/1.1864852]
Core-shell photoabsorption and photoelectron spectra of gas-phase pentacene: Experiment and theory
BETTI, Maria Grazia;MARIANI, CARLO;STRANGES, Stefano
2005
Abstract
The C K-edge photoabsorption and 1s core-level photoemission of pentacene (C22H14) free molecules are experimentally measured, and calculated by self-consistent-field and static-exchange approximation ab initio methods. Six nonequivalent C atoms present in the molecule contribute to the C 1s photoemission spectrum. The complex near-edge structures of the carbon K-edge absorption spectrum present two main groups of discrete transitions between 283 and 288?eV photon energy, due to absorption to ?* virtual orbitals, and broader structures at higher energy, involving ?* virtual orbitals. The sharp absorption structures to the ?* empty orbitals lay well below the thresholds for the C 1s ionizations, caused by strong excitonic and localization effects. We can definitely explain the C K-edge absorption spectrum as due to both final (virtual) and initial (core) orbital effects, mainly involving excitations to the two lowest-unoccupied molecular orbitals of ?* symmetry, from the six chemically shifted C 1s core orbitals.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.