| Autor: |
Lukashov SS; Department of Physics, Saint Petersburg State University, SPbSU, 7/9 Universitetskaya nab., St. Petersburg 199034, Russia., Martynov II; Department of Physics, Saint Petersburg State University, SPbSU, 7/9 Universitetskaya nab., St. Petersburg 199034, Russia., Poretsky SA; Department of Physics, Saint Petersburg State University, SPbSU, 7/9 Universitetskaya nab., St. Petersburg 199034, Russia., Pravilov AM; Department of Physics, Saint Petersburg State University, SPbSU, 7/9 Universitetskaya nab., St. Petersburg 199034, Russia., Sivokhina MM; Department of Physics, Saint Petersburg State University, SPbSU, 7/9 Universitetskaya nab., St. Petersburg 199034, Russia. |
| Abstrakt: |
This paper presents the experimental and theoretical analyses of ArICl(IP,v IP ,n IP ) states' population and decay at energies lower than the ArICl(E,v E = 0,n E ) dissociation limit (IP = E0 + , D'2, β1), v IP = 0, 1, and n IP are the quantum numbers of the van der Waals (vdW) modes. We have measured the excitation spectra of the ArICl(E,v E = 0,1,n E → X,v X ,n X ) and ArICl(β,0,n β → A and/or D ' ,v D ' ,n D ' →A ' luminescence as well as luminescence spectra themselves. To construct potential energy surfaces (PESs) for valence (A1, A'2) and ion-pair (E, β, and D') electronic states of the complex, we utilized the intermolecular diatomic-in-molecule perturbation theory first order method. The experimental and calculated spectroscopic characteristics of the T-shaped ArICl valence and E, β states agree well. The ArICl(D') state PES has no vdW levels in the T-shaped configuration, and collinear ArICl(D') binding energy is larger than that of the T-shaped ArICl(β) state. We calculated vibrational state energies and the ArICl(IP → valence states) luminescence excitation spectra, as well as luminescence spectra themselves, by using the Heidelberg MCTDH code. The comparison of the experimental and calculated excitation spectra shows that the latter describe their principal features. The bound-bound ArICl(E,0,n E → X and β,0,n β → A) parts of experimental luminescence spectra are described adequately by the calculated spectra, whereas bound-free ArICl(E,0,n E → X, D', 0, n D' → A') parts are not described since the bound-free transitions occur in repulsive parts of the ArICl(X, A ' PESs, which we cannot describe accurately. |
