Asymmetry in the dissociation of O2in the core hole excited states

1989 ◽  
Vol 22 (18) ◽  
pp. L517-L521 ◽  
Author(s):  
N Saito ◽  
I H Suzuki
Keyword(s):  
2020 ◽  
Vol 22 (3) ◽  
pp. 1400-1408
Author(s):  
Vincent V. Duong ◽  
David Prendergast ◽  
Alexander L. Ayzner

Resonant photoemission measurements show that ultrafast electron dynamics in core-excited states of large organic semiconductors depends on both the nature of the core-hole and the proximal chemical environment.


1994 ◽  
Vol 100 (11) ◽  
pp. 8550-8553 ◽  
Author(s):  
Kaidee Lee ◽  
Dae Young Kim ◽  
Chien‐I Ma ◽  
David M. Hanson

Author(s):  
D. Koulentianos ◽  
S. Carniato ◽  
R. Püttner ◽  
J. B. Martins ◽  
O. Travnikova ◽  
...  

A K−2V photoelectron spectrum of the CO molecule, showing several core-ionized core-excited states, has been recorded and the different spectral features have been interpreted in terms of their direct or conjugate nature.


2019 ◽  
Vol 26 (1) ◽  
pp. 152-158 ◽  
Author(s):  
Ondřej Šipr ◽  
Wilayat Khan ◽  
Yves Joly ◽  
Ján Minár

Ca and S K-edge spectra of CaS are calculated by the full-potential Green's function multiple-scattering method, by the FLAPW method and by the finite-difference method. All three techniques lead to similar spectra. Some differences remain close to the edge, both when comparing different calculations with each other and when comparing the calculations with earlier experimental data. Here it is found that using the full potential does not lead to significant improvement over the atomic spheres approximation and that the effect of the core hole can be limited to the photoabsorbing atom alone. Doping CaS with Eu will not affect the Ca and S K-edge XANES of CaS significantly but may give rise to a pre-edge structure not present for clean CaS.


2019 ◽  
Vol 74 (9) ◽  
pp. 743-749
Author(s):  
Kai Kai Li ◽  
Lin Zhuo ◽  
Yan Sun ◽  
Bing Cong Gou

AbstractBy systematic Rayleigh–Ritz variation calculations, the energies are reported for the core-excited states 1s2s2p2 5P and 1s2p3 5So in the Be-like isoelectronic sequence (Z = 11–20). Energy corrections, including the restricted variational method, mass polarisation, and relativistic effect, are considered to improve the accuracy of energy. The oscillator strengths and transition wavelength between these states are also reported. Computational data on hyperfine structures presented in this paper are calculated for the first time.


1977 ◽  
Vol 99 (24) ◽  
pp. 8120-8121 ◽  
Author(s):  
D. T. Clark ◽  
B. J. Cromarty ◽  
L. Colling

2013 ◽  
Vol 27 (16) ◽  
pp. 1330012 ◽  
Author(s):  
A. KOTANI

We consider two different resonant X-ray emission spectra for Ce compounds: Ce 3d to 2p X-ray emission (denoted by 3d-RXES) and valence to 2p X-ray emission (v-RXES), both of which follow the Ce 2p to 5d resonant excitation. We propose that the comparison of the 3d- and v-RXES spectra is a new powerful method of directly detecting the core-hole effect in the final state of Ce L 3 X-ray absorption spectra (XAS). We applied this method to recent experimental RXES spectra for CeO 2 and CeFe 2, and showed unambiguously that the core-hole effect should be essential in the XAS of both materials. This result is confirmed by theoretical calculations, which reproduce well the experimental RXES and XAS spectra. We conclude that the ground state of CeO 2 is in the mixed state of 4f0 and [Formula: see text] configurations, where [Formula: see text] is a ligand hole, instead of a pure 4f0 configuration which was proposed recently by first-principles energy band calculations. Also, we conclude that the double peaks observed in L 3 XAS of CeFe 2 are caused by the 4f0 and 4f1 configurations, which are mixed in the ground state but separated in energy by the large core-hole potential in the final state of XAS.


1994 ◽  
Vol 348 ◽  
Author(s):  
Andrey N. Belsky ◽  
Irina A. Kamenskikh ◽  
Andrey N. Vasil'ev ◽  
Alexander V. Gektin ◽  
Christian Pedrini ◽  
...  

ABSTRACTThe Auger decay of a core hole results in appearance of several strongly correlated excitations. This excited region strongly polarizes the lattice and thus the defect creation is possible. In all cases the core hole causes the strong local perturbation of electronic and lattice subsystems. The creation of such excited region with mutual relaxation of correlated electrons and holes can result in the increase of the efficiency of energy transfer to activators, acceleration of the luminescence kinetics, and the appearance of radiation-induced luminescence centers.


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