Overlayer-induced valence states, and evidence for charge transfer in Na/GaP(110) and Na/GaAs(110): A comparative photoemission study

Author(s):  
D. A. Evans
1991 ◽  
Vol 1 (9) ◽  
pp. 1347-1354 ◽  
Author(s):  
D. Schmeißer ◽  
A. Gonzales ◽  
J. U. von Schütz ◽  
H. Wachtel ◽  
H. C. Wolf

2020 ◽  
Author(s):  
Balázs Kozma ◽  
Attila Tajti ◽  
Baptiste Demoulin ◽  
Róbert Izsák ◽  
Marcel Nooijen ◽  
...  

There are numerous publications on benchmarking quantum chemistry methods for excited states. These studies rarely include Charge Transfer (CT) states although many interesting phenomena in e.g. biochemistry and material physics involve transfer of electron between fragments of the system. Therefore, it is timely to test the accuracy of quantum chemical methods for CT states, as well. In this study we first suggest a set benchmark systems consisting of dimers having low-energy CT states. On this set, the excitation energy has been calculated with coupled cluster methods including triple excitations (CC3, CCSDT-3, CCSD(T)(a)* ), as well as with methods including full or approximate doubles (CCSD, STEOM-CCSD, CC2, ADC(2), EOM-CCSD(2)). The results show that the popular CC2 and ADC(2) methods are much more inaccurate for CT states than for valence states. On the other hand, CCSD seems to have similar systematic overestimation of the excitation energies for both valence and CT states. Concerning triples methods, the new CCSD(T)(a)* method including non-iterative triple excitations preforms very well for all type of states, delivering essentially CCSDT quality results.<br>


RSC Advances ◽  
2019 ◽  
Vol 9 (35) ◽  
pp. 20161-20168
Author(s):  
Rong Zhang ◽  
Bo Xiang ◽  
Lei Xu ◽  
Liru Xia ◽  
Chunhua Lu

Ca-doping affects the overall catalytic efficiency by adjusting the distribution of Co valence states and oxygen vacancies due to the strengthening of the charge transfer between O-2p and Co-3d orbitals upon substitution of Gd by Ca.


2017 ◽  
Vol 46 (5) ◽  
pp. 1606-1617 ◽  
Author(s):  
D. Mikhailova ◽  
N. N. Kuratieva ◽  
Y. Utsumi ◽  
A. A. Tsirlin ◽  
A. M. Abakumov ◽  
...  

The V1−xRexO2 solid solution with 0.03 < x ≤ 0.15 undergoes below 1000 K a phase separation to two isostructural phases with mixed-valence states Re4+/Re6+, while only a single phase exists for x ≤ 0.03 and x ≥ 0.30 with Re6+ and Re4+, respectively.


1994 ◽  
Vol 08 (20) ◽  
pp. 1261-1268 ◽  
Author(s):  
H.I. STARNBERG ◽  
H.E. BRAUER ◽  
P.O. NILSSON ◽  
L.J. HOLLEBOOM ◽  
H.P. HUGHES

We report photoemission studies of the valence band structure of VSe 2 and of VSe2 intercalated with Cs. Pure VSe 2 showed significant band dispersion both perpendicular and parallel to the layers, i.e. the valence band of VSe 2 is 3D in character, confirming self-consistent LAPW band structure calculations. After Cs intercalation the perpendicular band dispersion vanished, while that parallel to the layers remained, showing that the valence band structure had become 2D. The observed changes go far beyond the rigid band model, but are largely understandable in terms of intercalation-induced decoupling of the VSe 2 layers, and charge transfer from the Cs.


1992 ◽  
Vol 45 (11) ◽  
pp. 6321-6324 ◽  
Author(s):  
C. J. Karlsson ◽  
E. Landemark ◽  
Y.-C. Chao ◽  
R. I. G. Uhrberg

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