scholarly journals All-Electron Gaussian-Based G0W0 for Valence and Core Excitation Energies of Periodic Systems

Author(s):  
Tianyu Zhu ◽  
Garnet Kin-Lic Chan
2014 ◽  
Vol 23 (08) ◽  
pp. 1450037
Author(s):  
Y. Y. Cheng ◽  
S. Q. Zhang ◽  
X. Q. Li ◽  
H. Hua ◽  
C. Xu ◽  
...  

Combining the new spectroscopy results of 144 Tb and previous spectroscopy studies of neighboring nuclei, a systematic investigation on the low-lying spectra in N = 78 ~ 80 isotones is performed. Good systematics have been found for the coupling patterns which couple the odd nucleon(s), such as πh11/2, [Formula: see text], to the 2+, 4+, 6+ and 3- core excitations. It is found that the relative excitation energies of the states formed by coupling h11/2 proton(s) to the 2+, 4+ core excitations are pushed up, in contrast with those formed by coupling h11/2 neutron hole(s) to the 2+, 4+ core excitations, which are pulled down. According to the systematics, the interpretation that the 17/2+ states observed in 141 Sm and 143 Gd are the fully aligned member of coupling the odd h11/2 neutron hole to the octupole 3- core excitation, is explored to the isotones 145 Dy , 142 Eu , and 144 Tb .


2017 ◽  
Vol 146 (14) ◽  
pp. 144109 ◽  
Author(s):  
Ida-Marie Høyvik ◽  
Rolf Heilemann Myhre ◽  
Henrik Koch

2004 ◽  
Vol 121 (21) ◽  
pp. 10339-10345 ◽  
Author(s):  
Osamu Takahashi ◽  
Lars G. M. Pettersson

Author(s):  
R.D. Leapman ◽  
P. Rez ◽  
D.F. Mayers

Microanalysis by EELS has been developing rapidly and though the general form of the spectrum is now understood there is a need to put the technique on a more quantitative basis (1,2). Certain aspects important for microanalysis include: (i) accurate determination of the partial cross sections, σx(α,ΔE) for core excitation when scattering lies inside collection angle a and energy range ΔE above the edge, (ii) behavior of the background intensity due to excitation of less strongly bound electrons, necessary for extrapolation beneath the signal of interest, (iii) departures from the simple hydrogenic K-edge seen in L and M losses, effecting σx and complicating microanalysis. Such problems might be approached empirically but here we describe how computation can elucidate the spectrum shape.The inelastic cross section differential with respect to energy transfer E and momentum transfer q for electrons of energy E0 and velocity v can be written as


1979 ◽  
Vol 40 (10) ◽  
pp. 1024-1024
Author(s):  
G. André ◽  
R. Bidaux ◽  
J.-P. Carton ◽  
R. Conte ◽  
L. de Seze

1986 ◽  
Vol 47 (C8) ◽  
pp. C8-575-C8-578 ◽  
Author(s):  
A. P. HITCHCOCK

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