scholarly journals Calculation of the effective interaction parameter in theLDA+Umethod by a linear response approach forFe(OH)2

2009 ◽  
Vol 80 (15) ◽  
Author(s):  
Mansoureh Pashangpour ◽  
Amir Abbas Sabouri-Dodaran ◽  
Khadijeh Imani ◽  
Nasser Nafari
2001 ◽  
Vol 39 (21) ◽  
pp. 2549-2561 ◽  
Author(s):  
C. C. Greenberg ◽  
M. D. Foster ◽  
C. M. Turner ◽  
S. Corona-Galvan ◽  
E. Cloutet ◽  
...  

Polymer ◽  
1999 ◽  
Vol 40 (16) ◽  
pp. 4713-4716 ◽  
Author(s):  
C.C. Greenberg ◽  
M.D. Foster ◽  
C.M. Turner ◽  
S. Corona-Galvan ◽  
E. Cloutet ◽  
...  

1991 ◽  
Vol 05 (18) ◽  
pp. 2951-2972 ◽  
Author(s):  
HUA CHEN ◽  
DANIEL C. MATTIS

A microscopic formula for the effective two-body interaction between electrons or holes in an ideal metal is derived within the linear response theory. Both the zero-range Hubbard interaction U0 and the long-range Coulomb interaction, denoted by ΔV(q), are included. The effective interaction, which is necessarily spin-dependent, is expressed in terms of the exact charge and spin density-density correlation functions and of their higher order mixtures. These correlation functions are analyzed diagrammatically. Attention is paid to clarifying the different roles played by U0 and ΔV(q). We also display the corresponding new formula for the free energy. Comparison is made with previous theories.


2012 ◽  
Vol 21 (05) ◽  
pp. 1250040 ◽  
Author(s):  
A. PASTORE ◽  
K. BENNACEUR ◽  
D. DAVESNE ◽  
J. MEYER

Nuclear effective interactions are often modeled by simple analytical expressions such as the Skyrme zero-range force. This effective interaction depends on a limited number of parameters that are usually fitted using experimental data obtained from doubly magic nuclei. It was recently shown that many Skyrme functionals lead to the appearance of instabilities, in particular when symmetries are broken, for example unphysical polarization of odd–even or rotating nuclei. In this paper, we show how the formalism of the linear response in infinite nuclear matter can be used to predict and avoid the regions of parameters that are responsible for these unphysical instabilities.


2007 ◽  
Vol 40 (21) ◽  
pp. 7644-7655 ◽  
Author(s):  
Du Yeol Ryu ◽  
Changhak Shin ◽  
Junhan Cho ◽  
Dong Hyun Lee ◽  
Jin Kon Kim ◽  
...  

2007 ◽  
Vol 126 (17) ◽  
pp. 174904 ◽  
Author(s):  
P. E. Theodorakis ◽  
A. Avgeropoulos ◽  
J. J. Freire ◽  
M. Kosmas ◽  
C. Vlahos

2010 ◽  
Author(s):  
L. H. Ho ◽  
A. P. Micolich ◽  
W. R. Clarke ◽  
O. Klochan ◽  
A. R. Hamilton ◽  
...  

Author(s):  
Keinosuke Kobayashi

Equidensitometry as developed by E. Lau and W. Krug has been little used in the analysis of ordinary electron photomicrographs, yet its application to the high voltage electron images proves merits of this procedure. Proper sets (families) of equidensities as shown in the next page are able to reveal the contour map of mass thickness distribution in thick noncrystalline specimens. The change in density of the electron micrograph is directly related to the mass thickness of corresponding area in the specimen, because of the linear response of photographic emulsions to electrons and the logarithmic relation between electron opacity and mass thickness of amorphous object.This linearity is verified by equidensitometry of a spherical solid object as shown in Fig. 1a. The object is a large (1 μ) homogeneous particle of polystyrene. Fig. 1b is a composite print of three equidensities of the 1st order prepared from Fig. 1a.


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