Role of short-range correlation in facilitation of wave propagation in a long-range ladder chain

2018 ◽  
Vol 505 ◽  
pp. 49-60 ◽  
Author(s):  
O. Farzadian ◽  
M.D. Niry
Keyword(s):  
Wave Propagation ◽  
Long Range ◽  
Short Range ◽  
Short Range Correlation ◽  
Range Correlation

Density dependences of long-range fluctuations and short-range correlation lengths of CHF3 and CH2F2 in supercritical states

2006 ◽  
Vol 124 (12) ◽  
pp. 124519 ◽  
Author(s):  
Takeshi Morita ◽  
Yoshihiro Takahashi ◽  
Yoshitada Tanaka ◽  
Asako Ayusawa Arai ◽  
Keiko Nishikawa
Keyword(s):  
Long Range ◽  
Short Range ◽  
Short Range Correlation ◽  
Correlation Lengths ◽  
Range Correlation

scholarly journals A first-principles-based correlation functional for harmonious connection of short-range correlation and long-range dispersion

2012 ◽  
Vol 137 (20) ◽  
pp. 204121 ◽  
Author(s):  
Marcin Modrzejewski ◽  
Michał Lesiuk ◽  
Łukasz Rajchel ◽  
Małgorzata M. Szczęśniak ◽  
Grzegorz Chałasiński
Keyword(s):  
Long Range ◽  
First Principles ◽  
Short Range ◽  
Short Range Correlation ◽  
Range Correlation

scholarly journals The effect of short range correlation on the inelastic C4 form factors of 18O nucleus

2019 ◽  
Vol 13 (28) ◽  
pp. 130-141
Author(s):  
Abdullah S. Mdekil
Keyword(s):  
Charge Density ◽  
Short Range ◽  
Form Factors ◽  
Model Space ◽  
Charge Density Distribution ◽  
Short Range Correlation ◽  
Range Correlation ◽  
Free Parameters ◽  
State Charge ◽  
Short Range Correlations

The effect of short range correlations on the inelastic longitudinalCoulomb form factors for different states of J   4 , T  1withexcitation energies 3.553,7.114, 8.960 and 10.310 MeV in 18O isanalyzed. This effect (which depends on the correlation parameter )is inserted into the ground state charge density distribution throughthe Jastrow type correlation function. The single particle harmonicoscillator wave function is used with an oscillator size parameter b.The parameters  and b are considered as free parameters, adjustedfor each excited state separately so as to reproduce the experimentalroot mean square charge radius of 18O. The model space of 18O doesnot contribute to the transition charge density. As a result, theinelastic Coulomb form factors of 18O comes absolutely from thecore polarization transition charge density. According to thecollective modes of nuclei, the core polarization transition chargedensity is assumed to have the form of Tassie shape. It is found thatthe introduction of the effect of short range correlations is necessaryfor obtaining a remarkable modification in the calculated inelasticlongitudinal Coulomb form factors and considered as an essential forexplanation the data amazingly throughout the whole range ofconsidered momentum transfer.

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