Dynamical local-field factor in the response function of an electron gas

1986 ◽  
Vol 34 (8) ◽  
pp. 4989-4995 ◽  
Author(s):  
Bogdan Dabrowski
1995 ◽  
Vol 75 (4) ◽  
pp. 689-692 ◽  
Author(s):  
Saverio Moroni ◽  
David M. Ceperley ◽  
Gaetano Senatore

1991 ◽  
Vol 69 (5) ◽  
pp. 573-580 ◽  
Author(s):  
K. L. Liu

We study the wavevector- and frequency- dependent exchange-correlation local-field factor, [Formula: see text], of the dynamical spin susceptibility, [Formula: see text], of a homogeneous electron gas. For high frequencies we calculate [Formula: see text] diagrammatically to second order in the Coulomb interaction, and consequently find that [Formula: see text] varies as q−2 ω−1/2 for large ω and finite q. We also consider an interpolation formula for [Formula: see text], that yields the exact small- and large- wave-number limits. Making use of these results and the Kramers–Kronig relation, we construct an approximate local-field factor that has the correct limiting behavior for both low and high frequencies.


1998 ◽  
Vol 12 (16) ◽  
pp. 639-648 ◽  
Author(s):  
A. Sarkar ◽  
D. Sen ◽  
S. Haldar ◽  
D. Roy

A simple parametric form for the static local field factor G(q) which appears in the dielectric screening theory of an electron gas is proposed. A very accurate fit of Ceperley–Alder data of electron correlation energy in the entire density range using Levin–Weniger interpolant is obtained and used for the calculation of G(q). Both the short- and long- wavelength limits of G(q) are satis ed exactly in the present formulation which ensures fulfilment of a number of other legitimate criteria and produces some interesting results. A comparative study of the various static local eld factors derived so far vis-a-vis the present work is made. Even within the approximations of a static self-consistent theory, reasonable prediction regarding Wigner Crystallization is obtained in the present work.


2004 ◽  
Vol 106 (4) ◽  
pp. 497-514 ◽  
Author(s):  
A. Sarkar ◽  
S. Haldar ◽  
D. Roy ◽  
D. Sen

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