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Bibcode Bot (talk | contribs) m Converting 0 "id = {{arxiv|...}}" to "|arxiv=...". Adding 2 arXiv eprint(s), 5 bibcode(s) and 0 doi(s). Did it miss something? Report bugs, errors, and suggestions at User talk:Bibcode Bot |
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|volume=25 |page=792
|doi=10.1016/0031-8914(59)90004-7
|bibcode = 1959Phy....25..792V }}</ref> to [[quantum fluid]]s as well. The classical HNC, together with the [[Percus–Yevick approximation]], are the two pillars which bear the brunt of most calculations in the theory of interacting [[classical fluids]]. Also, HNC and PY have become important in providing basic reference schemes in the theory of fluids,<ref>
{{cite book
|author=R. Balescu
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|pmid=11017415
|bibcode=2000PhRvL..84..959D
|arxiv = cond-mat/9909056 }}</ref> The value of the method lies in its ability to calculate the ''interacting'' pair distribution functions ''g''(''r'') at zero and finite temperatures. Comparison of the calculated ''g''(''r'') with results from Quantum Monte Carlo show remarkable agreement, even for very strongly correlated systems.
The interacting pair-distribution functions obtained from CHNC have been used to calculate the exchange-correlation energies, [[Landau parameter]]s of [[Fermi liquid]]s and other quantities of interest in many-body physics and [[density functional theory]], as well as in the theory of hot plasmas.
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|volume=65 |pages=195116
|doi=10.1103/PhysRevB.65.195116
|bibcode = 2002PhRvB..65s5116B }}
*{{cite journal
|author=M.W.C. Dharma-wardana, F. Perrot
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|volume=66 |pages=014110
|doi=10.1103/PhysRevB.66.014110
|bibcode = 2002PhRvB..66a4110D }}
*{{cite journal
|author=N.Q. Khanh, H. Totsuji
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|volume=129 |pages=37
|doi=10.1016/j.ssc.2003.09.010
|bibcode = 2004SSCom.129...37K }}
*{{cite journal
|author=M.W.C. Dharma-wardana
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|volume=72 |pages=125339
|doi=10.1103/PhysRevB.72.125339
|arxiv = cond-mat/0506804 |bibcode = 2005PhRvB..72l5339D }}
[[Category:Theoretical physics]]
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