Classical-map hypernetted-chain method: Difference between revisions

Revision as of 18:16, 11 June 2007

Revision as of 18:22, 11 June 2007

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'''Classical-map Hyper-Netted-Chain''' ('''CHNC''') technique is a method in many-body theoretical physics for interacting uniform [[electron liquid]]s in two and three dimensions, and to interacting [[hydrogen plasmas]]. The method extends the famous hyper-netted-chain

method (HNC) introduced by van Leeuwen et al.<ref>J. M. J. van Leeuwen, J. Groenveld, J. de Boer: Physica '''25''', 792 (1959)</ref> to [[quantum fluid]]s as well. The classical HNC, together with the Percus-Yevik (PY) equation, 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> R. Balescu, ''Equilibrium and Non-equilibrium Statistical Mechanics'' (Wiley 1975) p257-277 </ref>, and hence they are of great importance to the physics of many-particle systems.

The HNC and PY intergral equations provide the pair-distribution functions of the particles in a classical fluid, even for very high coupling strengths. The coupling strength is measured by the ratio of the potential energy to the kinetic energy. In a classical fluid, the kinetic energy is proportional to the temperature. In a quantum fluid, the situation is very complicated as one needs to deal with quantum operators, and matrix elements of such operators, which appear in various perturbation methods based on [[Feynman]] diagrams.

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In the CHNC method, the pair-distributions of the interacting particles are calculated using a mapping which ensures that the quantum mechanically correct non-interacting pair distribution function is recovered when the Coulomb interactions are switched off

<ref>M.W. C. Dharma-wardana and FrancoisFrançois Perrot, Physical Review Letters, vol. '''84''', page 959-962 (2000)</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 parameters 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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[[Quantum fluid]]

*C. Bulutay and B. Tanatar, Physical Review B, volume '''65''', page 195116 (2002)

*M. W. C. Dharma-wardana and FrancoisFrançois Perrot, Physical Review B, volume '''66''', page 014110 (2002)

*N. Q. Khanh and H. Totsuji, Solid State Com., vol.'''129''', page 37 (2004)

*M. W. C. Dharma-wardana, Physical Review B, volume72'''72''', page 125339 (2005)

[[Category:Theoretical physics]]