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Please use this identifier to cite or link to this item: http://dspace.bits-pilani.ac.in:8080/jspui/handle/123456789/14501
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dc.contributor.authorDutta, Sandipan-
dc.date.accessioned2024-03-04T05:35:01Z-
dc.date.available2024-03-04T05:35:01Z-
dc.date.issued2009-04-
dc.identifier.urihttps://onlinelibrary.wiley.com/doi/full/10.1002/qua.22234-
dc.identifier.urihttp://dspace.bits-pilani.ac.in:8080/jspui/xmlui/handle/123456789/14501-
dc.description.abstractSemiclassical methods of statistical mechanics can incorporate essential quantum effects by using effective quantum potentials. An ideal Fermi gas interacting with an impurity is represented by a classical fluid with effective electron–electron and electron-impurity quantum potentials. The electron-impurity quantum potential is evaluated at weak coupling, leading to a generalization of the Kelbg potential to include both diffraction and degeneracy effects. The electron–electron quantum potential for exchange effects only is the same as that discussed earlier by othersen_US
dc.language.isoenen_US
dc.publisherWileyen_US
dc.subjectPhysicsen_US
dc.subjectSemiclassicalen_US
dc.subjectFermi gasen_US
dc.titleQuantum potential for diffraction and exchange effectsen_US
dc.typeArticleen_US
Appears in Collections:Department of Physics

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