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DC Field | Value | Language |
---|---|---|
dc.contributor.author | Dutta, Sandipan | - |
dc.date.accessioned | 2024-03-04T05:35:01Z | - |
dc.date.available | 2024-03-04T05:35:01Z | - |
dc.date.issued | 2009-04 | - |
dc.identifier.uri | https://onlinelibrary.wiley.com/doi/full/10.1002/qua.22234 | - |
dc.identifier.uri | http://dspace.bits-pilani.ac.in:8080/jspui/xmlui/handle/123456789/14501 | - |
dc.description.abstract | Semiclassical 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 others | en_US |
dc.language.iso | en | en_US |
dc.publisher | Wiley | en_US |
dc.subject | Physics | en_US |
dc.subject | Semiclassical | en_US |
dc.subject | Fermi gas | en_US |
dc.title | Quantum potential for diffraction and exchange effects | en_US |
dc.type | Article | en_US |
Appears in Collections: | Department of Physics |
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