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Please use this identifier to cite or link to this item: http://hdl.handle.net/11375/9579
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dc.contributor.advisorCarbotte, J.P.en_US
dc.contributor.authorLarose, Lucieen_US
dc.date.accessioned2014-06-18T16:47:43Z-
dc.date.available2014-06-18T16:47:43Z-
dc.date.created2009-06-22en_US
dc.date.issued1975-12en_US
dc.identifier.otheropendissertations/469en_US
dc.identifier.other1145en_US
dc.identifier.other878000en_US
dc.identifier.urihttp://hdl.handle.net/11375/9579-
dc.description.abstract<p>The electronic part of the specific heat γ is calculated for dilute alloys at zero temperature. Only alloys where the impurity and the host ions have the same valence are considered. We take into account two mechanisms which change the value of γ of the pure metal. First the impurities affect the band structure and therefore the Fermi level density of states α (Eғ). Second they also influence the electron-phonon interaction and hence the mass renormalization. We calculate γ from first principles using the Born-von Karman lattice dynamics theory, electron-ion pseudopotentials and phonon Green's functions. The various corrections to γ are evaluated for NaK and KNa using the Ashcroft pseudopotentials form factors. It is found that the change in the mass renormalization is more important than that in α (Eғ) in calculating the electronic specific heat for the alloy.</p>en_US
dc.subjectPhysicsen_US
dc.subjectPhysicsen_US
dc.titleElectronic Specific Heat in Dilute Alloysen_US
dc.typethesisen_US
dc.contributor.departmentPhysicsen_US
dc.description.degreeMaster of Science (MS)en_US
Appears in Collections:Open Access Dissertations and Theses

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