We discuss the effect of k-dependent hybridization in the specific heat jum
p AC at the superconducting critical temperature T-c, considering an exact
analytical expression obtained from the extended BCS gap equation. Our mode
l intends to discuss a superconducting material described by a two-band mod
el, within an extended BCS picture. We consider a broad s-p conducting band
. hybridized with a narrow d-band. assuming that: (i) electron-electron rep
ulsion U-r, formulated via the Hubbard model and (ii) electron-electron att
raction due to electron-"fonon" interaction U-a, treated in a BCS framework
, both occur at the narrow d-band. One observes that there is a critical va
lue V-c for the hybridization (depending on the ratio a of the effective ma
sses of the narrow and broad bands), above which there is no AC jump. Moreo
ver, one observes that: (i) the ratio alpha of the effective band masses in
a homothetic band picture plays an important role in the jump, and (ii) th
e Hubbard like repulsive interaction is very small and therefore plays no s
ignificant role in the range of temperatures where superconductivity occurs
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