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The five-orbital model being considered here has strong hybridization among the five orbitals and, as a result, the change in basis matrix U does not have a block diagonal structure for all values of the momentum. If this were the case, it would be possible to obtain a pure intraband pairing arising from intraorbital pairing with orbital-dependent strength. Orbitals that do not hybridize with each other could have different pairing strengths, which in turn may produce FSs with independent gaps; it is the case in MgB2 (Ref.) and NdSe2 (Ref.).
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The five-orbital model being considered here has strong hybridization among the five orbitals and, as a result, the change in basis matrix U does not have a block diagonal structure for all values of the momentum. If this were the case, it would be possible to obtain a pure intraband pairing arising from intraorbital pairing with orbital-dependent strength. Orbitals that do not hybridize with each other could have different pairing strengths, which in turn may produce FSs with independent gaps; it is the case in MgB 2 (Ref.) and NdSe 2 (Ref.).
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