Though YB and LaB share the same crystal structure, atomic valence electron configuration, and phonon modes, they exhibit drastically different phonon-mediated superconductivity. YB superconducts below 8.4 K, giving it the second-highest critical temperature of known borides, second only to MgB. LaB does not superconduct until near-absolute zero temperatures (below 0.45 K), however. Though previous studies have quantified the canonical superconductivity descriptors of YB's greater Fermi-level (E) density of states and higher electron-phonon coupling (EPC), the root of this difference has not been assessed with full detail of the electronic structure. Through chemical bonding, we determine low-lying, unoccupied 4f atomic orbitals in lanthanum to be the key difference between these superconductors. These orbitals, which are not accessible in YB, hybridize with π B-B bonds and bring this π-system lower in energy than the σ B-B bonds otherwise at E. This inversion of bands is crucial: the optical phonon modes we show responsible for superconductivity cause the σ-orbitals of YB to change drastically in overlap, but couple weakly to the π-orbitals of LaB. These phonons in YB even access a crossing of electronic states, indicating strong EPC. No such crossing in LaB is observed. Finally, a supercell (the M k-point) is shown to undergo Peierls-like effects in YB, introducing additional EPC from both softened acoustic phonons and the same electron-coupled optical modes as in the unit cell. Overall, we find that LaB and YB have fundamentally different mechanisms of superconductivity, despite their otherwise near-identity.

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http://www.ncbi.nlm.nih.gov/pmc/articles/PMC10998635PMC
http://dx.doi.org/10.1073/pnas.2316101121DOI Listing

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