Three prerequisites for high-temperature superconductivity in t-PtBi₂
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Although the generic mechanism behind high-temperature superconductivity remains notoriously elusive, a set of favorable conditions for its occurrence in a given material has emerged: (i) the electronic structure should have a very high density of states near the Fermi level; (ii) electrons need to be susceptible to a sizable interaction with another degree of freedom to ensure pairing themselves; (iii) the ability to fine-tune some of the system properties significantly helps maximising the critical temperature. Here, by means of high-resolution ARPES, we show that all three criteria are remarkably fulfilled in trigonal platinum bismuthide (t-PtBi$_2$). Specifically, this happens on its surface, which hosts topological surface states known as Fermi arcs. Our findings pave the way for the stabilisation and optimisation of high-temperature superconductivity in this topological material.
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Cited by 2 Pith papers
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Mechanism for Nodal Topological Superconductivity on PtBi$_2$ Surface
Anisotropic electron-phonon coupling with screened Coulomb repulsion yields nodal gaps in PtBi2 surface superconductivity when bandwidth approximates phonon energy.
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Fermiology and spin polarization of topological surface states in PtBi$_2$
Spin-ARPES on PtBi2 shows spin-polarized singly degenerate Fermi-arc surface states with termination-dependent dispersion, supporting its candidacy for topological superconductivity.
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