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Ubiquity of Rotational Symmetry Breaking in Superconducting Films, From Fe(Te,Se)/Bi2Te3 to Nb, and the Effect of Measurement Geometry
1 Introduction The conventional picture of superconductivity was provided by the famous Bardeen–Cooper–Schrieffer (BCS) theory, where the electrons are paired by lattice vibration (phonon). Nevertheless, there have been other families of superconductors (SCs) that do not fall under this BCS category, where the pairing mechanism cannot be explained by the BCS theory.
Evidence of charge transfer in three-dimensional topological insulator/antiferromagnetic Mott insulator ${\mathrm{Bi}}_{1}{\mathrm{Sb}}_{1}{\mathrm{Te}}_{1.5}{\mathrm{Se}}_{1.5}/\ensuremath{\alpha}\text{\ensuremath{-}}{\mathrm{RuCl}}_{3}$ heterostructures
Abstract We report magnetotransport measurements on Bi1Sb1Te1.5Se1.5/RuCl3 heterostructure nanodevices. Bi1Sb1Te1.5Se1.5 (BSTS) is a strong three-dimensional topological insulator (3D-TI) that hosts conducting topological surface states (TSS) enclosing an insulating bulk. α−RuCl3 (namely, RuCl3) is an antiferromagnet that is predicted to behave as a Kitaev-like quantum spin liquid carrying chargeless Majorana excitations.
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