f$-electron hybridised metallic Fermi surface in magnetic field-induced metallic YbB$_{12}

• Main Authors: Liu, H, Hickey, A. J, Hartstein, M, Davies, A. J, Eaton, A. G, Elvin, T, Polyakov, E, Vu, T. H, Wichitwechkarn, V, Förster, T, Wosnitza, J, Murphy, T. P, Shitsevalova, N, Johannes, M. D, Hatnean, M. Ciomaga, Balakrishnan, G, Lonzarich, G. G, Sebastian, Suchitra E
• Format: Journal Article
• Language: English
• Published: 18.02.2021
• Subjects: Physics - Strongly Correlated Electrons
• DOI: 10.48550/arxiv.2102.09545

npj Quantum Materials 7, 12 (2022) The nature of the Fermi surface observed in the recently discovered family of unconventional insulators starting with SmB$_6$ and subsequently YbB$_{12}$ is a subject of intense inquiry. Here we shed light on this question by comparing quantum oscillations between the high magnetic field-induced metallic regime in YbB$_{12}$ and the unconventional insulating regime. In the field-induced metallic regime beyond 47 T, we find prominent quantum oscillations in the contactless resistivity characterised by multiple frequencies up to at least 3000 T and heavy effective masses up to at least 17 $m_\text{e}$, characteristic of an $f$-electron hybridised metallic Fermi surface. The growth of quantum oscillation amplitude at low temperatures in electrical transport and magnetic torque in insulating YbB$_{12}$ is closely similar to the Lifshitz-Kosevich low temperature growth of quantum oscillation amplitude in field-induced metallic YbB$_{12}$, pointing to an origin of quantum oscillations in insulating YbB$_{12}$ from in-gap neutral low energy excitations. The field-induced metallic regime of YbB$_{12}$ is characterised by more Fermi surface sheets of heavy quasiparticle effective mass that emerge in addition to the heavy Fermi surface sheets yielding multiple quantum oscillation frequencies below 1000 T observed in both insulating and metallic regimes. We thus observe a heavy multi-component Fermi surface in which $f$-electron hybridisation persists from the unconventional insulating to the field-induced metallic regime of YbB$_{12}$, which is in distinct contrast to the unhybridised conduction electron Fermi surface observed in the case of the unconventional insulator SmB$_6$. Our findings require a different theoretical model of neutral in-gap low energy excitations in which the $f$-electron hybridisation is retained in the case of the unconventional insulator YbB$_{12}$.