Excitonic instability of two-dimensional tilted Dirac cones
arXiv:1910.08999 · doi:10.1103/PhysRevResearch.2.033479
Abstract
The electron-electron Coulomb interaction in Dirac-Weyl semimetals harbours a novel paradigm of correlation effects that hybridizes diverse realms of solid-state physics with their relativistic counterpart. Driving spontaneous mass acquisition, the excitonic condensate of strongly-interacting massless Dirac fermions is one such example whose exact nature remains debated. Here, by focussing on the two-dimensional tilted Dirac cones in the organic salt -(BEDT-TTF)I, we show that the excitonic instability is controlled by a small chemicalpotential shift and an in-plane magnetic field. In combined analyses based on renormalization-group approaches and ladder approximation, we demonstrate that the nuclear relaxation rate is an excellent probe of excitonic-spin fluctuations in an extended parameter region. Comparative nuclear magnetic resonance (NMR) experiments show good agreements with this result, jointly revealing the importance of intervalley nesting between field-induced, spin-split Fermi pockets of opposite charge polarities. Our work provides an accurate framework to search for excitonic instability of strongly-interacting massless fermions.
arXiv comment26 pages, 5 figures, 1 supplementary file (9 pages, 3 figures)
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Cited by in corpus (9)
- Molecular Quantum Materials: Electronic Phases and Charge Dynamics in Two-Dimensional Organic Solids
- Anisotropic effects in two-dimensional materials
- Interaction-induced quantum spin Hall insulator in the organic Dirac electron system -(BEDT-TSeF)I
- Gap opening mechanism for correlated Dirac electrons in organic compounds -(BEDT-TTF)I and -(BEDT-TSeF)I
- Thermal difference reflectivity of tilted 2D Dirac materials
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