Loss of Quasiparticles: From Strange Metals to Flat Bands
ORAL · Invited
Abstract
Strange metals are a form of correlated systems at extreme, and a loss of Landau quasiparticles represents an underlying cause for their properties. It is in contrast to the resiliency of the quasiparticles when the electron-electron interactions are treated perturbatively. One prototype setting of interest arises in heavy fermion strange metals, which are well described by the beyond-Landau quantum criticality of Kondo destruction [1,2]. This mechanism has been supported by a large body of experiments, and the predicted loss of quasiparticles has recently received fairly direct evidence from shot noise [3]. Surprisingly, quantum information approaches in the form of entanglement witnesses have been found to elucidate the quantum critical fluid and loss of quasiparticles [4]. As another exemplary platform, I will consider the emergent flat bands of d-electron systems with a kagome or related frustrated lattice [5]. The notion of compact molecular orbitals is introduced, leading to a Kondo lattice description. This allows us [5] to advance the first theoretical understanding of the observed strange metal behavior, and to predict a phase diagram that is now seen in a new kagome metal. From this framework, I will briefly address the recently observed superconductivity in twisted WSe2 [6]. Some general implications will be discussed.
[1] H. Hu, L. Chen & Q. Si, Nat Phys, in press (2024); Q. Si et al., Nature 413, 804 (2001).
[2] S. Paschen & Q. Si, Nat. Rev. Phys. 3, 9 (2021); S. Kirchner et al, Rev. Mod. Phys. 92, 011002 (2020).
[3] L. Y. Chen et al., Science 382, 907 (2023); Y. Wang et al., Phys. Rev. Research 6, L042045 (2024).
[4] Y. Fang et al., arXiv:2402.18552.
[5] L. Chen et al., arXiv:2307.09431; F. Xie et al., arXiv 2403.03911 (2024); L. Chen et al., Nat Comm 15, 5242 (2024); H. Hu & Q. Si, Sci. Adv. 9, eadg0028 (2023).
[6] F. Xie et al., arXiv:2408.10185.
[1] H. Hu, L. Chen & Q. Si, Nat Phys, in press (2024); Q. Si et al., Nature 413, 804 (2001).
[2] S. Paschen & Q. Si, Nat. Rev. Phys. 3, 9 (2021); S. Kirchner et al, Rev. Mod. Phys. 92, 011002 (2020).
[3] L. Y. Chen et al., Science 382, 907 (2023); Y. Wang et al., Phys. Rev. Research 6, L042045 (2024).
[4] Y. Fang et al., arXiv:2402.18552.
[5] L. Chen et al., arXiv:2307.09431; F. Xie et al., arXiv 2403.03911 (2024); L. Chen et al., Nat Comm 15, 5242 (2024); H. Hu & Q. Si, Sci. Adv. 9, eadg0028 (2023).
[6] F. Xie et al., arXiv:2408.10185.
*In collaboration with A. Cai, J. Cano, L. Chen, L. Y. Chen, Y. Fang, K. Grube, H. Hu, K. Ingersent, A. Kandala, S. Kirchner, J. Kono, X.W. Li, C.-C. Liu, D. Natelson, S. Paschen, C. Setty, F. Steglich, S. Sur, J. D. Thompson, H. von Lohneysen, Y. Wang, S. Wirth, F. Xie, R. Yu & J.-X. Zhu.Supported by the DOE BES (DE-SC0018197), NSF (DMR-2220603), AFOSR (FA9550-21-1-0356), and VBFF (N00014-23-1-2870).
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Presenters
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Qimiao Si
- Rice University