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Strange Metal in Magic-Angle Graphene with near Planckian Dissipation

Yuan CaoDepartment of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USADebanjan ChowdhuryDepartment of Physics, Cornell University, Ithaca, New York 14853, USADaniel Rodan‐LegrainDepartment of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USAOriol Rubies-BigordàDepartment of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USAKenji WatanabeNational Institute for Materials Science, Namiki 1-1, Tsukuba, Ibaraki 305-0044, JapanTakashi TaniguchiNational Institute for Materials Science, Namiki 1-1, Tsukuba, Ibaraki 305-0044, JapanT. SenthilDepartment of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USAPablo Jarillo‐HerreroDepartment of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
2020en
ABI

Аннотация

Recent experiments on magic-angle twisted bilayer graphene have discovered correlated insulating behavior and superconductivity at a fractional filling of an isolated narrow band. Here we show that magic-angle bilayer graphene exhibits another hallmark of strongly correlated systems-a broad regime of T-linear resistivity above a small density-dependent crossover temperature-for a range of fillings near the correlated insulator. This behavior is reminiscent of similar behavior in other strongly correlated systems, often denoted "strange metals," such as cuprates, iron pnictides, ruthenates, and cobaltates, where the observations are at odds with expectations in a weakly interacting Fermi liquid. We also extract a transport "scattering rate," which satisfies a near Planckian form that is universally related to the ratio of (k_{B}T/ℏ). Our results establish magic-angle bilayer graphene as a highly tunable platform to investigate strange metal behavior, which could shed light on this mysterious ubiquitous phase of correlated matter.

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