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Linear resistivity and Sachdev-Ye-Kitaev (SYK) spin liquid behavior in a quantum critical metal with spin-1/2 fermions
“Strange metals” with resistivity depending linearly on temperature [Formula: see text] down to low [Formula: see text] have been a long-standing puzzle in condensed matter physics. Here, we consider a lattice model of itinerant spin- [Formula: see text] fermions interacting via onsite Hubbard inter...
Autores principales: | , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
National Academy of Sciences
2020
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7414094/ https://www.ncbi.nlm.nih.gov/pubmed/32699148 http://dx.doi.org/10.1073/pnas.2003179117 |
Sumario: | “Strange metals” with resistivity depending linearly on temperature [Formula: see text] down to low [Formula: see text] have been a long-standing puzzle in condensed matter physics. Here, we consider a lattice model of itinerant spin- [Formula: see text] fermions interacting via onsite Hubbard interaction and random infinite-ranged spin–spin interaction. We show that the quantum critical point associated with the melting of the spin-glass phase by charge fluctuations displays non-Fermi liquid behavior, with local spin dynamics identical to that of the Sachdev-Ye-Kitaev family of models. This extends the quantum spin liquid dynamics previously established in the large- [Formula: see text] limit of [Formula: see text] symmetric models to models with physical [Formula: see text] spin- [Formula: see text] electrons. Remarkably, the quantum critical regime also features a Planckian linear- [Formula: see text] resistivity associated with a [Formula: see text]-linear scattering rate and a frequency dependence of the electronic self-energy consistent with the marginal Fermi liquid phenomenology. |
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