Universal relation between residual resistivity and A coefficient in correlated metals
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arXiv
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| Main Authors: | , , , , , |
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| Format: | Preprint |
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2025
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| _version_ | 1866914014050648064 |
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| author | Efimova, Anna Yu. Saito, Yohei Kawamoto, Atsushi Dressel, Martin Rademaker, Louk Pustogow, Andrej |
| author_facet | Efimova, Anna Yu. Saito, Yohei Kawamoto, Atsushi Dressel, Martin Rademaker, Louk Pustogow, Andrej |
| contents | The effects of strong electronic correlations and disorder are crucial for emergent phenomena such as unconventional superconductivity, metal-insulator transitions, and quantum criticality. While both are omnipresent in real materials, their individual impacts on charge transport remain elusive. To disentangle their respective roles, we have independently varied the degree of randomness and the strength of electronic correlations -- by chemical substitution and physical pressure, respectively -- within the metallic phase nearby a Mott-insulating state. We find a distinct correlation dependence of the disorder-dependent residual resistivity $ρ_0$ in the Fermi-liquid regime $ρ(T)=ρ_0 + A T^2$, where $A\propto (m^{\star}/m)^2$ quantifies the electronic mass enhancement. Contrary to conventional expectations, we observe that at fixed disorder level $ρ_0$ grows linearly with $A$. This scaling can be understood in terms of chemical-potential fluctuations with variance $σ_μ^2$, yielding $ρ_0 \propto A\,σ_μ^2$. By comparing our findings to transport data on other organic Mott systems, oxides, heavy-fermion compounds, and moiré materials, we demonstrate that this new relation between residual resistivity and mass enhancement is a universal feature of correlated metals. |
| format | Preprint |
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arxiv_https___arxiv_org_abs_2508_21759 |
| institution | arXiv |
| publishDate | 2025 |
| record_format | arxiv |
| spellingShingle | Universal relation between residual resistivity and A coefficient in correlated metals Efimova, Anna Yu. Saito, Yohei Kawamoto, Atsushi Dressel, Martin Rademaker, Louk Pustogow, Andrej Strongly Correlated Electrons Materials Science The effects of strong electronic correlations and disorder are crucial for emergent phenomena such as unconventional superconductivity, metal-insulator transitions, and quantum criticality. While both are omnipresent in real materials, their individual impacts on charge transport remain elusive. To disentangle their respective roles, we have independently varied the degree of randomness and the strength of electronic correlations -- by chemical substitution and physical pressure, respectively -- within the metallic phase nearby a Mott-insulating state. We find a distinct correlation dependence of the disorder-dependent residual resistivity $ρ_0$ in the Fermi-liquid regime $ρ(T)=ρ_0 + A T^2$, where $A\propto (m^{\star}/m)^2$ quantifies the electronic mass enhancement. Contrary to conventional expectations, we observe that at fixed disorder level $ρ_0$ grows linearly with $A$. This scaling can be understood in terms of chemical-potential fluctuations with variance $σ_μ^2$, yielding $ρ_0 \propto A\,σ_μ^2$. By comparing our findings to transport data on other organic Mott systems, oxides, heavy-fermion compounds, and moiré materials, we demonstrate that this new relation between residual resistivity and mass enhancement is a universal feature of correlated metals. |
| title | Universal relation between residual resistivity and A coefficient in correlated metals |
| topic | Strongly Correlated Electrons Materials Science |
| url | https://arxiv.org/abs/2508.21759 |