Common superconducting transition in under and overdoped cuprate superconductors
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arXiv
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| Auteurs principaux: | , |
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| Format: | Preprint |
| Publié: |
2025
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| _version_ | 1866915369546940416 |
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| author | and, Hércules H. Santana de Mello, E. V. L. |
| author_facet | and, Hércules H. Santana de Mello, E. V. L. |
| contents | Underdoped cuprate superconductors are believed to be strongly correlated with electronic systems with small phase stiffness leading to a large phase fluctuation region is known as the pseudogap state. With increasing doping it is generally agree that they become Fermi liquid, rendering the end of the superconductivity due to the sufficiently large electronic screening. However, this scenario does not stand against a recent experiment\cite{OverJJ2022} that combined magnetic susceptibility and Scanning Tunnelling Microscopy (STM) which measured superconducting gaps and amplitudes amid charge inhomogeneity far beyond the critical doping $p_{\rm c} \approx 0.27$. We reproduced these results by calculating the localized superconducting amplitudes that emerge out of charge inhomogeneities, which forms a mesoscopic granular superconductor with an array of Josephson junctions, whose average couplings determine the critical temperature $T_{\rm c}$. The calculations agree with the experiments and both yield that underdoped and overdoped compounds have superconducting long-range order by the same mechanism. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2507_01718 |
| institution | arXiv |
| publishDate | 2025 |
| record_format | arxiv |
| spellingShingle | Common superconducting transition in under and overdoped cuprate superconductors and, Hércules H. Santana de Mello, E. V. L. Superconductivity Underdoped cuprate superconductors are believed to be strongly correlated with electronic systems with small phase stiffness leading to a large phase fluctuation region is known as the pseudogap state. With increasing doping it is generally agree that they become Fermi liquid, rendering the end of the superconductivity due to the sufficiently large electronic screening. However, this scenario does not stand against a recent experiment\cite{OverJJ2022} that combined magnetic susceptibility and Scanning Tunnelling Microscopy (STM) which measured superconducting gaps and amplitudes amid charge inhomogeneity far beyond the critical doping $p_{\rm c} \approx 0.27$. We reproduced these results by calculating the localized superconducting amplitudes that emerge out of charge inhomogeneities, which forms a mesoscopic granular superconductor with an array of Josephson junctions, whose average couplings determine the critical temperature $T_{\rm c}$. The calculations agree with the experiments and both yield that underdoped and overdoped compounds have superconducting long-range order by the same mechanism. |
| title | Common superconducting transition in under and overdoped cuprate superconductors |
| topic | Superconductivity |
| url | https://arxiv.org/abs/2507.01718 |