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TL;DRAbstract
We report the measurements of in-plane resistivity, Hall effect, and Nernst effect in Zn-doped ${\mathrm{YBa}}_{2}{\mathrm{Cu}}_{3}{\mathrm{O}}_{7\ensuremath{-}\ensuremath{\delta}}$ epitaxial thin films grown by pulsed laser deposition technique. The pseudogap temperature ${T}^{*}$, determined from the temperature dependence of resistivity, does not change significantly with Zn doping. Meanwhile the onset temperature $({T}^{\ensuremath{\nu}})$ of anomalous Nernst signal above ${T}_{c0}$, which is interpreted as evidence for vortex-like excitations, decreases sharply as the superconducting transition temperature ${T}_{c0}$ does. A significant decrease in the maximum of vortex Nernst signal in mixed state is also observed, which is consistent with the scenario that Zn impurities cause a decrease in the superfluid density and therefore suppress the superconductivity. The phase diagram of ${T}^{*}$, ${T}^{\ensuremath{\nu}}$, and ${T}_{c0}$ versus Zn content is presented and discussed.
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We report the measurements of in-plane resistivity, Hall effect, and Nernst effect in Zn-doped ${\mathrm{YBa}}_{2}{\mathrm{Cu}}_{3}{\mathrm{O}}_{7\ensuremath{-}\ensuremath{\delta}}$ epitaxial thin films grown by pulsed laser deposition technique. The pseudogap temperature ${T}^{*}$, determined from the temperature dependence of resistivity, does not change significantly with Zn doping. Meanwhile the onset temperature $({T}^{\ensuremath{\nu}})$ of anomalous Nernst signal above ${T}_{c0}$, which is interpreted as evidence for vortex-like excitations, decreases sharply as the superconducting transition temperature ${T}_{c0}$ does. A significant decrease in the maximum of vortex Nernst signal in mixed state is also observed, which is consistent with the scenario that Zn impurities cause a decrease in the superfluid density and therefore suppress the superconductivity. The phase diagram of ${T}^{*}$, ${T}^{\ensuremath{\nu}}$, and ${T}_{c0}$ versus Zn content is presented and discussed.
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