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Superconducting phase diagram of H3S under high magnetic fields.

Shirin Mozaffari | Dan Sun | Vasily S Minkov | Alexander P Drozdov | Dmitry Knyazev | Jonathan B Betts | Mari Einaga | Katsuya Shimizu | Mikhail I Eremets | Luis Balicas | Fedor F Balakirev
Nature communications | 2019

The discovery of superconductivity at 260 K in hydrogen-rich compounds like LaH10 re-invigorated the quest for room temperature superconductivity. Here, we report the temperature dependence of the upper critical fields μ0Hc2(T) of superconducting H3S under a record-high combination of applied pressures up to 160 GPa and fields up to 65 T. We find that Hc2(T) displays a linear dependence on temperature over an extended range as found in multigap or in strongly-coupled superconductors, thus deviating from conventional Werthamer, Helfand, and Hohenberg (WHH) formalism. The best fit of Hc2(T) to the WHH formalism yields negligible values for the Maki parameter α and the spin-orbit scattering constant λSO. However, Hc2(T) is well-described by a model based on strong coupling superconductivity with a coupling constant λ ~ 2. We conclude that H3S behaves as a strong-coupled orbital-limited superconductor over the entire range of temperatures and fields used for our measurements.

Pubmed ID: 31175310

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Associated grants

  • Agency: National Science Foundation (NSF), International
    Id: DMR-1644779

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National High Magnetic Field Laboratory Advanced Magnetic Resonance Imaging and Spectroscopy Core Facility (tool)

RRID:SCR_017362

Facility offers array of solid state, solution state, MRI/S (animal and human), MR microscopy and diffusion capabilities and techniques. Among their machines is 900 MHz 105 mm bore magnet. Techniques and instruments are available at two different MagLab facilities in Florida, NMR-MRI/S Facility at MagLab headquarters near Florida State University in Tallahassee and Advanced Magnetic Resonance Imaging and Spectroscopy Facility (AMRIS) housed within McKnight Brain Institute at University of Florida in Gainesville.

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