The resistive transition to superconductivity in YbRh2Si2.
Invited
Abstract
We report electrical transport measurements on the putative heavy fermion superconductor YbRh2Si2 [1]. Measurements of the Nyquist noise were made on a high quality single crystal sample, over the temperature range 1K to 0.6 mK. On cooling below 12 mK, there is a clear transition from normal metal into a state in which the resistance decreases with decreasing temperature, initially approximately linearly, towards zero. We propose this to be a superconducting state, with phase fluctuations. The transition to a zero-resistance phase-coherent superconducting state is identified at 3.6 mK. The Nyquist noise was then studied in magnetic fields up to 9 mT, applied in plane, perpendicular to the c-axis. The zero resistance state was observed to be quenched above approximately 6 mT. At 9 mT we observe “re-entrance” of the normal state resistance at the lowest temperature. In the light of this critical field behavior, we discuss the nature of the superconductivity in the system, and the interplay with both electronic and nuclear magnetism. This work opens the prospect of tuning the magnetism by choice of Yb isotope in enriched samples, and studies at ultralow temperatures of electric transport at the field-tuned quantum critical point.
[1] E. Schuberth et al., Science, 351, 495 (2016).
[1] E. Schuberth et al., Science, 351, 495 (2016).
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Presenters
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John Saunders
Physics, Royal Holloway University of London
Authors
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Lev Levitin
Physics, Royal Holloway University of London
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Harriet van der Vliet
Physics, Royal Holloway University of London
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Jan Nyeki
Physics, Royal Holloway University of London
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Andrew Casey
Physics, Royal Holloway University of London
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Sandra Hamann
Max Planck Institute for Chemical Physics of Solids
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Alexander Steppke
Max Planck Institute for Chemical Physics of Solids
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Markus Koenig
Max Planck Institute for Chemical Physics of Solids
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Kristin Kliemt
Physics Institut, Goethe University
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Cornelius Krellner
Physics Institut, Goethe University
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Manuel Brando
Max Planck Institute for Chemical Physics of Solids
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John Saunders
Physics, Royal Holloway University of London