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Abstract
The quantum vortex liquid (QVL) is an intriguing state of type-II superconductors in which intense quantum fluctuations of the superconducting (SC) order parameter destroy the Abrikosov lattice even at very low temperatures. Such a state has only rarely been observed, however, and remains poorly understood. One of the key questions is the precise origin of such intense quantum fluctuations and the role of nearby non-SC phases or quantum critical points in amplifying these effects. Here we report a high-field magnetotransport study of FeSe1−xSx and FeSe1−xTex which show a broad QVL regime both within and beyond their respective electron nematic phases. A clear correlation is found between the extent of the QVL and the strength of the superconductivity. This comparative study enables us to identify the essential elements that promote the QVL regime in unconventional superconductors and to demonstrate that the QVL regime itself is most extended wherever superconductivity is weakest.
In a quantum vortex liquid, the superconducting vortex lattice is melted by quantum fluctuations instead of thermal fluctuations. Here, the authors present high-field magnetotransport measurements of FeSe1−xSx and FeSe1−xTex, which provide evidence for a broad quantum vortex liquid regime.
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1 Radboud University, High Field Magnet Laboratory (HFML-EMFL) and Institute for Molecules and Materials, Nijmegen, Netherlands (GRID:grid.5590.9) (ISNI:0000000122931605); Institut za fiziku, Zagreb, Croatia (GRID:grid.454227.2) (ISNI:0000 0004 0383 9274)
2 Radboud University, High Field Magnet Laboratory (HFML-EMFL) and Institute for Molecules and Materials, Nijmegen, Netherlands (GRID:grid.5590.9) (ISNI:0000000122931605)
3 University of Tokyo, Department of Advanced Materials Science, Kashiwa, Japan (GRID:grid.26999.3d) (ISNI:0000 0001 2151 536X)
4 University of Bristol, H. H. Wills Physics Laboratory, Bristol, UK (GRID:grid.5337.2) (ISNI:0000 0004 1936 7603)
5 Radboud University, High Field Magnet Laboratory (HFML-EMFL) and Institute for Molecules and Materials, Nijmegen, Netherlands (GRID:grid.5590.9) (ISNI:0000000122931605); National Tsing Hua University, No. 101, Section. 2, Kuang-Fu Road, Center for Theory and Computation, Hsinchu, Taiwan (GRID:grid.38348.34) (ISNI:0000 0004 0532 0580)
6 University of Tokyo, Institute for Solid State Physics, Kashiwa, Japan (GRID:grid.26999.3d) (ISNI:0000 0001 2151 536X)
7 Hirosaki University, Graduate School of Science and Technology, Hirosaki, Japan (GRID:grid.257016.7) (ISNI:0000 0001 0673 6172)
8 Okayama University, Research Institute for Interdisciplinary Science, Kita-Ku, Japan (GRID:grid.261356.5) (ISNI:0000 0001 1302 4472)
9 Kyoto University, Department of Physics, Sakyo-Ku, Japan (GRID:grid.258799.8) (ISNI:0000 0004 0372 2033)
10 Radboud University, High Field Magnet Laboratory (HFML-EMFL) and Institute for Molecules and Materials, Nijmegen, Netherlands (GRID:grid.5590.9) (ISNI:0000000122931605); University of Bristol, H. H. Wills Physics Laboratory, Bristol, UK (GRID:grid.5337.2) (ISNI:0000 0004 1936 7603)