Pressure-temperature phase diagram of YbNi<sub>2</sub>B<sub>2</sub>C
ORAL
Abstract
The RNi2B2C (R = Gd - Lu, Y) series have attracted much attention due to the interplay between superconductivity and local-magnetism. For the Lu, Tm - Dy, superconducting transition temperature Tc decrease and the AFM transition temperature TN increases and scales with de Gennes scaling at ambient pressure. However, YbNi2B2C displays neither superconductivity nor magnetism down to low temperature at ambient pressure but rather is a heavy fermion compound with γ ∼ 530 mJ/mol K2. Studies suggest YbNi2B2C might be close to a quantum critical point (QCP) on the nonmagnetic side in the Doniach phase diagram. Resistance of single-crystalline YbNi2B2C is measured under pressure up to 16 GPa down to 50 mK as an attempt to reach QCP. Temperature-pressure phase diagram will be presented and discussed.
*This work is supported by DOE/BES, Materials Science and Engineering Division under contract No. DE-AC02-07CH11358. L. X. was supported, in part, by the W. M. Keck Foundation V.S. acknowledges support by DOE/BES under contract No. DE-FG02-99ER45775. A. G. acknowledges support of RSF 16-12-10464 grant.
–
Presenters
Li Xiang
Department of Physics, Iowa State University, Ames Laboratory, Ames, Iowa 50011, USA
Ames Laboratory/Iowa State University
Physics, Iowa State University/Ames Laboratory
Iowa State University and Ames Laboratory
Authors
Li Xiang
Department of Physics, Iowa State University, Ames Laboratory, Ames, Iowa 50011, USA
Ames Laboratory/Iowa State University
Physics, Iowa State University/Ames Laboratory
Iowa State University and Ames Laboratory
Yuji Furukawa
Ames Laboratory, Iowa State University
Department of Physics, Iowa State University, Ames Laboratory, Ames, Iowa 50011, USA
Ames Laboratory and Dept. of Phys. and Astro.,, Iowa State Univ.
Iowa State University & Ames Lab
Ames Lab & Dept of Physics and Astronomy, Iowa State University
Iowa State University
Viktor V. Struzhkin
Carnegie Institution of Washington, Geophysical Laboratory, Washington, DC 20015, USA
Geophysical Laboratory, Carnegie Institution of Washington
Geophysical Laboratory, Carnegie Institute of Washington
Alexander Gavriliuk
FSRC Crystallography and Photonics of Russian Academy of Sciences, Moscow 119333, Russia
Sergey Budko
Iowa State University
Department of Physics, Iowa State University, Ames Laboratory, Ames, Iowa 50011, USA
Ames Laboratory, Iowa State University
Ames Laboratory/Iowa State University
Ames Laboratory and Dept. of Phys. and Astro.,, Iowa State Univ.
Ames Laboratory and Department of Physics & Astronomy, Iowa State University, Ames, IA 50010, USA
Ames Lab & Dept of Physics and Astronomy, Iowa State University
Physics, Iowa State University/Ames Laboratory
Iowa State University and Ames Laboratory
Paul Canfield
Ames Laboratory and Dept. of Physics, Iowa State University
Ames Laboratory, U.S. DOE, Iowa State University, Ames, Iowa 50011, USA.
Ames Laboratory
Iowa State University
Department of Physics, Iowa State University, Ames Laboratory, Ames, Iowa 50011, USA
Ames Laboratory, Iowa State University
Ames Laboratory/Iowa State University
Iowa State University and Ames Laboratory
Ames Laboratory and Iowa State University, Ames, IA, USA
Ames Laboratory and Dept. of Phys. and Astro.,, Iowa State Univ.
Ames Laboratory and Department of Physics & Astronomy, Iowa State University, Ames, IA 50010, USA
Ames Lab & Dept of Physics and Astronomy, Iowa State University
Department of Physics & Astronomy, Iowa State University
Department of physics and astronomy, Iowa State University/Ames Laboratory