Thermodynamic evidence for the anisotropic field-induced change of the superconducting order parameter in the chiral superconductor candidate UTe<sub>2</sub>.
ORAL
Abstract
UTe2 is an unconventional superconductor widely believed to host a spin-triplet ground state. We present measurements of the specific heat C(H, T) of a high-quality single crystal sample of UTe2 at low temperature (70 mK < T < 2 K) and with magnetic fields to 12 T applied along the three principal crystallographic axes.
Our sample of UTe2 exhibits a single specific heat anomaly at the superconducting transition temperature Tc ≈ 2 K and a small zero-field residual Sommerfeld coefficient γ0 = C/T (T=0) ≈ 10 mJ mol-1K-2. The magnetic field evolution of the residual Sommerfeld coefficient γ0(H) is distinct for the three field directions. In magnetic fields to 4 T for fields along a, b, and c axes, we find that γ0 ≈ αi√H, with i=a,b,c, as expected for a nodal superconductor; however, we observe a striking change of behavior of γ0(H) above 4 T. A well-pronounced kink in γ0(H) is observed at 4 T for H || a,b, whereas a smooth change from square-root to linear behavior is observed around 4 T for H || c. These results strongly indicate that the zero-field superconducting ground state is stable to 4 T and undergoes a field-induced change above 4 T. At low fields, the nodes appear to be predominantly located in the ab plane. Above 4 T, the change in the superconducting order parameter is strongest when the field is applied in the ab plane, with nodes moving away from the direction of the applied field. We will discuss the implications of our results for the determination of the superconducting order parameter in UTe2 at high fields.
Our sample of UTe2 exhibits a single specific heat anomaly at the superconducting transition temperature Tc ≈ 2 K and a small zero-field residual Sommerfeld coefficient γ0 = C/T (T=0) ≈ 10 mJ mol-1K-2. The magnetic field evolution of the residual Sommerfeld coefficient γ0(H) is distinct for the three field directions. In magnetic fields to 4 T for fields along a, b, and c axes, we find that γ0 ≈ αi√H, with i=a,b,c, as expected for a nodal superconductor; however, we observe a striking change of behavior of γ0(H) above 4 T. A well-pronounced kink in γ0(H) is observed at 4 T for H || a,b, whereas a smooth change from square-root to linear behavior is observed around 4 T for H || c. These results strongly indicate that the zero-field superconducting ground state is stable to 4 T and undergoes a field-induced change above 4 T. At low fields, the nodes appear to be predominantly located in the ab plane. Above 4 T, the change in the superconducting order parameter is strongest when the field is applied in the ab plane, with nodes moving away from the direction of the applied field. We will discuss the implications of our results for the determination of the superconducting order parameter in UTe2 at high fields.
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Presenters
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Andrew J Woods
Los Alamos National Laboratory
Authors
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Andrew J Woods
Los Alamos National Laboratory
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Sangyun Lee
Los Alamos National Laboratory
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Priscila Rosa
Los Alamos National Laboratory
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Sean Thomas
Los Alamos National Laboratory
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Eric D Bauer
Los Alamos Natl Lab
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Shizeng Lin
Los Alamos National Laboratory, Los Alamos National Laboratory, New Mexico, USA, Los Alamos National Lab
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Roman Movshovich
Los Alamos Natl Lab, Los Alamos National Laboratory