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Fermi-Surface Instabilities in the Heavy-Fermion Superconductor UTe2
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abstract
We present different transport measurements up to fields of 29~T in the recently discovered heavy-fermion superconductor UTe$_{2}$ with magnetic field $H$ applied along the easy magnetization a-axis of the body-centered orthorhombic structure. The thermoelectric power varies linearly with temperature above the superconducting transition, $T_{SC}= 1.5$ K, indicating that superconductivity develops in a Fermi liquid regime. As a function of field the thermolelectric power shows successive anomalies which are attributed to field-induced Fermi surface instabilities. These Fermi-surface instabilities appear at critical values of the magnetic polarization. Remarkably, the lowest magnetic field instability for $H\parallel a$ occurs for the same critical value of the magnetization (0.4 $\mu_B$) than the first order metamagnetic transition at 35~T for field applied along the $b$-axis. The estimated number of charge carriers at low temperature reveals a metallic ground state distinct from LDA calculations indicating that strong electronic correlations are a major issue in this compound.
Forward citations
Cited by 3 Pith papers
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Quasi-two-dimensional Fermi surfaces and unitary spin-triplet pairing in the heavy fermion superconductor UTe$_2$
UTe2 is predicted to host quasi-two-dimensional Fermi surfaces and a strong-spin-orbit-coupling unitary spin-triplet superconducting state with point nodes, ruling out non-unitary pairing.
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Insulator-metal transition and topological superconductivity in UTe2 from a first-principles calculation
The authors show that a GGA+U calculation with U above 1 eV turns insulating DFT UTe2 metallic, and the resulting Fermi surfaces imply time-reversal-invariant topological superconductivity with Majorana surface states...
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Point Node Gap Structure of Spin-Triplet Superconductor UTe2
Heat flow, magnetic penetration, and specific heat data on UTe2 are best explained by a spin-triplet superconducting gap with point nodes, once a fitted divergent specific heat term is removed.
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