TY - JOUR
T1 - Magnetic-field-induced phenomena in the paramagnetic superconductor Ute2
AU - Knafo, William
AU - Vališka, Michal
AU - Braithwaite, Daniel
AU - Lapertot, Gérard
AU - Knebel, Georg
AU - Pourret, Alexandre
AU - Brison, Jean Pascal
AU - Flouquet, Jacques
AU - Aoki, Dai
N1 - Publisher Copyright:
© 2019 The Physical Society of Japan
PY - 2019
Y1 - 2019
N2 - We present magnetoresistivity measurements on the heavy-fermion superconductor UTe2 in pulsed magnetic fields μ0H up to 68T and temperatures T from 1.4 to 80K. Magnetic fields applied along the three crystallographic directions a (easy magnetic axis), b, and c (hard magnetic axes), are found to induce different phenomena—depending on the field direction—beyond the low-field suppression of the superconducting state. For H ∥ a, a broad anomaly in the resistivity is observed at 0H ’ 10T and T = 1.4K. For H ∥ c, no magnetic transition nor crossover are observed. For H ∥ b, a sharp first-order-like step in the resistivity indicates a metamagnetic transition at the field 0Hm ’ 35T. When the temperature is raised signature of first-order metamagnetism is observed up to a critical endpoint at TCEP ’ 7K. At higher temperatures a crossover persists up to 28K, i.e., below the temperature Tmax ¼ 35K where the magnetic susceptibility is maximal. A sharp maximum in the Fermi-liquid quadratic coefficient A of the low-temperature resistivity is found at Hm. It indicates an enhanced effective mass associated with critical magnetic fluctuations, possibly coupled with a Fermi surface instability.
AB - We present magnetoresistivity measurements on the heavy-fermion superconductor UTe2 in pulsed magnetic fields μ0H up to 68T and temperatures T from 1.4 to 80K. Magnetic fields applied along the three crystallographic directions a (easy magnetic axis), b, and c (hard magnetic axes), are found to induce different phenomena—depending on the field direction—beyond the low-field suppression of the superconducting state. For H ∥ a, a broad anomaly in the resistivity is observed at 0H ’ 10T and T = 1.4K. For H ∥ c, no magnetic transition nor crossover are observed. For H ∥ b, a sharp first-order-like step in the resistivity indicates a metamagnetic transition at the field 0Hm ’ 35T. When the temperature is raised signature of first-order metamagnetism is observed up to a critical endpoint at TCEP ’ 7K. At higher temperatures a crossover persists up to 28K, i.e., below the temperature Tmax ¼ 35K where the magnetic susceptibility is maximal. A sharp maximum in the Fermi-liquid quadratic coefficient A of the low-temperature resistivity is found at Hm. It indicates an enhanced effective mass associated with critical magnetic fluctuations, possibly coupled with a Fermi surface instability.
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U2 - 10.7566/JPSJ.88.063705
DO - 10.7566/JPSJ.88.063705
M3 - Article
AN - SCOPUS:85067296625
SN - 0031-9015
VL - 88
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 6
M1 - 063705
ER -