Showing 1–20 of 41 results
/ Date/ Name
Aug 8, 2018A practical Single Source Shortest Path algorithm for random directed graphs with arbitrary weight in expecting linear timeMay 8, 2019Metamagnetic Transition in Heavy Fermion Superconductor UTe2Jul 28, 2023Superconducting-Spin Reorientation in Spin-Triplet Multiple Superconducting Phases of UTe2Oct 11, 2022New Gd-based magnetic compound GdPt$_2$B with a chiral crystal structureApr 26, 2022Magnetovolume Effect on the First-Order Metamagnetic Transition in UTe$_2$Mar 9, 2020Spin-Triplet Superconductivity in UTe2 and Ferromagnetic SuperconductorsMar 12, 2021Pressure induced multicriticality and electronic instability in quasi-kagome ferromagnet URhSnMay 18, 2021Magnetic Properties under Pressure in Novel Spin-Triplet Superconductor UTe2Mar 19, 2020Anisotropy of the Upper Critical Field in the Heavy-Fermion Superconductor UTe2 under PressureMar 21, 2025Efficient and Expressive Public Key Authenticated Encryption with Keyword Search in Multi-user ScenariosFeb 9, 2026Intimate relationship between spin configuration in the triplet pair and superconductivity in UTe$_2$Mar 6, 2019Unconventional Superconductivity in Heavy Fermion UTe2Feb 15, 2020Orientation of point nodes and nonunitary triplet pairing tuned by the easy-axis magnetization in UTe2Jun 4, 2019125Te-NMR Study on a Single Crystal of Heavy Fermion Superconductor UTe2Jan 19, 2022Slow Electronic Dynamics in the Paramagnetic State of UTe$_2$Jun 3, 2022First Observation of de Haas-van Alphen Effect and Fermi Surfaces in Unconventional Superconductor UTe2Mar 16, 2022Superconducting order parameter in UTe$_2$ determined by Knight shift measurementMay 2, 2023Low-temperature Magnetic Fluctuations Investigated by $^{125}$Te-NMR on the Uranium-based Superconductor UTe$_{2}$Jun 15, 2016Large Upper Critical Field of Superconductivity in the Single Crystal U6CoNov 5, 2024Clear Reduction in Spin Susceptibility and Superconducting Spin Rotation for $H \parallel a$ in the Early-Stage Sample of Spin-Triplet Superconductor UTe$_2$