1,325 research outputs found

    Pressure-temperature Phase Diagram of Polycrystalline UCoGe Studied by Resistivity Measurement

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    Recently, coexistence of ferromagnetism (T_Curie = 2.8K) and superconductivity (T_sc = 0.8K) has been reported in UCoGe, a compound close to a ferromagnetic instability at ambient pressure P. Here we present resistivity measurements under pressure on a UCoGe polycrystal. The phase diagram obtained from resistivity measurements on a polycrystalline sample is found to be qualitatively different to those of all other ferromagnetic superconductors. By applying high pressure, ferromagnetism is suppressed at a rate of 1.4 K/GPa. No indication of ferromagnetic order has been observed above P ~ 1GPa. The resistive superconducting transition is, however, quite stable in temperature and persists up to the highest measured pressure of about 2.4GPa. Superconductivity would therefore appear also in the paramagnetic phase. However, the appearance of superconductivity seems to change at a characteristic pressure P* ~ 0.8GPa. Close to a ferromagnetic instability, the homogeneity of the sample can influence strongly the electronic and magnetic properties and therefore bulk phase transitions may differ from the determination by resistivity measurements.Comment: 4 pages, 4 figures, submitted to J. Phys. Soc. Jp

    Absence of Meissner State and Robust Ferromagnetism in the Superconducting State of UCoGe: Possible Evidence of Spontaneous Vortex State

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    We report ac magnetic susceptibility and dc magnetization measurements on the superconducting ferromagnet UCoGe (with superconducting and Curie temperatures of TSC∼0.5T_{{\rm SC}} \sim 0.5~K and TCurie∼2.5T_{{\rm Curie}} \sim 2.5~K, respectively). In the normal, ferromagnetic state (TSC<T<TCurieT_{{\rm SC}} < T < T_{{\rm Curie}}), the magnetization curve exhibits a hysteresis loop similar to that of a regular itinerant ferromagnet. Upon lowering the temperature below TSCT_{{\rm SC}}, the spontaneous magnetization is unchanged, but the hysteresis is markedly enhanced. Even deeply inside the superconducting state, ferromagnetism is not completely shielded, and there is no Meissner region, a magnetic field region of H<Hc1H < H_{\rm c1} (a lower critical field). From these results, we suggest that UCoGe is the first material in which ferromagnetism robustly survives in the superconducting state and a spontaneous vortex state without the Meissner state is realized.Comment: 5 pages, 4 figures, to be published in J. Phys. Soc. Jp

    Microscopic Coexistence of Ferromagnetism and Superconductivity in Single-Crystal UCoGe

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    Unambiguous evidence for the microscopic coexistence of ferromagnetism and superconductivity in UCoGe (TCurie∼2.5T_{\rm Curie} \sim 2.5 K and TSCT_{\rm SC} ∼\sim 0.6 K) is reported from 59^{59}Co nuclear quadrupole resonance (NQR). The 59^{59}Co-NQR signal below 1 K indicates ferromagnetism throughout the sample volume, while nuclear spin-lattice relaxation rate 1/T11/T_1 in the ferromagnetic (FM) phase decreases below TSCT_{\rm SC} due to the opening of the superconducting(SC) gap. The SC state was found to be inhomogeneous, suggestive of a self-induced vortex state, potentially realizable in a FM superconductor. In addition, the 59^{59}Co-NQR spectrum around TCurieT_{\rm Curie} show that the FM transition in UCoGe possesses a first-order character, which is consistent with the theoretical prediction that the low-temperature FM transition in itinerant magnets is generically of first-order.Comment: 5 pages, 5 figure

    Muon spin rotation and relaxation in the superconducting ferromagnet UCoGe

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    We report zero-field muon spin rotation and relaxation measurements on the superconducting ferromagnet UCoGe. Weak itinerant ferromagnetic order is detected by a spontaneous muon spin precession frequency below the Curie temperature TC=3T_C = 3 K. The μ+\mu^+ precession frequency persists below the bulk superconducting transition temperature Tsc=0.5T_{sc} = 0.5 K, where it measures a local magnetic field Bloc=0.015B_{loc} = 0.015 T. The amplitude of the μ\muSR signal provides unambiguous proof for ferromagnetism present in the whole sample volume. We conclude ferromagnetism coexists with superconductivity on the microscopic scale.Comment: 4 pages, 3 figures, accepted for publication in PR
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