146 research outputs found
Anomalous Paramagnetic Effects in the Mixed State of LuNi2B2C
Anomalous paramagnetic effects in dc magnetization were observed in the mixed
state of LuNi2B2C, unlike any reported previously. It appears as a kink-like
feature for H > 30 kOe and becomes more prominent with increasing field. A
specific heat jump at the corresponding temperature suggests that the anomaly
is due to a true bulk transition. A magnetic flux transition from a square to
an hexagonal lattice is consistent with the anomaly.Comment: 5 pages, 4 figure
Evidence for the Coexistence of Anisotropic Superconducting Gap and Nonlocal Effects in the Non-magnetic Superconductor LuNi2B2C
A study of the dependence of the heat capacity Cp(alpha) on field angle in
LuNi2B2C reveals an anomalous disorder effect. For pure samples, Cp(alpha)
exhibits a fourfold variation as the field H < Hc2 is rotated in the [001]
plane, with minima along (alpha = 0). A slightly disordered sample,
however, develops anomalous secondary minima along for H > 1 T, leading
to an 8-fold pattern. The anomalous pattern is discussed in terms of coexisting
superconducting gap anisotropy and non-local effects.Comment: 5 pages, 4 figure
Magnetic field dependence of superconducting energy gaps in YNi2B2C: Evidence of multiband superconductivity
We present results of in field directional point contact spectroscopy (DPCS)
study in the quaternary borocarbide superconductor YNi2B2C, which is
characterized by a highly anisotropic superconducting gap function. For I||a,
the superconducting energy gap (D), decreases linearly with magnetic field and
vanishes around 3.25T which is well below the upper critical field (Hc2~6T)
measured at the same temperature (2.2K). For I||c, on the other hand, D
decreases weakly with magnetic field but the broadening parameter (G) increases
rapidly with magnetic field with the absence of any resolvable feature above
3.5T. From an analysis of the field variation of energy gaps and the zero bias
density of states we show that the unconventional gap function observed in this
material could originate from multiband superconductivity.Comment: 19 pages including figures (final version
TESS and CHEOPS discover two warm sub-Neptunes transiting the bright K-dwarf HD 15906
We report the discovery of two warm sub-Neptunes transiting the bright (G = 9.5 mag) K-dwarf HD 15906 (TOI 461, TIC 4646810). This star was observed by the Transiting Exoplanet Survey Satellite (TESS) in sectors 4 and 31, revealing two small transiting planets. The inner planet, HD 15906 b, was detected with an unambiguous period but the outer planet, HD 15906 c, showed only two transits separated by ∼ 734 d, leading to 36 possible values of its period. We performed follow-up observations with the CHaracterising ExOPlanet Satellite (CHEOPS) to confirm the true period of HD 15906 c and improve the radius precision of the two planets. From TESS, CHEOPS, and additional ground-based photometry, we find that HD 15906 b has a radius of 2.24 ± 0.08 R⊕ and a period of 10.924709 ± 0.000032 d, whilst HD 15906 c has a radius of 2.93+0.07−0.06 R⊕ and a period of 21.583298+0.000052−0.000055 d. Assuming zero bond albedo and full day-night heat redistribution, the inner and outer planet have equilibrium temperatures of 668 ± 13 K and 532 ± 10 K, respectively. The HD 15906 system has become one of only six multiplanet systems with two warm (≲ 700 K) sub-Neptune sized planets transiting a bright star (G ≤ 10 mag). It is an excellent target for detailed characterization studies to constrain the composition of sub-Neptune planets and test theories of planet formation and evolution
Virtual Recovery of Content from X-Ray Micro-Tomography Scans of Damaged Historic Scrolls
Part of this work was carried out with funding from the EPSRC (project EP/G010110/1, High defnition X-ray
microtomography and advanced visualisation techniques for information recovery from unopenable historical
documents), the China Postdoctoral Innovation Program (No. 230210342) and the China Scholarship Council
(File No. 201406020068
Hidden Magnetism and Quantum Criticality in the Heavy Fermion Superconductor CeRhIn5
With understood exceptions, conventional superconductivity does not coexist
with long-range magnetic order[1]. In contrast, unconventional
superconductivity develops near a boundary separating magnetically ordered and
magnetically disordered phases[2,3]. A maximum in the superconducting
transition temperature Tc develops where this boundary extrapolates to T=0 K,
suggesting that fluctuations associated with this magnetic quantum-critical
point are essential for unconventional superconductivity[4,5]. Invariably
though, unconventional superconductivity hides the magnetic boundary when T <
Tc, preventing proof of a magnetic quantum-critical point[5]. Here we report
specific heat measurements of the pressure-tuned unconventional superconductor
CeRhIn5 in which we find a line of quantum-phase transitions induced inside the
superconducting state by an applied magnetic field. This quantum-critical line
separates a phase of coexisting antiferromagnetism and superconductivity from a
purely unconventional superconducting phase and terminates at a quantum
tetracritical point where the magnetic field completely suppresses
superconductivity. The T->0 K magnetic field-pressure phase diagram of CeRhIn5
is well described with a theoretical model[6,7] developed to explain
field-induced magnetism in the high-Tc cuprates but in which a clear
delineation of quantum-phase boundaries has not been possible. These
experiments establish a common relationship among hidden magnetism, quantum
criticality and unconventional superconductivity in cuprate and heavy-electron
systems, such as CeRhIn5.Comment: journal reference adde
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