12,914 research outputs found

    Possible f-wave superconductivity in Sr2_2RuO4_4?

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    Until recently it has been believed that the superconductivity in Sr2_2RuO4_4 is described by p-wave pairing. However, both the recent specific heat and the magnetic penetration depth measurements on the purest single crystals of Sr2_2RuO4_4 appear to be explained more consistently in terms of f-wave superconductivity. In order to further this hypothesis, we study theoretically the thermodynamics and thermal conductivity of f-wave superconductors in a planar magnetic field. We find the simple expressions for these quantities when HHc2H \ll H_{c2} and TTcT \ll T_{c}, which should be readily accessible experimentally.Comment: 6 pages, 2 figure

    Critical Current of the Spin-Triplet Superconducting Phase in Sr2_2RuO4_4

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    There have been two different proposals for the spin-triplet order parameter of the superconducting phase in Sr2_2RuO4_4; an ff-wave order parameter and the multigap model where some of the bands have the line node. In an effort to propose an experiment that can distinguish two cases, we study the behavior of the supercurrent and compute the critical current for these order parameters when the sample is a thin film with the thickness dξd \ll \xi where ξ\xi is the coherence length. It is found that the supercurrent behaves very differently in two models. This will serve as a sharp test for the identification of the correct order parameter.Comment: 4 pages, 1 figur

    Threshold electric field in unconventional density waves

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    As it is well known most of charge density wave (CDW) and spin density wave (SDW) exhibit the nonlinear transport with well defined threshold electric field E_T. Here we study theoretically the threshold electric field of unconventional density waves. We find that the threshold field increases monotonically with temperature without divergent behaviour at T_c, unlike the one in conventional CDW. The present result in the 3D weak pinning limit appears to describe rather well the threshold electric field observed recently in the low-temperature phase (LTP) of alpha-(BEDT-TTF)_2KHg(SCN)_4.Comment: 4 pages, 2 figure

    Thermal conductivity in B- and C- phase of UPt_3

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    Although the superconductivity in UPt_3 is one of the most well studied, there are still lingering questions about the nodal directions in the B and C phase in the presence of a magnetic field. Limiting ourselves to the low temperature regime (T<<Delta(0)), we study the magnetothermal conductivity with in semiclassical approximation using Volovik's approach. The angular dependence of the magnetothermal conductivity for an arbitrary field direction should clarify the nodal structure in UPt_3.Comment: 4 pages, 5 figure

    Electronic Quantum Monte Carlo Calculations of Atomic Forces, Vibrations, and Anharmonicities

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    Atomic forces are calculated for first-row monohydrides and carbon monoxide within electronic quantum Monte Carlo (QMC). Accurate and efficient forces are achieved by using an improved method for moving variational parameters in variational QMC. Newton's method with singular value decomposition (SVD) is combined with steepest descent (SD) updates along directions rejected by the SVD, after initial SD steps. Dissociation energies in variational and diffusion QMC agree well with experiment. The atomic forces agree quantitatively with potential energy surfaces, demonstrating the accuracy of this force procedure. The harmonic vibrational frequencies and anharmonicity constants, derived from the QMC energies and atomic forces, also agree well with experimental values.Comment: 6 pages, 2 figures; updated conten

    Novel vortex lattice transition in d-wave superconductors

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    We study the vortex state in a magnetic field parallel to the cc axis in the framework of the extended Ginzburg Landau equation. We find the vortex acquires a fourfold modulation proportional to cos(4ϕ)\cos(4\phi) where ϕ\phi is the angle r{\bf r} makes with the aa-axis. This term gives rise to an attractive interaction between two vortices when they are aligned parallel to (1,1,0)(1,1,0) or (1,1,0)(1,-1,0). We predict the first order vortex lattice transition at B=Hcrκ1Hc2(t)B=H_{cr}\sim \kappa^{-1} H_{c2}(t) from triangular into the square lattice tilted by 4545^\circ from the aa axis. This gives the critical field HcrH_{cr} a few Tesla for YBCO and Bi2212 monocrystals at low temperatures (T10KT\leq 10 K).Comment: 6 pages, 4 figure

    Neural-Network Vector Controller for Permanent-Magnet Synchronous Motor Drives: Simulated and Hardware-Validated Results

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    This paper focuses on current control in a permanentmagnet synchronous motor (PMSM). The paper has two main objectives: The first objective is to develop a neural-network (NN) vector controller to overcome the decoupling inaccuracy problem associated with conventional PI-based vector-control methods. The NN is developed using the full dynamic equation of a PMSM, and trained to implement optimal control based on approximate dynamic programming. The second objective is to evaluate the robust and adaptive performance of the NN controller against that of the conventional standard vector controller under motor parameter variation and dynamic control conditions by (a) simulating the behavior of a PMSM typically used in realistic electric vehicle applications and (b) building an experimental system for hardware validation as well as combined hardware and simulation evaluation. The results demonstrate that the NN controller outperforms conventional vector controllers in both simulation and hardware implementation

    Low-lying excitations around a single vortex in a d-wave superconductor

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    A full quantum-mechanical treatment of the Bogoliubov-de Gennes equation for a single vortex in a d-wave superconductor is presented. First, we find low-energy states extended in four diagonal directions, which have no counterpart in a vortex of s-wave superconductors. The four-fold symmetry is due to 'quantum effect', which is enhanced when pFξp_{F}\xi is small. Second, for pFξ1p_{F}\xi \sim 1, a peak with a large energy gap E0ΔE_{0}\sim \Delta is found in the density of states, which is due to the formation of the lowest bound states.Comment: 7pages, Revte

    Helstrom Theorem by No-Signaling Condition

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    We prove a special case of Helstrom theorem by using no-signaling condition in the special theory of relativity that faster-than-light communication is impossible.Comment: Minor corrections (A reference added, discussion part deleted, typos in equations corrected), 2 pages, RevTe
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