996 research outputs found

    Amensie en demensie met verwysing na die intellek

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    ,,Es ist der Geist der sich den Kórper baut” het Goethe gesê en hy het daardeur die monistiese begrip in die psigiatrie beklemtoon. Dwarsdeur die eeue het die ontwikkelingsgeskiedenis van die mens maar telkens getoon hoedat daar by die mens veral, nie anders gedink kan word dan as 'n psigosomatiese eenheid nie.

    Critical Collapse in Einstein-Gauss-Bonnet Gravity in Five and Six Dimensions

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    Einstein-Gauss-Bonnet gravity (EGB) provides a natural higher dimensional and higher order curvature generalization of Einstein gravity. It contains a new, presumably microscopic, length scale that should affect short distance properties of the dynamics, such as Choptuik scaling. We present the results of a numerical analysis in generalized flat slice co-ordinates of self-gravitating massless scalar spherical collapse in five and six dimensional EGB gravity near the threshold of black hole formation. Remarkably, the behaviour is universal (i.e. independent of initial data) but qualitatively different in five and six dimensions. In five dimensions there is a minimum horizon radius, suggestive of a first order transition between black hole and dispersive initial data. In six dimensions no radius gap is evident. Instead, below the GB scale there is a change in the critical exponent and echoing period.Comment: 21 pages, 39 figures, a couple of references and two new figures adde

    Quantum Griffiths phase in CePd(1-x)Rh(x) with x ~ 0.8

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    The magnetic field dependence of the magnetisation (MM) and the temperature dependence of the ac susceptibility (χ=dM/dH\chi' = dM/dH) of CePd(1-x)Rh(x) single crystals with 0.80x0.860.80 \leq x \leq 0.86 are analysed within the frame of the quantum Griffiths phase scenario, which predicts MHλM \propto H^{\lambda} and χTλ1\chi' \propto T^{\lambda-1} with 0λ10 \leq \lambda \leq 1. All MM vs HH and χ\chi' vs TT data follow the predicted power-law behaviour. The parameter λ\lambda, extracted from χ(T)\chi'(T), is very sensitive to the Rh content xx and varies systematically with xx from -0.1 to 0.4. The value of λ\lambda, derived from M(H)M(H) measurements on a \cpr single crystal, seems to be rather constant, λ0.2\lambda \approx 0.2, in a broad range of temperatures between 0.05 and 2 K and fields up to about 10 T. All observed signatures and the λ\lambda values are thus compatible with the quantum Griffiths scenario.Comment: 4 pages, 3 figure

    Huge First-Order Metamagnetic Transition in the Paramagnetic Heavy-Fermion System CeTiGe

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    We report on the observation of large, step-like anomalies in the magnetization (ΔM=0.74\Delta M = 0.74\,μB\mu_{\rm B}/Ce), in the magnetostriction (Δl/l0=2.0103\Delta l/l_{0} = 2.0 \cdot 10^{-3}), and in the magnetoresistance in polycrystals of the paramagnetic heavy-fermion system CeTiGe at a critical magnetic field μ0Hc\mu_0 H_c \approx 12.5\,T at low temperatures. The size of these anomalies is much larger than those reported for the prototypical heavy-fermion metamagnet CeRu2_2Si2_2. Furthermore, hysteresis between increasing and decreasing field data indicate a real thermodynamic, first-order type of phase transition, in contrast to the crossover reported for CeRu2_2Si2_2. Analysis of the resistivity data shows a pronounced decrease of the electronic quasiparticle mass across HcH_c. These results establish CeTiGe as a new metamagnetic Kondo-lattice system, with an exceptionally large, metamagnetic transition of first-order type at a moderate field.Comment: 5 pages, 4 figure

    Non-Fermi liquid states in the pressurized CeCu2(Si1xGex)2CeCu_2(Si_{1-x}Ge_x)_2 system: two critical points

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    In the archetypal strongly correlated electron superconductor CeCu2_2Si2_2 and its Ge-substituted alloys CeCu2_2(Si1x_{1-x}Gex_{x})2_2 two quantum phase transitions -- one magnetic and one of so far unknown origin -- can be crossed as a function of pressure \cite{Yuan 2003a}. We examine the associated anomalous normal state by detailed measurements of the low temperature resistivity (ρ\rho) power law exponent α\alpha. At the lower critical point (at pc1p_{c1}, 1α1.51\leq\alpha\leq 1.5) α\alpha depends strongly on Ge concentration xx and thereby on disorder level, consistent with a Hlubina-Rice-Rosch scenario of critical scattering off antiferromagnetic fluctuations. By contrast, α\alpha is independent of xx at the upper quantum phase transition (at pc2p_{c2}, α1\alpha\simeq 1), suggesting critical scattering from local or Q=0 modes, in agreement with a density/valence fluctuation approach.Comment: 4 pages, including 4 figures. New results added. Significant changes on the text and Fig.

    Scanning a photonic crystal slab nanocavity by condensation of xenon

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    Allowing xenon or nitrogen gas to condense onto a photonic crystal slab nanocavity maintained at 10–20 K results in shifts of the nanocavity mode wavelength by as much as 5 nm (~=4 meV). This occurs in spite of the fact that the mode defect is achieved by omitting three holes to form the spacer. This technique should be useful in changing the detuning between a single quantum dot transition and the nanocavity mode for cavity quantum electrodynamics experiments, such as mapping out a strong coupling anticrossing curve. Compared with temperature scanning, it has a much larger scan range and avoids phonon broadening

    Flight Evaluation of an Aircraft with Side and Center Stick Controllers and Rate-Limited Ailerons

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    As part of an ongoing government and industry effort to study the flying qualities of aircraft with rate-limited control surface actuators, two studies were previously flown to examine an algorithm developed to reduce the tendency for pilot-induced oscillation when rate limiting occurs. This algorithm, when working properly, greatly improved the performance of the aircraft in the first study. In the second study, however, the algorithm did not initially offer as much improvement. The differences between the two studies caused concern. The study detailed in this paper was performed to determine whether the performance of the algorithm was affected by the characteristics of the cockpit controllers. Time delay and flight control system noise were also briefly evaluated. An in-flight simulator, the Calspan Learjet 25, was programmed with a low roll actuator rate limit, and the algorithm was programmed into the flight control system. Side- and center-stick controllers, force and position command signals, a rate-limited feel system, a low-frequency feel system, and a feel system damper were evaluated. The flight program consisted of four flights and 38 evaluations of test configurations. Performance of the algorithm was determined to be unaffected by using side- or center-stick controllers or force or position command signals. The rate-limited feel system performed as well as the rate-limiting algorithm but was disliked by the pilots. The low-frequency feel system and the feel system damper were ineffective. Time delay and noise were determined to degrade the performance of the algorithm
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