70,511 research outputs found

    Perception of the visual horizontal in normal and labyrinthine defective subjects during prolonged rotation

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    Oculogravic illusion - perception of visual horizontal in normal and inner ear defective subjects during prolonged rotatio

    Factors contributing to the delay in the perception of the oculogravic illusion

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    Horizontal perception change delay of man after counter rotation - effects of pre-exposure conditions on visual discrimination recover

    Influence of Contact Cues on the Perception of the Oculogravic Illusion

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    Influence of otolith and monotolith information in perception of oculogravic illusio

    The egocentric localization of the visual horizontal in normal and labyrinthine- defective observers as a function of head and body tilt

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    Egocentric localization of visual horizontal in normal and labyrinthine-defective observers as function of head and body til

    The RHMC algorithm for theories with unknown spectral bounds

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    The Rational Hybrid Monte Carlo (RHMC) algorithm extends the Hybrid Monte Carlo algorithm for lattice QCD simulations to situations involving fractional powers of the determinant of the quadratic Dirac operator. This avoids the updating increment (dtdt) dependence of observables which plagues the Hybrid Molecular-dynamics (HMD) method. The RHMC algorithm uses rational approximations to fractional powers of the quadratic Dirac operator. Such approximations are only available when positive upper and lower bounds to the operator's spectrum are known. We apply the RHMC algorithm to simulations of 2 theories for which a positive lower spectral bound is unknown: lattice QCD with staggered quarks at finite isospin chemical potential and lattice QCD with massless staggered quarks and chiral 4-fermion interactions (χ\chiQCD). A choice of lower bound is made in each case, and the properties of the RHMC simulations these define are studied. Justification of our choices of lower bounds is made by comparing measurements with those from HMD simulations, and by comparing different choices of lower bounds.Comment: Latex(Revtex 4) 25 pages, 8 postscript figure

    Beta lives - some statistical perspectives on the capital asset pricing model

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    This note summarizes some technical issues relevant to the use of the idea of excess return in empirical modelling. We cover the case where the aim is to construct a measure of expected return on an asset and a model of the CAPM type is used. We review some of the problems and show examples where the basic CAPM may be used to develop other results which relate the expected returns on assets both to the expected return on the market and other factors

    Helmet weight simulator

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    A device for providing acceleration cues to the helmet of a simulator pilot is described. Pulleys are attached to both shoulders of the pilot. A cable is attached to both sides of the helmet and extends through the pulleys to a takeup reel that is controlled by a torque motor. Control signals are applied to a servo system including the torque motor, the takeup reel and a force transducer which supplies the feedback signal. In one embodiment of the invention the force transducer is in the cable and in another it is in the takeup reel

    Nature of the spin liquid state of the Hubbard model on honeycomb lattice

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    Recent numerical work (Nature 464, 847 (2010)) indicates the existence of a spin liquid phase (SL) that intervenes between the antiferromagnetic and semimetallic phases of the half filled Hubbard model on a honeycomb lattice. To better understand the nature of this exotic phase, we study the quantum J1−J2J_1-J_2 spin model on the honeycomb lattice, which provides an effective description of the Mott insulating region of the Hubbard model. Employing the variational Monte Carlo approach, we analyze the phase diagram of the model, finding a phase transition between antiferromagnet and an unusual Z2Z_2 SL state at J2/J1≈0.08J_2/J_1\approx 0.08, which we identify as the SL phase of the Hubbard model. At higher J2/J1≳0.3J_2/J_1\gtrsim 0.3 we find a transition to a dimerized state with spontaneously broken rotational symmetry.Comment: 5 pages, 6 figure
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