1,723,540 research outputs found

    Mathematical structures of space-time

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    At first we introduce the space-time manifold and we compare some aspects of Riemannian and Lorentzian geometry such as the distance function and the relations between topology and curvature. We then define spinor structures in general relativity, and the conditions for their existence are discussed. The causality conditions are studied through an analysis of strong causality, stable causality and global hyperbolicity. In looking at the asymptotic structure of space-time, we focus on the asymptotic symmetry group of Bondi, Metzner and Sachs, and the b-boundary construction of Schmidt. The Hamiltonian structure of space-time is also analyzed, with emphasis on Ashtekar's spinorial variables. Finally, the question of a rigorous theory of singularities in space-times with torsion is addressed, describing in detail recent work by the author. We define geodesics as curves whose tangent vector moves by parallel transport. This is different from what other authors do, because their definition of geodesics only involves the Christoffel symbols, though studying theories with torsion. We then prove how to extend Hawking's singularity theorem without causality assumptions to the space-time of the ECSK theory. This is achieved studying the generalized Raychaudhuri equation in the ECSK theory, the conditions for the existence of conjugate points and properties of maximal timelike geodesics. Our result can also be interpreted as a no-singularity theorem if the torsion tensor does not obey some additional conditions. Namely, it seems that the occurrence of singularities in closed cosmological models based on the ECSK theory is less generic than in general relativity. Our work should be compared with important previous papers. There are some relevant differences, because we rely on a different definition of geodesics, we keep the field equations of the ECSK theory in their original form rather than casting them in a form similar to general relativity with a modified energy-momentum tensor, and we emphasize the role played by the full extrinsic curvature tensor and by the variation formulae

    Analysis of unsupported gait in toddlers with autism

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    Analysis of unsupported gait in toddlers with autism. Esposito G, Venuti P, Apicella F, Muratori F. Department of Cognitive Science and Education, University of Trento, Italy. [email protected] AIMS: A number of studies have suggested the importance of motor development in autism. Motor development has been considered a possible bio-marker of autism since it does not depend on either social or linguistic development. In this study, using retrospective video analysis we investigated the first unsupported gait in toddlers with autism. METHODS: Fifty-five toddlers, belonging to three groups were recruited: toddlers with autistic disorder (AD, n=20, age 14.2mo, sd 1.4mo) and as comparison groups: typically developing toddlers (TD, n=20, age 12.9mo, sd 1.1mo) and toddlers with non-autistic developmental delays of mixed aetiology (DD, n=15, age 13.1mo, sd 0.8mo). The Walking Observation Scale (WOS) and the Positional Pattern for Symmetry during Walking (PPSW) were used to gather data on the first unsupported gait. The WOS includes 11 items that analyze gait through three axes: foot movements; arm movements; general movements while the PPSW analyses static and dynamical symmetry during gait. RESULTS: Our results have identified significant differences in gait patterns among the group of toddlers with AD as opposed to the control groups. Significant differences between AD and the two control groups were found for both WOS (p<.001) and PPSW (p<.001). CONCLUSION: The specificity of motor disturbances we have identified in autism (postural asymmetry) is consistent with previous findings that implicated cerebellar involvement in the motor symptoms of autism

    From ordinary to partial differential equations

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    This book is addressed to mathematics and physics students who want to develop an interdisciplinary view of mathematics, from the age of Riemann, Poincaré and Darboux to basic tools of modern mathematics. It enables them to acquire the sensibility necessary for the formulation and solution of difficult problems, with an emphasis on concepts, rigour and creativity. It consists of eight self-contained parts: ordinary differential equations; linear elliptic equations; calculus of variations; linear and non-linear hyperbolic equations; parabolic equations; Fuchsian functions and non-linear equations; the functional equations of number theory; pseudo-differential operators and pseudo-differential equations. The author leads readers through the original papers and introduces new concepts, with a selection of topics and examples that are of high pedagogical value

    New photon propagators in quantum electrodynamics

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    A Lagrangian for quantum electrodynamics is found which makes it explicit that the photon mass is eventually set to zero in the physical part on observational ground. It remains possible to obtain a counterterm Lagrangian where the only non-gauge-invariant term is proportional to the squared divergence of the potential, while the photon propagator in momentum space falls off like k^{−2} at large k, which indeed agrees with perturbative renormalizability. The resulting radiative corrections to the Coulomb potential in QED are also shown to be gauge-independent. A fundamental role of the space of 4-vectors with components given by 4×4 matrices is therefore suggested by our scheme, where such matrices can be used to define a single gauge-averaging functional in the path integral

    New application of noncanonical maps in quantum mechanics

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    One invertible and one unitary operator can be used to reproduce the effect of a q-deformed commutator of annihilation and creation operators. The original annihilation and creation operators are mapped into new operators, not conjugate to each other, whose standard commutator equals the identity plus a correction proportional to the original number operator. The consistency condition for the existence of this new set of operators is derived, by exploiting the Stone theorem on 1-parameter unitary groups. The above scheme leads to modified “equations of motion” which do not preserve the properties of the original first-order set for annihilation and creation operators. Their relation with commutation relations is also studied

    Local supersymmetry in one-loop quantum cosmology

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    The contribution of physical degrees of freedom to the one-loop amplitudes of Euclidean supergravity is here evaluated in the case of flat Euclidean backgrounds bounded by a three-sphere, recently considered in perturbative quantum cosmology. In Euclidean supergravity, the spin-3/2 potential has the pair of independent spatial components (psi_{i}^{A}, {widetilde psi}_{i}^{A'}). Massless gravitinos are here subject to the following local boundary conditions on S**3: sqrt{2} ; {_{e}n_{A}^{; ; A'}} psi_{i}^{A}=pm {widetilde psi}_{i}^{A'}, where {_{e}n_{A}^{; ; A'}} is the Euclidean normal to the three-sphere boundary. The physical degrees of freedom (denoted by PDF) are picked out imposing the supersymmetry constraints and choosing the gauge condition e_{AA'}^{; ; ; ; ; i}psi_{i}^{A}=0, e_{AA'}^{; ; ; ; ; i}{widetilde psi}_{i}^{A'}=0. These local boundary conditions are then found to imply the eigenvalue condition {[J_{n+2}(E)]}^{2}-{[J_{n+3}(E)]}^{2}=0, ; forall n geq 0, with degeneracy (n+4)(n+1). One can thus apply again a zeta-function technique previously used for massless spin-1over2{1over 2} fields. The PDF contribution to the full zeta(0) value is found to be =-289/360. Remarkably, for the massless gravitino field the PDF method and local boundary conditions lead to a result for zeta(0) which is equal to the PDF value one obtains using spectral boundary conditions on S**3

    Nonlocal boundary conditions in Euclidean quantum gravity

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    Non-local boundary conditions for Euclidean quantum gravity are proposed, consisting of an integro-differential boundary operator acting on metric perturbations. In this case, the operator P on metric perturbations is of Laplace type, subject to non-local boundary conditions; in contrast, its adjoint is the sum of a Laplacian and of a singular Green operator, subject to local boundary conditions. Self-adjointness of the boundary value problem is correctly formulated by looking at Dirichlet-type and Neumann-type realizations of the operator P, following recent results in the literature. The set of non-local boundary conditions for perturbative modes of the gravitational field is written in general form on the Euclidean 4-ball. For a particular choice of the non-local boundary operator, explicit formulae for the boundary value problem are obtained in terms of a finite number of unknown functions, but subject to some consistency conditions. Among the related issues, the problem arises of whether non-local symmetries exist in Euclidean quantum gravity

    Asymptotic heat kernels in quantum field theory

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    Asymptotic expansions were first introduced by Henri Poincar ́e in 1886. This paper describes their application to the semi-classical evaluation of amplitudes in quantum field theory with boundaries. By using zeta-function regularization, the conformal anomaly for a massless spin-1/2 field in flat Euclidean backgrounds with boundary is obtained on imposing locally supersymmetric boundary conditions. The quantization program for gauge fields and gravitation in the presence of boundaries is then introduced by focusing on conformal anomalies for higher-spin fields. The conditions under which the covariant Schwinger-DeWitt and the non-covariant, mode-by-mode analysis of quantum amplitudes agree are described

    Gauge-averaging functionals for Euclidean Maxwell theory in the presence of boundaries

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    This paper studies the one-loop expansion of the amplitudes of electromagnetism about flat Euclidean backgrounds bounded by a 3-sphere, recently considered in perturbative quantum cosmology, by using zeta-function regularization. For a specific choice of gauge averaging functional, the contributions to the full zeta(0) value owed to physical degrees offreedom, decoupled gauge mode, coupled gauge modes, and Paddeev-Popov ghost field are derived in detail, and alternative choices for such a functional are also studied. This analysis enables one to get a better understanding of different quantization techniques for gauge fields and gravitation in the presence of boundarie
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