38,011 research outputs found

    Combined analysis of the decays τ−→KSπ−ντ\tau^-\to K_S\pi^-\nu_\tau and τ−→K−ηντ\tau^-\to K^-\eta\nu_\tau

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    In a combined study of the decay spectra of τ−→KSπ−ντ\tau^-\to K_S\pi^-\nu_\tau and τ−→K−ηντ\tau^-\to K^-\eta\nu_\tau decays within a dispersive representation of the required form factors, we illustrate how the K∗(1410)K^*(1410) resonance parameters, defined through the pole position in the complex plane, can be extracted with improved precision as compared to previous studies. While we obtain a substantial improvement in the mass, the uncertainty in the width is only slightly reduced, with the findings MK∗′=1304±17 M_{K^{*\prime}}=1304 \pm 17\,MeV and ΓK∗′=171±62 \Gamma_{K^{*\prime}} = 171 \pm 62\,MeV. Further constraints on the width could result from updated analyses of the KπK\pi and/or KηK\eta spectra using the full Belle-I data sample. Prospects for Belle-II are also discussed. As the K−π0K^-\pi^0 vector form factor enters the description of the decay τ−→K−ηντ\tau^-\to K^-\eta\nu_\tau, we are in a position to investigate isospin violations in its parameters like the form factor slopes. In this respect also making available the spectrum of the transition τ−→K−π0ντ\tau^-\to K^-\pi^0\nu_\tau would be extremely useful, as it would allow to study those isospin violations with much higher precision.Comment: 20 pages, 1figur

    Confinement of electrons in layered metals

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    We analyze the out of plane hopping in models of layered systems where the in--plane properties deviate from Landau's theory of a Fermi liquid. We show that the hopping term acquires a non trivial energy dependence, due to the coupling to in plane excitations, and can be either relevant or irrelevant at low energies or temperatures. The latter is always the case if the Fermi level lies close to a saddle point in the dispersion relation.Comment: 4 pages, 1 eps figur

    Suspensions Thermal Noise in the LIGO Gravitational Wave Detector

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    We present a calculation of the maximum sensitivity achievable by the LIGO Gravitational wave detector in construction, due to limiting thermal noise of its suspensions. We present a method to calculate thermal noise that allows the prediction of the suspension thermal noise in all its 6 degrees of freedom, from the energy dissipation due to the elasticity of the suspension wires. We show how this approach encompasses and explains previous ways to approximate the thermal noise limit in gravitational waver detectors. We show how this approach can be extended to more complicated suspensions to be used in future LIGO detectors.Comment: 28 pages, 13 figure

    Cyclic homogeneous Riemannian manifolds

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    In spin geometry, traceless cyclic homogeneous Riemannian manifolds equipped with a homogeneous spin structure can be viewed as the simplest manifolds after Riemannian symmetric spin spaces. In this paper, we give some characterizations and properties of cyclic and traceless cyclic homogeneous Riemannian manifolds and we obtain the classification of simply-connected cyclic homogeneous Riemannian manifolds of dimension less than or equal to four. We also present a wide list of examples of non-compact irreducible Riemannian 33-symmetric spaces admitting cyclic metrics and give the expression of these metrics

    Tensorial perturbations in the bulk of inflating brane worlds

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    In this paper we consider the stability of some inflating brane-world models in quantum cosmology. It is shown that whereas the singular model based on the construction of inflating branes from Euclidean five-dimensional anti-de Sitter space is unstable to tensorial cosmological perturbations in the bulk, the nonsingular model which uses a five-dimensional asymptotically anti-de Sitter wormhole to construct the inflating branes is stable to these perturbations.Comment: 4 pages, RevTex, to appear in Phys. Rev.

    Homogeneous spin Riemannian manifolds with the simplest Dirac operator

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    We show the existence of nonsymmetric homogeneous spin Riemannian manifolds whose Dirac operator is like that on a Riemannian symmetric spin space. Such manifolds are exactly the homogeneous spin Riemannian manifolds (M,g)(M,g) which are traceless cyclic with respect to some quotient expression M=G/KM=G/K and reductive decomposition g=k⊕m\mathfrak{g} = \mathfrak{k} \oplus \mathfrak{m}. Using transversally symmetric fibrations of noncompact type, we give a list of them
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