58,493 research outputs found

    P. Jensen: Über den galvanischen Schwindel. Pflügers Archiv f. d. ges. Physiol. Bd. 64. S. 182-222. 1896

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    P. JENSEN: ÜBER DEN GALVANISCHEN SCHWINDEL. PFLÜGERS ARCHIV F. D. GES. PHYSIOL. BD. 64. S. 182-222. 1896 Zeitschrift für Psychologie und Physiologie der Sinnesorgane (-) Zeitschrift für Psychologie und Physiologie der Sinnesorgane (13) (a0004) P. Jensen: Über den galvanischen Schwindel. Pflügers Archiv f. d. ges. Physiol. Bd. 64. S. 182-222. 1896 (13) (p0122

    Logarithmic variance profiles and the corresponding f-1 spectra of temperature fluctuations in turbulent Rayleigh-Bénard convection

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    We report experimental results for the temperature variance 2(z) and the corresponding frequency spectra P(f) in turbulent Rayleigh-Bénard convection (RBC) in a cylindrical sample of aspect ratioT= D/L = 1:00 (D = 1:12 m is the diameter and L = 1:12 m the height). The measurements were conducted in the Rayleigh-number range 1011 < Ra < 1:35 1014 and Pr ' 0:8. For Ra = 1:35x1014, 2(z) could be described well by a logarithmic dependence on the vertical position z in a range of z 1 < z < z 2 with z 1 ' 70 and z 2 = 0:1L. Here L=(2Nu) is the thickness of a thin thermal sublayer adjacent to the horizontal plate where the heat flux (denoted by the Nusselt number Nu) is carried mostly by thermal diffusion. In the log layer, we found that the temperature spectra had a significant frequency range over which P(f) f with close to 1. As Ra decreased, increased so that the log layer became thinner. At Ra = 2:05 1011, z 2 < z 1 and therefore there was no range for a log layer. Correspondingly, the temperature spectrum near the horizontal plate did not have the f1 scaling form either

    Evidence for the decay B0→J/ψω and measurement of the relative branching fractions of meson decays to J/ψη and J/ψη′

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    First evidence of the B 0 → J / ψ ω decay is found and the B s 0 → J / ψ η and B s 0 → J / ψ η ′ decays are studied using a dataset corresponding to an integrated luminosity of 1.0 fb -1 collected by the LHCb experiment in proton-proton collisions at a centre-of-mass energy of sqrt(s) = 7 TeV. The branching fractions of these decays are measured relative to that of the B 0 → J / ψ ρ 0 decay:frac(B (B 0 → J / ψ ω), B (B 0 → J / ψ ρ 0)) = 0.89 ± 0.19 (stat) - 0.13 + 0.07 (syst),frac(B (B s 0 → J / ψ η), B (B 0 → J / ψ ρ 0)) = 14.0 ± 1.2 (stat) - 1.5 + 1.1 (syst) - 1.0 + 1.1 (frac(f d, f s)),frac(B (B s 0 → J / ψ η ′), B (B 0 → J / ψ ρ 0)) = 12.7 ± 1.1 (stat) - 1.3 + 0.5 (syst) - 0.9 + 1.0 (frac(f d, f s)), where the last uncertainty is due to the knowledge of f d / f s, the ratio of b-quark hadronization factors that accounts for the different production rate of B 0 and B s 0 mesons. The ratio of the branching fractions of B s 0 → J / ψ η ′ and B s 0 → J / ψ η decays is measured to befrac(B (B s 0 → J / ψ η ′), B (B s 0 → J / ψ η)) = 0.90 ± 0.09 (stat) - 0.02 + 0.06 (syst)

    The Auslander-Gruson-Jensen Recollement

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    For any ring RR, the Auslander-Gruson-Jensen functor is the exact contravariant functor DA:fp(Mod(R),Ab)(mod(Rop),Ab)\textsf{D}_A:\textsf{fp}(\textsf{Mod}(R),\textsf{Ab})\longrightarrow(\textsf{mod}(R^{op}),\textsf{Ab}) sending representable functors $(X,\hspace{0.05cm}\underline{\ \ }\hspace{0.1cm} )totensorfunctors to tensor functors X\otimes\hspace{0.05cm}\underline{\ \ }\hspace{0.1cm} .Weshowthatthisfunctoradmitsafullyfaithfulleftadjoint. We show that this functor admits a fully faithful left adjoint \textsf{D}_Landafullyfaithfulrightadjoint and a fully faithful right adjoint \textsf{D}_R.Theleftadjoint. The left adjoint DL(mod(Rop),Ab)fp(Mod(R),Ab)\textsf{D}_L\:(\textsf{mod}(R^{op}),\textsf{Ab})\longrightarrow \textsf{fp}(\textsf{Mod}(R),\textsf{Ab})inducesanequivalenceofcategories induces an equivalence of categories fp(Mod(R),Ab){F  DAF=0}(mod(Rop),Ab)op\frac{\textsf{fp}(\textsf{Mod}(R),\textsf{Ab})}{\{F\ |\ \textsf{D}_A F=0\}}\cong(\textsf{mod}(R^{op}),\textsf{Ab})^{op}where where \{F \ |\ \textsf{D}_A F=0\}istheSerresubcategoryof is the Serre subcategory of \textsf{fp}(\textsf{Mod}(R),\textsf{Ab})consistingofallfunctors consisting of all functors Farisingfrompureexactsequences.Asaresult,thefunctor arising from pure exact sequences. As a result, the functor \textsf{D}_AisseentobeaSerrelocalizationfunctor.Therightadjoint is seen to be a Serre localization functor. The right adjoint DR:(mod(Rop),Ab)fp(Mod(R),Ab)\textsf{D}_R:(\textsf{mod}(R^{op}),\textsf{Ab})\longrightarrow \textsf{fp}(\textsf{Mod}(R),\textsf{Ab})togetherwith together with \textsf{D}_A$ restricts to the well known Auslander-Gruson-Jensen duality.Comment: 11 pages. Updating to match published versio

    An equivalent condition to the Jensen inequality for the generalized Sugeno integral

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    Abstract For the classical Jensen inequality of convex functions, i.e., H ( 1 μ ( D ) ∫ D f d μ ) ≤ 1 μ ( D ) ∫ D H ∘ f d μ , H(1μ(D)Dfdμ)1μ(D)DHfdμ,\begin{aligned} H \biggl(\frac{1}{\mu(D)} \int_{D}f\,d\mu \biggr)\leq\frac{1}{\mu (D)} \int_{D} H\circ f\,d\mu, \end{aligned} an equivalent condition is proved in the framework of the generalized Sugeno integral. Also, the necessary and sufficient conditions for the validity of the discrete form of the Jensen inequality for the generalized Sugeno integral are given

    Some new estimates of the ‘Jensen gap’

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    Abstract Let ( μ , Ω ) (μ,Ω)( \mu,\Omega ) be a probability measure space. We consider the so-called ‘Jensen gap’ J ( φ , μ , f ) = ∫ Ω φ ( f ( s ) ) d μ ( s ) − φ ( ∫ Ω f ( s ) d μ ( s ) ) J(φ,μ,f)=Ωφ(f(s))dμ(s)φ(Ωf(s)dμ(s)) J ( \varphi,\mu,f ) = \int_{\Omega}\varphi \bigl( f ( s ) \bigr)\,d\mu ( s ) -\varphi \biggl( \int_{\Omega }f ( s )\,d\mu ( s ) \biggr) for some classes of functions φ. Several new estimates and equalities are derived and compared with other results of this type. Especially the case when φ has a Taylor expansion is treated and the corresponding discrete results are pointed out

    Erratum to: Effect of moderate red wine intake on cardiac prognosis after recent acute myocardial infarction of subjects with Type 2 diabetes mellitus (Diabetic Medicine, (2006), 23, 9, (974-981), 10.1111/j.1464-5491.2006.01886.x)

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    In an article by Marfella et al, the author name C. Saron is incorrect and should be listed as C. Sardu. Therefore the correct author list is: R. Marfella, F. Cacciapuoti, M. Siniscalchi, F. C. Sasso, F. Marchese, F. Cinone, E. Musacchio, M. A. Marfella, L. Ruggiero, G. Chiorazzo, D. Liberti, G. Chiorazzo, G. F. Nicoletti, C. Sardu, F. D'Andrea, C. Ammendola, M. Verza and L. Coppola.In an article by Marfella et al, the author name C. Saron is incorrect and should be listed as C. Sardu. Therefore the correct author list is: R. Marfella, F. Cacciapuoti, M. Siniscalchi, F. C. Sasso, F. Marchese, F. Cinone, E. Musacchio, M. A. Marfella, L. Ruggiero, G. Chiorazzo, D. Liberti, G. Chiorazzo, G. F. Nicoletti, C. Sardu, F. D'Andrea, C. Ammendola, M. Verza and L. Coppola
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