355 research outputs found

    Spheroidal and elliptical galaxy radial velocity dispersion determined from Cosmological General Relativity

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    Radial velocity dispersion in spheroidal and elliptical galaxies, as a function of radial distance from the center of the galaxy, has been derived from Cosmological Special Relativity. For velocity dispersions in the outer regions of spherical galaxies, the dynamical mass calculated for a galaxy using Carmelian theory may be 10 to 100 times less than that calculated from standard Newtonian physics. This means there is no need to include halo dark matter. The velocity dispersion is found to be approximately constant across the galaxy after falling from an initial high value at the center.Comment: 10 pages, 3 figure

    Modeling of Rotational Nonequilibrium in Post-Normal Shock Flow Analyses

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    Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/106447/1/AIAA2013-191.pd

    Ultraviolet Complete Electroweak Model Without a Higgs Particle

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    An electroweak model with running coupling constants described by an energy dependent entire function is utraviolet complete and avoids unitarity violations for energies above 1 TeV. The action contains no physical scalar fields and no Higgs particle and the physical electroweak model fields are local and satisfy microcausality. The WW and ZZ masses are compatible with a symmetry breaking SU(2)L×U(1)YU(1)emSU(2)_L\times U(1)_Y \rightarrow U(1)_{\rm em}, which retains a massless photon. The vertex couplings possess an energy scale ΛW>1\Lambda_W > 1 TeV predicting scattering amplitudes that can be tested at the LHC.Comment: 19 pages, no figures, LaTex file. Equation and text corrected. Reference added. Results remain the same. Final version published in European Physics Journal Plus, 126 (2011

    Optimized Variables of the Study of Λb\Lambda_b Polarization

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    The value of the bb-baryon polarization can be extracted from inclusive data at LEP with better than 10\% precision based on current statistics. We present a new variable by which to measure the polarization, which is the ratio of the average electron energy to the average neutrino energy. This variable is both sensitive to polarization and insensitive to fragmentation uncertainties.Comment: 10 pages (LaTeX), 2 figures, MIT-CTP-2270, CERN-PPE/94-0

    Analysis of the vertexes ΞQΞQV\Xi_Q^*\Xi'_Q V, ΣQΣQV\Sigma_Q^*\Sigma_Q V and radiative decays ΞQΞQγ\Xi_Q^*\to \Xi'_Q \gamma, ΣQΣQγ\Sigma_Q^*\to \Sigma_Q \gamma

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    In this article, we study the vertexes ΞQΞQV\Xi_Q^*\Xi'_Q V and ΣQΣQV\Sigma_Q^* \Sigma_Q V with the light-cone QCD sum rules, then assume the vector meson dominance of the intermediate ϕ(1020)\phi(1020), ρ(770)\rho(770) and ω(782)\omega(782), and calculate the radiative decays ΞQΞQγ\Xi_Q^*\to \Xi'_Q \gamma and ΣQΣQγ\Sigma_Q^*\to \Sigma_Q \gamma.Comment: 28 pages, 4 tables, revised versio

    Initial-State Interactions in the Unpolarized Drell-Yan Process

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    We show that initial-state interactions contribute to the cos2ϕ\cos 2 \phi distribution in unpolarized Drell-Yan lepton pair production ppp p and ppˉ+X p \bar p \to \ell^+ \ell^- X, without suppression. The asymmetry is expressed as a product of chiral-odd distributions h1(x1,p2)×hˉ1(x2,k2)h_1^\perp(x_1,\bm{p}_\perp^2)\times \bar h_1^\perp(x_2,\bm{k}_\perp^2) , where the quark-transversity function h1(x,p2)h_1^\perp(x,\bm{p}_\perp^2) is the transverse momentum dependent, light-cone momentum distribution of transversely polarized quarks in an {\it unpolarized} proton. We compute this (naive) TT-odd and chiral-odd distribution function and the resulting cos2ϕ\cos 2 \phi asymmetry explicitly in a quark-scalar diquark model for the proton with initial-state gluon interaction. In this model the function h1(x,p2)h_1^\perp(x,\bm{p}_\perp^2) equals the TT-odd (chiral-even) Sivers effect function f1T(x,p2)f^\perp_{1T}(x,\bm{p}_\perp^2). This suggests that the single-spin asymmetries in the SIDIS and the Drell-Yan process are closely related to the cos2ϕ\cos 2 \phi asymmetry of the unpolarized Drell-Yan process, since all can arise from the same underlying mechanism. This provides new insight regarding the role of quark and gluon orbital angular momentum as well as that of initial- and final-state gluon exchange interactions in hard QCD processes.Comment: 22 pages, 6 figure

    When Will Adolescents Tell Someone About Dating Violence Victimization?

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    This study examined factors that influence help-seeking among a diverse sample of adolescents who experienced dating violence. A sample of 57 high school students in an urban community reported on the prevalence and characteristics of dating violence in their relationships. Someone observing a dating violence incident and a survivor’s attaching an emotional meaning to the event significantly influenced adolescents to talk to someone. When dating violence occurred in isolation, survivors were more likely to receive no support from others in the aftermath of the incident. Differences between boys’ and girls’ help-seeking and implications for dating violence intervention and prevention programming are discussed.Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/90887/1/Black-Tolman-Callahan-Saunders- Weisz- 2008-When will adolescents tell someone about dating violence VAW.pd

    Dilepton Spectra from Decays of Light Unflavored Mesons

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    The invariant mass spectrum of the e+ee^{+}e^{-} and μ+μ\mu ^{+}\mu ^{-} pairs from decays of light unflavored mesons with masses below the ϕ(1020)\phi (1020)-meson mass to final states containing along with a dilepton pair one photon, one meson, and two mesons are calculated within the framework of the effective meson theory. The results can be used for simulations of the dilepton spectra in heavy-ion collisions and for experimental searches of dilepton meson decays.Comment: 73 pages, 19 figures, 3 tables, REVTeX, new references adde

    Deep Inelastic Scattering from off-Shell Nucleons

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    We derive the general structure of the hadronic tensor required to describe deep-inelastic scattering from an off-shell nucleon within a covariant formalism. Of the large number of possible off-shell structure functions we find that only three contribute in the Bjorken limit. In our approach the usual ambiguities encountered when discussing problems related to off-shellness in deep-inelastic scattering are not present. The formulation therefore provides a clear framework within which one can discuss the various approximations and assumptions which have been used in earlier work. As examples, we investigate scattering from the deuteron, nuclear matter and dressed nucleons. The results of the full calculation are compared with those where various aspects of the off-shell structure are neglected, as well as with those of the convolution model.Comment: 36 pages RevTeX, 9 figures (available upon request), ADP-93-210/T128, PSI-PR-93-13, accepted for publication in Physical Review

    Quark Imaging in the Proton Via Quantum Phase-Space Distributions

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    We develop the concept of quantum phase-space (Wigner) distributions for quarks and gluons in the proton. To appreciate their physical content, we analyze the contraints from special relativity on the interpretation of elastic form factors, and examine the physics of the Feynman parton distributions in the proton's rest frame. We relate the quark Wigner functions to the transverse-momentum dependent parton distributions and generalized parton distributions, emphasizing the physical role of the skewness parameter. We show that the Wigner functions allow to visualize quantum quarks and gluons using the language of the classical phase space. We present two examples of the quark Wigner distributions and point out some model-independent features.Comment: 20 pages with 3 fiture
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