143,465 research outputs found

    Farming with Soybeans For Marketing For Feeding For Land Use

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    The Soybean: Its Place in a Farming System

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    Power Spectrum of Cosmic Momentum Field Measured from the SFI Galaxy Sample

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    We have measured the cosmic momentum power spectrum from the peculiar velocities of galaxies in the SFI sample. The SFI catalog contains field spiral galaxies with radial peculiar velocities derived from the I-band Tully-Fisher relation. As a natural measure of the large-scale peculiar velocity field, we use the cosmic momentum field that is defined as the peculiar velocity field weighted by local number of galaxies. We have shown that the momentum power spectrum can be derived from the density power spectrum for the constant linear biasing of galaxy formation, which makes it possible to estimate \beta_S = \Omega_m^{0.6} / b_S parameter precisely where \Omega_m is the matter density parameter and b_S is the bias factor for optical spiral galaxies. At each wavenumber k we estimate \beta_S(k) as the ratio of the measured to the derived momentum power over a wide range of scales (0.026 h^{-1}Mpc <~ k <~ 0.157 h^{-1}Mpc) that spans the linear to the quasi-linear regimes. The estimated \beta_S(k)'s have stable values around 0.5, which demonstrates the constancy of \beta_S parameter at scales down to 40 h^{-1}Mpc. We have obtained \beta_S=0.49_{-0.05}^{+0.08} or \Omega_m = 0.30_{-0.05}^{+0.09} b_S^{5/3}, and the amplitude of mass fluctuation as \sigma_8\Omega_m^{0.6}=0.56_{-0.21}^{+0.27}. The 68% confidence limits include the cosmic variance. We have also estimated the mass density power spectrum. For example, at k=0.1047 h Mpc^{-1} (\lambda=60 h^{-1}Mpc) we measure \Omega_m^{1.2} P_{\delta}(k)=(2.51_{-0.94}^{+0.91})\times 10^3 (h^{-1}Mpc)^3, which is lower compared to the high-amplitude power spectra found from the previous maximum likelihood analyses of peculiar velocity samples like Mark III, SFI, and ENEAR.Comment: 12 pages, 9 figures, accepted for publication in Ap

    Isospin-violating dark matter from a double portal

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    We study a simple model that can give rise to isospin-violating interactions of Dirac fermion asymmetric dark matter to protons and neutrons through the interference of a scalar and U(1)' gauge boson contribution. The model can yield a large suppression of the elastic scattering cross section off Xenon relative to Silicon thus reconciling CDMS-Si and LUX results while being compatible with LHC findings on the 126 GeV Higgs, electroweak precision tests and flavour constraints.Comment: 25 pages, 7 figure

    A mindful approach to eating disorders

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    The strongest experimental constraints on SU(5)xU(1) supergravity models

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    We consider a class of well motivated string-inspired flipped SU(5)SU(5) supergravity models which include four supersymmetry breaking scenarios: no-scale, strict no-scale, dilaton, and special dilaton, such that only three parameters are needed to describe all new phenomena (mt,tanβ,mg~)(m_t,\tan\beta,m_{\tilde g}). We show that the LEP precise measurements of the electroweak parameters in the form of the ϵ1\epsilon_1 variable, and the CLEOII allowed range for \bsg are at present the most important experimental constraints on this class of models. For m_t\gsim155\,(165)\GeV, the ϵ1\epsilon_1 constraint (at 90(95)\%CL) requires the presence of light charginos (m_{\chi^\pm_1}\lsim50-100\GeV depending on mtm_t). Since all sparticle masses are proportional to mg~m_{\tilde g}, m_{\chi^\pm_1}\lsim100\GeV implies: m_{\chi^0_1}\lsim55\GeV, m_{\chi^0_2}\lsim100\GeV, m_{\tilde g}\lsim360\GeV, m_{\tilde q}\lsim350\,(365)\GeV, m_{\tilde e_R}\lsim80\,(125)\GeV, m_{\tilde e_L}\lsim120\,(155)\GeV, and m_{\tilde\nu}\lsim100\,(140)\GeV in the no-scale (dilaton) flipped SU(5)SU(5) supergravity model. The \bsg constraint excludes a significant fraction of the otherwise allowed region in the (mχ1±,tanβ)(m_{\chi^\pm_1},\tan\beta) plane (irrespective of the magnitude of the chargino mass), while future experimental improvements will result in decisive tests of these models. In light of the ϵ1\epsilon_1 constraint, we conclude that the outlook for chargino and selectron detection at LEPII and at HERA is quite favorable in this class of models.Comment: CTP-TAMU-40/93, Latex, 13 pages, 10 figures (available as uuencoded 0.963MB file from [email protected]
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