200 research outputs found

    Common names of weeds in Missouri field crops

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    "Common weeds in field crops are known by at least two common names; some by a dozen or more. For example, Abutilon theophrasti may be referred to as wild cotton in southeast Missouri, while farmers in a northwest community may call it butter print. Indian mallow might be the preferred name in another locale. But if you want to use the name that will get the most nods of recognition from farmers throughout this country, call it velvetleaf. The many common names of weeds frequently creates communication problems. During a conversation, two people may refer to a plant species, but use different common names. They don't realize that they are both referring to the same plant. More importantly, this confusion can result in erroneous weed management decisions."--First page.William W. Dierker and Mitchell E. Roof (Integrated Pest Management College of Agriculture)New 8/82/8

    Weed competition in soybeans and corn

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    "6/82/1M""The effects of weed competition on crop yields demonstrate the importance of weed control practices. This review of weed competition focuses on crops that are economically important to Missouri."--first paragraphUniversity of Missouri Extension DivisionIncludes bibliographical reference

    Domain Growth, Wetting and Scaling in Porous Media

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    The lattice Boltzmann (LB) method is used to study the kinetics of domain growth of a binary fluid in a number of geometries modeling porous media. Unlike the traditional methods which solve the Cahn-Hilliard equation, the LB method correctly simulates fluid properties, phase segregation, interface dynamics and wetting. Our results, based on lattice sizes of up to 4096×40964096\times 4096, do not show evidence to indicate the breakdown of late stage dynamical scaling, and suggest that confinement of the fluid is the key to the slow kinetics observed. Randomness of the pore structure appears unnecessary.Comment: 13 pages, latex, submitted to PR

    Effects of pressure on spin fluctuations and the exchange interaction in La2CuO4 as determined by two‐magnon Raman scattering (abstract)

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    We have measured the two‐magnon Raman scattering spectrum of magnetic La2CuO4 at pressures of up to 100 kbar. Analysis of the moments of the two‐magnon line shape indicates that the renormalization parameters resulting from spin fluctuations are essentially pressure independent in this pressure range. Our results provide the first direct determination of the pressure dependence of the in‐plane exchange coupling constant J. The pressure dependence of J is compared with that of the Néel temperature and discussed in the context of recent theories for quasi‐two‐dimensional magnetic systems.Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/71024/2/JAPIAU-69-8-5392-1.pd

    Rigid Chiral Membranes

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    Statistical ensembles of flexible two-dimensional fluid membranes arise naturally in the description of many physical systems. Typically one encounters such systems in a regime of low tension but high stiffness against bending, which is just the opposite of the regime described by the Polyakov string. We study a class of couplings between membrane shape and in-plane order which break 3-space parity invariance. Remarkably there is only {\it one} such allowed coupling (up to boundary terms); this term will be present for any lipid bilayer composed of tilted chiral molecules. We calculate the renormalization-group behavior of this relevant coupling in a simplified model and show how thermal fluctuations effectively reduce it in the infrared.Comment: 11 pages, UPR-518T (This replaced version has fonts not used removed.

    Observation of the Smectic C -- Smectic I Critical Point

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    We report the first observation of the smectic C--smectic I (C--I) critical point by Xray diffraction studies on a binary system. This is in confirmity with the theoretical idea of Nelson and Halperin that coupling to the molecular tilt should induce hexatic order even in the C phase and as such both C and I (a tilted hexatic phase) should have the same symmetry. The results provide evidence in support of the recent theory of Defontaines and Prost proposing a new universality class for critical points in layered systems.Comment: 9 pages Latex and 5 postscript figures available from [email protected] on request, Phys.Rev.Lett. (in press

    On the origin of the A1g_{1g} and B1g_{1g} electronic Raman scattering peaks in the superconducting state of YBa2_{2}Cu3_{3}O7δ_{7-\delta}

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    The electronic Raman scattering has been investigated in optimally oxygen doped YBa2_{2}Cu3_{3}O7δ_{7-\delta} single crystals as well as in crystals with non-magnetic, Zn, and magnetic, Ni, impurities. We found that the intensity of the A1g_{1g} peak is impurity independent and their energy to TcT_{c} ratio is almost constant (2Δ/kBTc52\Delta/k_{B}T_{c}\sim5). Moreover, the signal at the B1g_{1g} channel is completely smeared out when non-magnetic Zn impurities are present. These results are qualitatively interpreted in terms of the Zeyher and Greco's theory that relates the electronic Raman scattering in the A1g_{1g} and B1g_{1g} channels to \textit{d}-CDW and superconducting order parameters fluctuations, respectively.Comment: Submited to Phys. Rev. Let

    A study of the superconducting gap in RNi2_2B2_2C (R = Y, Lu) single crystals by inelastic light scattering

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    Superconductivity-induced changes in the electronic Raman scattering response were observed for the RNi2_2B2_2C (R = Y, Lu) system in different scattering geometries. In the superconducting state, 2Δ\Delta-like peaks were observed in A1g_{1g}, B1g_{1g}, and B2g_{2g} spectra from single crystals. The peaks in A1g_{1g} and B2g_{2g} symmetries are significantly sharper and stronger than the peak in B1g_{1g} symmetry. The temperature dependence of the frequencies of the 2Δ\Delta-like peaks shows typical BCS-type behavior, but the apparent values of the 2Δ2\Delta gap are strongly anisotropic for both systems. In addition, for both YNi2_2B2_2C and LuNi2_2B2_2C systems, there exists reproducible scattering strength below the 2Δ2\Delta gap which is roughly linear to the frequency in B1g_{1g} and B2g_{2g} symmetries. This discovery of scattering below the gap in non-magnetic borocarbide superconductors, which are thought to be conventional BCS-type superconductors, is a challenge for current understanding of superconductivity in this system.Comment: Added text, changed a figure, and added references. Will appear in Phys. Rev.

    Evolution of speckle during spinodal decomposition

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    Time-dependent properties of the speckled intensity patterns created by scattering coherent radiation from materials undergoing spinodal decomposition are investigated by numerical integration of the Cahn-Hilliard-Cook equation. For binary systems which obey a local conservation law, the characteristic domain size is known to grow in time τ\tau as R=[Bτ]nR = [B \tau]^n with n=1/3, where B is a constant. The intensities of individual speckles are found to be nonstationary, persistent time series. The two-time intensity covariance at wave vector k{\bf k} can be collapsed onto a scaling function Cov(δt,tˉ)Cov(\delta t,\bar{t}), where δt=k1/nBτ2τ1\delta t = k^{1/n} B |\tau_2-\tau_1| and tˉ=k1/nB(τ1+τ2)/2\bar{t} = k^{1/n} B (\tau_1+\tau_2)/2. Both analytically and numerically, the covariance is found to depend on δt\delta t only through δt/tˉ\delta t/\bar{t} in the small-tˉ\bar{t} limit and δt/tˉ1n\delta t/\bar{t} ^{1-n} in the large-tˉ\bar{t} limit, consistent with a simple theory of moving interfaces that applies to any universality class described by a scalar order parameter. The speckle-intensity covariance is numerically demonstrated to be equal to the square of the two-time structure factor of the scattering material, for which an analytic scaling function is obtained for large tˉ.\bar{t}. In addition, the two-time, two-point order-parameter correlation function is found to scale as C(r/(Bnτ12n+τ22n),τ1/τ2)C(r/(B^n\sqrt{\tau_1^{2n}+\tau_2^{2n}}),\tau_1/\tau_2), even for quite large distances rr. The asymptotic power-law exponent for the autocorrelation function is found to be λ4.47\lambda \approx 4.47, violating an upper bound conjectured by Fisher and Huse.Comment: RevTex: 11 pages + 12 figures, submitted to PR
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