328 research outputs found

    Structure and dynamics of the HIV-2 TAR RNA-argininamide complex by NMR spectroscopy

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    Thesis (Ph. D.)--Massachusetts Institute of Technology, Dept. of Chemistry, 1998.Includes bibliographical references (leaves 248-269).by Alexander S. Brodsky.Ph.D

    NNLO corrections to top-pair production at hadron colliders: the all-fermionic scattering channels

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    This is a second paper in our ongoing calculation of the next-to-next-to-leading order (NNLO) QCD correction to the total inclusive top-pair production cross-section at hadron colliders. In this paper we calculate the reaction qqˉttˉ+qqˉq\bar q \to t\bar t + q\bar q which was not considered in our previous work on qqˉttˉ+Xq\bar q \to t\bar t +X due to its phenomenologically negligible size. We also calculate all remaining fermion-pair-initiated partonic channels qq,qqˉqq', q\bar q' and qqqq that contribute to top-pair production starting from NNLO. The contributions of these reactions to the total cross-section for top-pair production at the Tevatron and LHC are small, at the permil level. The most interesting feature of these reactions is their characteristic logarithmic rise in the high energy limit. We compute the constant term in the leading power behavior in this limit, and achieve precision that is an order of magnitude better than the precision of a recent theoretical prediction for this constant. All four partonic reactions computed in this paper are included in our numerical program Top++. The calculation of the NNLO corrections to the two remaining partonic reactions, qgttˉ+Xqg\to t\bar t+X and ggttˉ+Xgg\to t\bar t+X, is ongoing.Comment: 1+16 pages; 3 figure

    Cisplatin resistant spheroids model clinically relevant survival mechanisms in ovarian tumors

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    © The Author(s), 2016. This article is distributed under the terms of the Creative Commons Attribution License. The definitive version was published in PLoS 11 (2016): e0151089, doi: 10.1371/journal.pone.0151089 .The majority of ovarian tumors eventually recur in a drug resistant form. Using cisplatin sensitive and resistant cell lines assembled into 3D spheroids we profiled gene expression and identified candidate mechanisms and biological pathways associated with cisplatin resistance. OVCAR-8 human ovarian carcinoma cells were exposed to sub-lethal concentrations of cisplatin to create a matched cisplatin-resistant cell line, OVCAR-8R. Genome-wide gene expression profiling of sensitive and resistant ovarian cancer spheroids identified 3,331 significantly differentially expressed probesets coding for 3,139 distinct protein-coding genes (Fc >2, FDR < 0.05) (S2 Table). Despite significant expression changes in some transporters including MDR1, cisplatin resistance was not associated with differences in intracellular cisplatin concentration. Cisplatin resistant cells were significantly enriched for a mesenchymal gene expression signature. OVCAR-8R resistance derived gene sets were significantly more biased to patients with shorter survival. From the most differentially expressed genes, we derived a 17-gene expression signature that identifies ovarian cancer patients with shorter overall survival in three independent datasets. We propose that the use of cisplatin resistant cell lines in 3D spheroid models is a viable approach to gain insight into resistance mechanisms relevant to ovarian tumors in patients. Our data support the emerging concept that ovarian cancers can acquire drug resistance through an epithelial-to-mesenchymal transition.This work was funded by the NIH NCRR supplement grant P41 RR001395-27S1 (J.W.H.), NSF DBI-1005378 “REU Site: Biological Discovery in Woods Hole”, faculty startup funds from the Office of Research at Oklahoma State University (W.C.), and the Mary Kay Foundation (A.S.B.)

    Exon expression profiling reveals stimulus-mediated exon use in neural cells

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    Exon centric microarrays were used to resolve the calcium-modulated gene expression response into transcript-level an exon-level regulation

    Four-fermion interaction from torsion as dark energy

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    The observed small, positive cosmological constant may originate from a four-fermion interaction generated by the spin-torsion coupling in the Einstein-Cartan-Sciama-Kibble gravity if the fermions are condensing. In particular, such a condensation occurs for quark fields during the quark-gluon/hadron phase transition in the early Universe. We study how the torsion-induced four-fermion interaction is affected by adding two terms to the Dirac Lagrangian density: the parity-violating pseudoscalar density dual to the curvature tensor and a spinor-bilinear scalar density which measures the nonminimal coupling of fermions to torsion.Comment: 6 pages; published versio

    Dilepton production in proton-proton collisions at BEVALAC energies

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    The dilepton production in elementary ppe+eX{pp\to e^{+}e^{-}X} reactions at BEVALAC energies Tlab=1÷5T_{lab}=1\div 5 GeV is investigated. The calculations include direct e+e{e^{+}e^{-}} decays of the vector mesons ρ0\rho ^{0}, ω\omega , and ϕ\phi , Dalitz decays of the π0\pi ^{0}-, η\eta -, % \rho -, ω\omega -, and ϕ\phi -mesons, and of the baryon resonances % \Delta (1232),N(1520), ...... . The subthreshold vector meson production cross sections in pppp collisions are treated in a way sufficient to avoid double counting with the inclusive vector meson production. The vector meson dominance model for the transition form factors of the resonance Dalitz decays Re+eNR\to e^{+}e^{-}N is used in an extended form to ensure correct asymptotics which are in agreement with the quark counting rules. Such a modification gives an unified and consistent description of both RNγR\to N\gamma radiative decays and RNρ(ω)R\to N\rho (\omega) meson decays. The effect of multiple pion production on the experimental efficiency for the detection of the dilepton pairs is studied. We find the dilepton yield in reasonable agreement with the experimental data for the set of intermediate energies whereas at the highest energy Tlab=4.88T_{lab}=4.88 GeV the number of dilepton pairs is likely to be overestimated experimentally in the mass range M=300÷700M=300\div 700 MeV.Comment: 25 pages (IOP style), 5 figures, revised manuscript accepted for publication in JP
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