3,200 research outputs found

    Dependence of nucleotide physical properties on their placement in codons and determinative degree

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    Various physical properties such as dipole moment, heat of formation and energy of the most stable formation of nucleotides and bases were calculated by PM3 (modified neglect of diatomic overlap, parametric method number 3) and AM1 (Austin model 1) methods. As distinct from previous calculations, for nucleotides the interaction with neighbours is taken into account up to gradient of convergence equaling 1. The dependences of these variables from the place in the codon and the determinative degree were obtained. The difference of these variables for codons and anticodons is shown.Comment: 13 pages, 8 figures, PD

    Exlusive charmed meson pair production

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    The experimental data of BELLE Collaboration on the exclusive charmed meson pair production in the process of monophotonic e+e−e^+e^--annihilation (e+e−→γ∗→DDˉe^+e^-\to \gamma^* \to D\bar D) has been studied. It has been shown that these data is described satisfactorily in the frame work of constituent quark model. Our studies have demonstrated that the central production process e+e−→e+e−γγ→e+e−DDˉ+Xe^+e^-\to e^+e^-\gamma\gamma \to e^+e^-D\bar D +X and the process of monophotonic e+e−e^+e^--annihilation yield comparable numbers of the charmed meson pairs.Comment: 15 pages, 7 figures, RevTeX

    The Color-Octet Contributions to PP-wave BcB_c Meson Hadroproduction

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    The contributions from the color-octet components ∣(cbˉ)8(1S0)g>|(c\bar b)_{\bf 8}(^{1}S_{0}) g> and ∣(cbˉ)8(3S1)g>|(c\bar b)_{\bf 8}(^{3}S_{1}) g> to the hBch_{B_c} or χBcJ\chi_{B_c}^J (the PP-wave BcB_c meson) hadroproduction are estimated in terms of the complete O(αs4){\cal O}(\alpha_s^4) calculation. As necessary inputs in the estimate, we take the values of the octet matrix elements according to the NRQCD scaling rules, and as a result, we have found that the contributions to the PP-wave production may be the same in order of magnitude as those from the color-singlet ones, ∣(cbˉ)1(1P1)>|(c\bar b)_{\bf 1}(^{1}P_{1})> and ∣(cbˉ)1(3PJ)>|(c\bar b)_{\bf 1}(^{3}P_{J})> (J=1,2,3J=1,2,3). Especially, our result indicates that the observation of the color-octet contributions to the PP-wave production in the low transverse momentum region is not very far from the present experimental capability at Tevatron and LHC.Comment: 14 pages, 4 figures (8 eps-files for figures), add references and correct typo
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