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15661por Rosner, Jonathan L“…The enhancement \Delta \Gamma (\Lambda_b) of the \Lambda_b decay rate due to four-fermion processes of weak scattering and Pauli interference is calculated within the quark model. An estimate of the relative bu wave function at zero separation, |\Psi(0)|^2_{bu}, is obtained in terms of the \Sigma_b^* - \Sigma_b hyperfine splitting, the B^* - B hyperfine splitting, and the B meson decay constant f_B. …”
Publicado 1996
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15662“…Meson--photon--photon transition form factors for S-, P-, and D-wave states are calculated, the meson being treated as a non-relativistic heavy-quark--antiquark pair. The full dependence on both photon virtualities is included. …”
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15663por Esposito, Giampiero“…In the second part, a number of relevant physical applications are studied: non-local boundary conditions for massless spin-1/2 fields, massless spin-3/2 potentials on manifolds with boundary, geometric theory of massive spin-3/2 potentials, local boundary conditions in quantum supergravity, quark boundary conditions, one-loop quantum cosmology, conformally covariant operators and Euclidean quantum gravity.…”
Publicado 1998
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15664“…We also study causal time-delay of low-energy excitation on heavy quark or meson and find an excellent agreement between anti-de Sitter supergravity and super Yang-Mills theory descriptions. …”
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15665“…When one of the $b$ hadrons in the event undergoes semileptonic decay, the charge of its parent $b$ quark at decay time is reflected by that of the lepton, its flight length is reconstructed by a topological vertexing technique, and the $b$ hadron momentum is measured using an energy flow method. …”
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15666por Quast, G“…Together with measurements of the top quark and W boson masses at the Tevatron pp collider at Fermilab these results provide tests of the Standard Model of the electroweak interaction with unprecedented precision and permit to place stringent limits on the mass of the Higgs boson, the last free parameter of the model. (68 refs).…”
Publicado 1999
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15667por Le Goff, J M“…Semi-inclusive data were analyzed in order to produce the first polarized quark distributions. Data obtained with a dedicated low $x$ trigger extend down to $x=6 \times 10^{-5}$ for $Q^{2} \geq$ 0.01 GeV$^{2}$. …”
Publicado 2000
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15668por Aleppo, M“…The contributions from charm quark fragmentation and from b hadron decays are disentangled. …”
Publicado 2000
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15669por Antinori, Federico“…QCD predicts that under such conditions a phase transition from a system composed of colourless hadrons to a Quark-Gluon Plasma (QGP) should occur. A rich ultrarelativistic heavy-ion physics programme is under way both at BNL-AGS and at CERN-SPS since 1986. …”
Publicado 2001
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15670por Baines, J T M“…About one collision in every hundred will produce a bb quark pair. Therefore, in addition to rejecting background from non-bb events, the trigger must have the ability to identify and select those events containing the B-decay channels of specific interest. …”
Publicado 2001
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15671“…Direct photons have been proposed as a promising signature for the quark-gluon plasma (QGP) formation in relativistic heavy-ion collisions. …”
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15672por Antinori, Federico“…QCD predicts that under such conditions a phase transition from a system composed of colourless hadrons to a Quark-Gluon Plasma (QGP) should occur. A rich ultrarelativistic heavy-ion physics programme is under way both at BNL-AGS and at CERN-SPS since 1986. …”
Publicado 2002
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15673por Takai, H“…Recent results from RHIC experiments suggest that a hot QCD matter, known as quark gluon plasma (QGP), may be formed in Gold+Gold collisions at a center mass energy of 200 GeV per colliding pair. …”
Publicado 2003
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15674“…This problem can be to large extent overcome if both top-quark decays are reconstructed in addition to the reconstruction of the H-->bb mass peak. …”
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15675“…Within this model, the lower squark-gluino mass limit allowing the detection of the h is about 450 GeV, and observation should be pssible already with a few*10^3 pb-1, and extends up to quark - gluino masses of approx. 1.5 TeV with 10^5 pb-1. …”
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15676“…We discuss a number of applications of our model which include the calculation of the deuteron structure functions, nuclear valence and sea quark distributions and nuclear structure functions for neutrino charged-current scattering.…”
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15677“…Structure functions for nu N and nu N interactions were obtained from the three-quark-boson nucleon model constructed before from the study of deep inelastic eN scattering (see abstr. …”
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15678“…Some justification is given for the quark counting rule for total cross sections. Implications for the Regge-Gribov calculus in processes involving baryons are discussed. (30 refs).…”
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15679por Sandhoff, Marisa“…This cross section ratio is needed to improve the W+jets normalization for top quark analyses and to test Monte Carlo generator and QCD predictions. …”
Publicado 2015
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15680por Zherebchevsky, V I, Igolkin, S N, Krymov, E B, Maltsev, N A, Makarov, N A, Feofilov, G A“…The extra lightweight mechanical support structures, together with the novel pixel detectors, provide a record-breaking total radiation length of 0.3% X 0 per layer, which will make it possible to considerably extend the physical program of investigations of the quark-gluon plasma in ultra-relativistic heavy-ion collisions at the Large Hadron Collider. …”
Publicado 2014
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