46 research outputs found

    Renormalization Group Summation and the Free Energy of Hot QCD

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    Using an approach developed in the context of zero-temperature QCD to systematically sum higher order effects whose form is fixed by the renormalization group equation, we sum to all orders the leading log (LL) and next-to-leading log (NLL) contributions to the thermodynamic free energy in hot QCD. While the result varies considerably less with changes in the renormalization scale than does the purely perturbative result, a novel ambiguity arises which reflects the strong scheme dependence of thermal perturbation theory.Comment: 7 pages REVTEX4, 2 figures; v2: typos correcte

    Large effects on \BsBs mixing by vector-like quarks

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    We calculate the contributions of the vector-like quark model to \BsBs mixing, taking into account the constraints from the decay BXsγB\to X_s\gamma. In this model the neutral bosons mediate flavor-changing interactions at the tree level. However, \BsBs mixing is dominated by contributions from the box diagrams with the top quark and the extra up-type quark. In sizable ranges of the model parameters, the mixing parameter xsx_s is much different from the standard model prediction.Comment: 11 pages, 4 figures, To be published in Phys. Rev.

    Mass Suppression in Octet Baryon Production

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    There is a striking suppression of the cross section for production of octet baryons in e+ee^+ e ^- annihilation, as the mass of the produced hadron increases. We present a simple parametrization for the fragmentation functions into octet baryons guided by two input models: the SU(3) flavor symmetry part is given by a quark-diquark model, and the baryon mass suppression part is inspired by the string model. We need only eight free parameters to describe the fragmentation functions for all octet baryons. These free parameters are determined by a fit to the experimental data of octet baryon production in e+ee^+ e ^- annihilation. Then we apply the obtained fragmentation functions to predict the cross section of the octet baryon production in charged lepton DIS and find consistency with the available experimental data. Furthermore, baryon production in pppp collisions is suggested to be an ideal domain to check the predicted mass suppression.Comment: 20 pages, 5 figure

    Possible Effects of Noncommutative Geometry on Weak CP Violation and Unitarity Triangles

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    Possible effects of noncommutative geometry on weak CP violation and unitarity triangles are discussed by taking account of a simple version of the momentum-dependent quark mixing matrix in the noncommutative standard model. In particular, we calculate nine rephasing invariants of CP violation and illustrate the noncommutative CP-violating effect in a couple of charged D-meson decays. We also show how inner angles of the deformed unitarity triangles are related to CP-violating asymmetries in some typical B_d and B_s transitions into CP eigenstates. B-meson factories are expected to help probe or constrain noncommutative geometry at low energies in the near future.Comment: RexTev 16 pages. Modifications made. References added. Accepted for publication in Phys. Rev.

    Semi-inclusive B Decays and Direct CP Violation in QCD Factorization

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    We have systematically investigated the semi-inclusive B decays B->MX, which are manifestations of the quark decay b->Mq, within the framework of QCD-improved factorization. These decays are theoretically clean and have distinctive experimental signatures. We focus on a class of these that do not require any form factor information and therefore may be especially suitable for extracting information on the angles α\alpha and γ\gamma of the unitarity triangle. The nonfactorizable effects, such as vertex-type and penguin-type corrections to the two-body b decay and hard spectator corrections to the 3-body decay are calculable in the heavy quark limit. QCD factorization is applicable when the emitted meson is a light meson or a charmonium. We discuss the issue of the CPT constraint on partial rate asymmetries. The strong phase coming from final-state rescattering due to hard gluon exchange between the final states can induce large rate asymmetries for tree-dominated color-suppressed modes (π0,ρ0,ω)Xsˉ(\pi^0,\rho^0,\omega)X_{\bar s}. The nonfactorizable hard spectator interactions in the 3-body decay, though phase-space suppressed, are extremely important for the tree-dominated modes (π0,ρ0,ω)Xsˉ,ϕX(\pi^0,\rho^0,\omega)X_{\bar s}, \phi X, JXs,JXJ X_s,J X and the penguin-dominated mode ωXssˉ\omega X_{s\bar s}. In fact, they are dominated by the hard spectator corrections. Our result for B(BJ/ψXs){\cal B} (B\to J/\psi X_s) is in agreement with experiment. The semi-inclusive decay modes: Bs0(π0,ρ0,ω)XsˉB^0_s\to (\pi^0,\rho^0,\omega)X_{\bar s}, ρ0Xssˉ\rho^0X_{s\bar s}, B0(KX,KX)B^0\to(K^-X,K^{*-}X) and B(K0Xs,K0Xs)B^-\to (K^0X_s,K^{*0}X_s) are the most promising ones in searching for direct CP violation. In fact, they have branching ratios of order 10610410^{-6}-10^{-4} and CP rate asymmetries of order (1040)(10-40)%.Comment: 28 page

    Nuclear transparency from quasielastic A(e,e'p) reactions uo to Q^2=8.1 (GeV/c)^2

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    The quasielastic (e,e^\primep) reaction was studied on targets of deuterium, carbon, and iron up to a value of momentum transfer Q2Q^2 of 8.1 (GeV/c)2^2. A nuclear transparency was determined by comparing the data to calculations in the Plane-Wave Impulse Approximation. The dependence of the nuclear transparency on Q2Q^2 and the mass number AA was investigated in a search for the onset of the Color Transparency phenomenon. We find no evidence for the onset of Color Transparency within our range of Q2Q^2. A fit to the world's nuclear transparency data reflects the energy dependence of the free proton-nucleon cross section.Comment: 11 pages, 6 figure

    Short Distance vs. Long Distance Physics: The Classical Limit of the Minimal Length Uncertainty Relation

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    We continue our investigation of the phenomenological implications of the "deformed" commutation relations [x_i,p_j]=i hbar[(1 + beta p^2) delta_{ij} + beta' p_i p_j]. These commutation relations are motivated by the fact that they lead to the minimal length uncertainty relation which appears in perturbative string theory. In this paper, we consider the effects of the deformation on the classical orbits of particles in a central force potential. Comparison with observation places severe constraints on the value of the minimum length.Comment: 20 pages REVTEX4, 4 color eps figures, typos correcte

    The cause and control of cavity spot in carrots

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