11,428 research outputs found

    Pseuduscalar Heavy Quarkonium Decays With Both Relativistic and QCD Radiative Corrections

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    We estimate the decay rates of ηc2γ\eta_c\rightarrow 2\gamma, ηc2γ\eta_c'\rightarrow 2\gamma, and J/ψe+eJ/\psi\rightarrow e^+ e^-, ψe+e\psi^\prime\rightarrow e^+e^-, by taking into account both relativistic and QCD radiative corrections. The decay amplitudes are derived in the Bethe-Salpeter formalism. The Bethe-Salpeter equation with a QCD-inspired interquark potential are used to calculate the wave functions and decay widths for these ccˉc\bar{c} states. We find that the relativistic correction to the ratio RΓ(ηc2γ)/Γ(J/ψe+e)R\equiv \Gamma (\eta_c \rightarrow 2\gamma)/ \Gamma (J/ \psi \rightarrow e^+ e^-) is negative and tends to compensate the positive contribution from the QCD radiative correction. Our estimate gives Γ(ηc2γ)=(67) keV\Gamma(\eta_c \rightarrow 2\gamma)=(6-7) ~keV and Γ(ηc2γ)=2 keV\Gamma(\eta_c^\prime \rightarrow 2\gamma)=2 ~keV, which are smaller than their nonrelativistic values. The hadronic widths Γ(ηc2g)=(1723) MeV\Gamma(\eta_c \rightarrow 2g)=(17-23) ~MeV and Γ(ηc2g)=(57) MeV\Gamma(\eta_c^\prime \rightarrow 2g)=(5-7)~MeV are then indicated accordingly to the first order QCD radiative correction, if αs(mc)=0.260.29\alpha_s(m_c)=0.26-0.29. The decay widths for bbˉb\bar b states are also estimated. We show that when making the assmption that the quarks are on their mass shells our expressions for the decay widths will become identical with that in the NRQCD theory to the next to leading order of v2v^2 and αs\alpha_s.Comment: 14 pages LaTex (2 figures included

    CP violation in the inclusive b -> s g decay in the framework of multi Higgs doublet models

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    We study the decay width and CP asymmetry of the inclusive process b--> s g (g denotes gluon) in the multi Higgs doublet models with complex Yukawa couplings, including next to leading QCD corrections. We analyse the dependencies of the decay width and CP asymmetry on the scale \mu and CP violating parameter \theta. We observe that there exist an enhancement in the decay width and CP asymmetry is at the order of 10^{-2}.Comment: 11 pages, 8 Figure

    Evaluation of Bovine Myosin Heavy Chain Isoforms and Muscle Fiber Cross-Sectional Area on the Eating Quality of 11 Different Beef Muscles

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    Objective: The objective of this study was to investigate the contribution of muscle fiber type and size on the eating quality of 11 different beef muscles. Study Description: Eleven different beef muscles were utilized from two separate studies. In study 1, shoulder clod, flank, knuckle, mock tender, top sirloin butt, brisket, eye of round, and ribeye were collected from 10 U.S. Department of Agriculture choice carcasses (n = 80), and each muscle was fabricated into steaks at 2 days postmortem. In study 2, strip loin, tri-tip, and heel were collected from 10 USDA low choice carcasses (n = 30). Myofibrillar proteins were extracted and analyzed by immunoblot to determine muscle fiber type. Cross sectional area (CSA) and muscle fiber diameter were determined under the microscope. An average of 400 fibers per sample were analyzed to determine CSA and muscle fiber diameter. Pearson correlation analysis was conducted to determine the relationship between muscle fiber type, CSA, and diameter with the results for the eating quality of beef as determined by a trained panel that were reported in previous studies. Results: In study 1, there was a positive correlation between fiber type 1 and initial juiciness (r = 0.37; P \u3c 0.05), sustained juiciness (r = 0.39; P \u3c 0.05) and lipid flavor (r = 0.41; P \u3c 0.05). Conversely, there was a negative correlation between fiber type 2A and initial juiciness (r = -0.40; P \u3c 0.05) sustained juiciness (r = -0.42; P \u3c 0.05), and lipid flavor (r = -0.45; P \u3c 0.01). Both studies saw a negative correlation between muscle fiber CSA and diameter with connective tissue content (P \u3c 0.05), but positive correlations to overall tenderness (P \u3c 0.05). The Bottom Line: This study shows that muscles predominated by type 1 fibers will likely deliver a higher eating quality experience for consumers, while muscles with more glycolytic fibers 2A and 2X will deliver a less favorable eating experience for consumers. On the other hand, these data also demonstrated that larger muscle fiber CSA and diameter are not necessarily a negative eating quality marker as muscles with those characteristics had less connective tissue and had greater tenderness scores

    First Observations of a "Fast Beam-Ion Instability"

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    We report the results of experiments on a "fast beam-ion instability" at the Advanced Light Source (ALS). This ion instability, which can arise even where the ions are not trapped over multiple beam passages, will likely be important for many future accelerators. In our experiments, we filled the ALS storage ring with helium gas, raising the pressure approximately two orders of magnitude above the nominal value. With gaps in the bunch train large enough to avoid conventional (multi-turn) ion trapping, we observed a factor of 2-3 increase in the vertical beam size along with coherent beam oscillations. The single-pass nature of this instability was demonstrated

    Calculation of the Coherent Synchrotron Radiation Impedance from a Wiggler

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    Most studies of Coherent Synchrotron Radiation (CSR) have only considered the radiation from independent dipole magnets. However, in the damping rings of future linear colliders, a large fraction of the radiation power will be emitted in damping wigglers. In this paper, the longitudinal wakefield and impedance due to CSR in a wiggler are derived in the limit of a large wiggler parameter KK. After an appropriate scaling, the results can be expressed in terms of universal functions, which are independent of KK. Analytical asymptotic results are obtained for the wakefield in the limit of large and small distances, and for the impedance in the limit of small and high frequencies.Comment: 10 pages, 8 figure

    Constraints on the Mass and Mixing of the 4th Generation Quark From Direct CP Violationϵ/ϵ\epsilon^{\prime}/\epsilon and Rare K Decays

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    We investigate the ϵ/ϵ\epsilon^{\prime} /\epsilon for KππK\to \pi\pi in a sequential fourth generation model. By giving the basic formulae for ϵ/ϵ\epsilon^{\prime}/\epsilon in this model, we analyze the numerical results which are dependent of mtm_{t^{\prime}} and imaginary part of the fourth CKM factor, ImVtsVtd{Im}V^{*}_{t^{'}s}V_{t^{'}d} (or VtsVtdV^{*}_{t^{'}s}V_{t^{'}d} and the fourth generation CKM matrix phase θ\theta). We find that, unlike the SM, when taking the central values of all parameters for ϵ/ϵ\epsilon^{\prime}/\epsilon, the values of ϵ/ϵ\epsilon^{\prime}/ \epsilon can easily fit to the current experimental data for all values of hadronic matrix elements estimated from various approaches. Also, we show that the experimental values of ϵ/ϵ\epsilon^{\prime}/\epsilon and rare K decays can provide a strong constraint on both mass and mixing of the fourth generation quark. When taking the values of hadronic matrix elements from the lattice or 1/N expansion calculations, a large region of the up-type quark mass mtm_{t^{\prime}} is excluded.Comment: 18 pages, 4 eps figure

    Neutrino Oscillations in Supersymmetry without Lepton number conservation and R-parity

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    With the on-shell renormalization scheme, we discuss neutrino masses up to one-loop approximation in the Supersymmetry without lepton number conservation and R-parity. Ii is shown that in this model with experimentally allowed parameters, Δm232,Δm122\Delta m^2_{23}, \Delta m^2_{12} and the mixing angles sinθ23,sinθ12|\sin\theta{23}|,|\sin\theta_{12}| which are consistent with the present observation values can be produced. We find that small neutrino mass (\leq 1 eV) sets a loose constraint on the R-parity violation parameters in the soft breaking terms.Comment: 22 pages, plus one ps figure, accepted for publication in PR

    An inclusive measurement of the photon energy spectrum in b->s gamma decays

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    We report a fully inclusive measurement of the flavour changing neutral current decay b->s gamma in the energy range 1.8 GeV < E* < 2.8 GeV, covering 95% of the total spectrum. Using 140 fb^-1 we obtain BF(b->s gamma)= 3.55 +/- 0.32 +0.30-0.31 +0.11-0.07, where the errors are statistical, systematic and from theory corrections. We also measure the first and second moments of the photon energy spectrum above 1.8 GeV and obtain = 2.292 +/- 0.026 +/- 0.034 GeV and -^2 = 0.0305 +/- 0.0074 +/- 0.0063 GeV^2, where the errors are statistical and systematic.Comment: RevTex4, 6 pages, Submitted to Phys.Rev.Lett. Replaced: added table of systematic errors. New results take into account radiative J/Psi decay

    Scanning tunneling microscopy and spectroscopy at low temperatures of the (110) surface of Te doped GaAs single crystals

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    We have performed voltage dependent imaging and spatially resolved spectroscopy on the (110) surface of Te doped GaAs single crystals with a low temperature scanning tunneling microscope (STM). A large fraction of the observed defects are identified as Te dopant atoms which can be observed down to the fifth subsurface layer. For negative sample voltages, the dopant atoms are surrounded by Friedel charge density oscillations. Spatially resolved spectroscopy above the dopant atoms and above defect free areas of the GaAs (110) surface reveals the presence of conductance peaks inside the semiconductor band gap. The appearance of the peaks can be linked to charges residing on states which are localized within the tunnel junction area. We show that these localized states can be present on the doped GaAs surface as well as at the STM tip apex.Comment: 8 pages, 8 figures, accepted for publication in PR

    Nanometer-scale ablation with a table-top soft x-ray laser

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    Includes bibliographical references (page 3617).Ablation of holes with diameters as small as 82 nm and very clean walls was obtained in poly(methyl methacrylate) focusing pulses from a Ne-like Ar 46.9 nm compact capillary-discharge laser with a freestanding Fresnel zone plate diffracting into third order. These results demonstrate the feasibility of using focused soft x-ray laser beams for the direct nanoscale patterning of materials and the development of new nanoprobes
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