968 research outputs found

    Beyond CP violation: hadronic physics at BaBar

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    I report on recent studies of hadronic physics performed by the BaBar Collaboration. Emphasis is given to the measurement of the properties of newly discovered charmed hadrons and to the searches for light and heavy pentaquarks.Comment: 14 pages, 20 postscript figues, contributed to the Proceedings of the First APS Topical Group Meeting on Hadron Physics, Fermilab, Batavia, IL (October 24-26, 2004

    The Pattern of CP Asymmetries in b→sb\to s Transitions

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    New CP violating physics in b→sb\to s transitions will modify the CP asymmetries in B decays into final CP eigenstates (ϕKS\phi K_S, ηâ€ČKS\eta^\prime K_S, π0KS\pi^0 K_S, ωKS\omega K_S, ρ0KS\rho^0 K_S and ηKS\eta K_S) from their Standard Model values. In a model independent analysis, the pattern of deviations can be used to probe which Wilson coefficients get a significant contribution from the new physics. We demonstrate this idea using several well-motivated models of new physics, and apply it to current data.Comment: 20 pages, 3 figures, 6 tables. v3: Discussion of higher order corrections extended; Version appearing in JHE

    Developing a requirements management toolset: Lessons learned

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    Requirements Engineering (RE) is a multi-faceted discipline involving various methods, techniques and tools. RE researchers and practitioners are emphasizing the importance of having an integrated RE process. The need for an integrated toolset to support the effective management of such an integrated RE process cannot be over-emphasized. Tools integration has been identified as an important next step toward the future of requirements management tools. This paper reports on some of the significant architectural and technical issues encountered and the lessons learned in the process of developing an integrated Requirements Management (RM) Toolset: PARsed Natural language Input Processor (PARSNIP) by integrating various independent tools. This paper provides insights on architectural and technological issues typical of these types of projects, the approaches and techniques used to address the architectural mismatches and the technological incompatibilities

    The 2004 UTfit Collaboration Report on the Status of the Unitarity Triangle in the Standard Model

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    Using the latest determinations of several theoretical and experimental parameters, we update the Unitarity Triangle analysis in the Standard Model. The basic experimental constraints come from the measurements of |V_ub/V_cb|, Delta M_d, the lower limit on Delta M_s, epsilon_k, and the measurement of the phase of the B_d - anti B_d mixing amplitude through the time-dependent CP asymmetry in B^0 to J/psi K^0 decays. In addition, we consider the direct determination of alpha, gamma, 2 beta + gamma and cos(2 beta) from the measurements of new CP-violating quantities, recently performed at the B factories. We also discuss the opportunities offered by improving the precision of the various physical quantities entering in the determination of the Unitarity Triangle parameters. The results and the plots presented in this paper can also be found at http://www.utfit.org, where they are continuously updated with the newest experimental and theoretical results.Comment: 32 pages, 17 figures. High resolution figures and updates can be found at http://www.utfit.org v2: misprints correcte

    Nonleptonic charmless two-body B→ATB \to AT decays

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    In this work we have studied hadronic charmless two-body B decays involving p-wave mesons in final state. We have calculated branching ratios of B→ATB\to AT decays (where AA and TT denotes a 3P1^3P_1 axial-vector and a tensor meson, respectively), using B→TB \to T form factors obtained in the covariant light-front (CLF) approach, and the full effective Hamiltonian. We have obtained that B(B0→a1+a2−)=42.47×10−6\mathcal{B}(B^{0} \to a_{1}^{+}a_{2}^{-}) =42.47 \times10^{-6}, B(B+→a1+a20)=22.71×10−6\mathcal{B}(B^{+} \to a_{1}^{+}a_{2}^{0}) = 22.71 \times10^{-6}, B(B→f1K2∗)=(2.8−4)×10−6\mathcal{B}(B \to f_{1}K_{2}^{*}) = (2.8-4) \times 10^{-6} (with f1=,f1(1285),f1(1420)f_{1}=, f_{1}(1285),f_{1}(1420)) for ξ3P1=53.2∘\theta_{^{3}P_{1}} = 53.2^{\circ}, B(B→f1(1420)K2∗)=(5.91−6.42)×10−6\mathcal{B}(B \to f_{1}(1420)K_{2}^{*}) = (5.91-6.42) \times 10^{-6} with ξ3P1=27.9∘\theta_{^{3}P_{1}} = 27.9^{\circ}, B(B→K1a2)=(1.7−5.7)[1−9.3]×10−6\mathcal{B}(B \to K_{1}a_{2})= (1.7 - 5.7) [1-9.3] \times10^{-6} for ξK1=−37∘[−58∘]\theta_{K_{1}} = -37^{\circ} [-58^{\circ}] where K1=K1(1270),K1(1400)K_1 = K_1(1270), K_1(1400). It seems that these decays can be measured in experiments at BB factories. Additionally, we have found that B(B→K1(1270)a2)/B(B→K1(1400)a2)\mathcal{B}(B \to K_{1}(1270)a_{2})/\mathcal{B}(B \to K_{1}(1400)a_{2}) and B(B→f1(1420)K2∗)/B(B→f1(1285)K2∗)\mathcal{B}(B \to f_1(1420)K_{2}^{*})/\mathcal{B}(B \to f_1(1285)K_{2}^{*}) ratios could be useful to determine numerical values of mixing angles ξK1\theta_{K_{1}} and ξ3P1\theta_{^{3}P_{1}}, respectively.Comment: 12 page

    Using goals to model strategy map for business IT alignment

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    Strategy Map (SM) is one of the widely used methods to create business aligned IT strategy map providing valuable insights to business executives. However, problem with strategy map method is that it is not easy to use which can lend itself to various interpretations. This is because linkages between the strategic objectives in the four strategy map perspectives are not explicit which makes SM ambiguous. Goal modelling approaches from Requirements Engineering (RE) have proven rigorous in elicitation and representation of information system requirements. In an attempt to make explicit the causal relationships of SM linkages meaningful this research proposes the use of goal modelling approach i*

    Constraining the Unitarity Triangle with B -> V gamma

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    We discuss the exclusive radiative decays B→K∗γB\to K^{*}\gamma, Bâ†’ÏÎłB \to\rho\gamma, and Bâ†’Ï‰ÎłB\to\omega\gamma in QCD factorization within the Standard Model. The analysis is based on the heavy-quark limit of QCD. Our results for these decays are complete to next-to-leading order in QCD and to leading order in the heavy-quark limit. Special emphasis is placed on constraining the CKM-unitarity triangle from these observables. We propose a theoretically clean method to determine CKM parameters from the ratio of the B→ρlÎœB\to\rho l\nu decay spectrum to the branching fraction of Bâ†’ÏÎłB\to\rho\gamma. The method is based on the cancellation of soft hadronic form factors in the large energy limit, which occurs in a suitable region of phase space. The ratio of the Bâ†’ÏÎłB\to\rho\gamma and B→K∗γB\to K^{*}\gamma branching fractions determines the side RtR_{t} of the standard unitarity triangle with reduced hadronic uncertainties. The recent Babar bound on B(B0→ρ0Îł)B(B^0\to\rho^0\gamma) implies Rt<0.81(Ο/1.3)R_t < 0.81 (\xi/1.3), with the limiting uncertainty coming only from the SU(3) breaking form factor ratio Ο\xi. This constraint is already getting competitive with the constraint from BsB_{s}-Bˉs\bar B_{s} mixing. Phenomenological implications from isospin-breaking effects are briefly discussed.Comment: 23 pages, 8 figure

    Phenomenological Constraints on Extended Quark Sectors

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    We study the flavor physics in two extensions of the quark sector of the Standard Model (SM): a four generation model and a model with a single vector--like down--type quark (VDQ). In our analysis we take into account the experimental constraints from tree--level charged current processes, rare Kaon decay processes, rare B decay processes, the Z→bbˉZ\to b \bar{b} decay, KK, BB and DD mass differences, and the CP violating parameters \frac \epsilon^\prime}{\epsilon}, Ï”K\epsilon_K and aψKa_{\psi K}. All the constraints are taken at two sigma. We find bounds on parameters which can be used to represent the New Physics contributions in these models (λtâ€Čbd\lambda_{t^ \prime}^{bd}, λtâ€Čbs\lambda_{t^ \prime}^{bs} and λtâ€Čsd\lambda_{t^ \prime}^{sd} in the four--generation model, and UbdU_{bd}, UbsU_{bs} and UsdU_{sd} in the VDQ model) due to all the above constraints. In both models the predicted ranges for aSLa_{SL} (the CP asymmetry in semi-leptonic decays), ΔMD\Delta M_D, B(K+→π+ΜΜˉ)B(K^+\to\pi^+ \nu \bar{\nu}), B(KL→π0ΜΜˉ)B(K_L\to\pi^0 \nu \bar{\nu}) and B(KL→ΌΌˉ)SDB(K_L\to \mu \bar{\mu})_{SD} can be significantly higher than the predictions of the SM, while the allowed ranges for aψKa_{\psi K} and for ΔmBS\Delta m_{B_S} are consistent with the SM prediction.Comment: 22 pages, 5 figures (v3: added a reference, updated a reference, added missing units

    Quenched lattice calculation of semileptonic heavy-light meson form factors

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    We calculate, in the continuum limit of quenched lattice QCD, the matrix elements of the heavy-heavy vector current between heavy-light pseudoscalar meson states. We present the form factors for different values of the initial and final meson masses at finite momentum transfer. In particular, we calculate the non-perturbative correction to the differential decay rate of the process B --> D l nu including the case of a non-vanishing lepton mass.Comment: 16 pages, 10 figures, version accepted for publication on JHE

    Drug Interaction Study Of Apixaban With Cyclosporine Or Tacrolimus: Results From A Phase 1, Randomized, Open-Label, Crossover Study In Healthy Volunteers

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    BACKGROUND Solid organ transplant recipients commonly require anticoagulation. Apixaban (APX) is principally metabolized by CYP3A4, undergoes direct intestinal excretion, and is a substrate to P-glycoprotein (P-gp) and Breast Cancer Resistance Protein (BCRP) transporters. We examined the potential drug interaction between cyclosporine (CsA) and tacrolimus (Tac) [combined inhibitors of CYP3A4, P-gp and, BCRP] with APX.https://jdc.jefferson.edu/petposters/1005/thumbnail.jp
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