212 research outputs found

    Assessing the Triple Deficit Hypothesis for Major South Asian Countries: A Panel Data Analysis

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    The paper examines the ‘triple deficit hypothesis'-an extension of the ‘twin deficit hypothesis' with inclusion of private saving gap for a panel of five South Asian countries, namely India, Pakistan, Bangladesh, Srilanka and Nepal for the period 1985-2015. The results based on first and second generation panel cointegration tests indicate long-run relationship among budget balance (BB), current account balance (CAB) and private saving gap. The long-run coefficients obtained using MG-DOLS, MG-FMOLS and CCEMG indicate positive impact of BB and private saving gap on CAB thus confirming triple deficit hypothesis. The causality analysis reveals feedback relationship between CAB and BB implying that improvement in CAB requires fiscal austerity but fiscal adjustment is not fully policy controlled and requires adjustment in current account. Further, the causation also runs from saving gap to CAB and BB implying that plugging the saving gap would help improve both current account and budget balance. Keywords:  Triple Deficit Hypothesis, South Asia, Panel Cointegration, Panel Causality, GM-DOLS, GM- FMOLS, CCEMG Estimator JEL Classifications: E60, F32, H6

    Effect of FCNC mediated Z boson on lepton flavor violating decays

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    We study the three body lepton flavor violating (LFV) decays μee+e\mu^- \to e^- e^+ e^-, τlilj+lj\tau^- \to l_i^- l_j^+ l_j^- and the semileptonic decay τμϕ\tau \to \mu \phi in the flavor changing neutral current (FCNC) mediated ZZ boson model. We also calculate the branching ratios for LFV leptonic B decays, Bd,sμeB_{d,s} \to \mu e, Bd,sτeB_{d,s} \to \tau e, Bd,sτμB_{d,s} \to \tau \mu and the conversion of muon to electron in Ti nucleus. The new physics parameter space is constrained by using the experimental limits on μee+e\mu^- \to e^- e^+ e^- and τμμ+μ\tau^- \to \mu^- \mu^+ \mu^-. We find that the branching ratios for τeee\tau \to eee and τμϕ\tau \to \mu \phi processes could be as large as O(108)\sim {\cal O}(10^{-8}) and BrBd,sτμ,τe)O(1010){\rm Br}B_{d,s} \to \tau \mu, \tau e) \sim {\cal O}(10^{-10}). For other LFV B decays the branching ratios are found to be too small to be observed in the near future.Comment: 15 pages, 8 figures, typos corrected, one more section added, version to appear in EPJ

    Signature of new physics in B -> phi pi decay

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    We investigate the effect of an extra fourth quark generation and FCNC mediated ZZ and ZZ' bosons on the rare decay mode BϕπB^- \to \phi \pi^-. In the standard model, this mode receives only bdb \to d penguin contributions and therefore, highly suppressed with branching ratio 5×109\sim 5 \times 10^{-9}. This in turn makes this mode a very sensitive probe for new physics. We find that due to the above mentioned new physics contributions there is a significant enhancement in its branching ratio. Furthermore, the direct CP violation parameter which is identically zero in the SM is found to be quite significant. If this mode will be observed in the upcoming LHCb experiment, it will not only provide a clear signal of new physics but also can be used to constrain the new physics parameter space.Comment: 13 pages, 3 figures, version to appear in Phys. Lett.

    Possibility of extracting the weak phase γ\gamma from ΛbΛD0\Lambda_b \to \Lambda D^0 decays

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    We explore the possibility of extracting the weak phase γ\gamma from pure tree decays ΛbΛ(D0,D0ˉ,DCP0)\Lambda_b \to \Lambda (D^0, \bar{D^0}, D^0_{CP}) in a model independent way. The CP violating weak phase γ\gamma can be determined cleanly, without any hadronic uncertainties, as these decay modes are free from the penguin pollutions. Furthermore, neither tagging nor time dependent studies are required to extract the angle γ\gamma with these modes.Comment: 12 pages, LaTex, Minor changes in the text, version to appear in Phys. Rev.

    Probing the unparticle signal in bdb \to d penguin processes

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    We investigate the effect of unparticles in the pure bd b \to d penguin processes B0K0Kˉ0 B^0 \to K^0 \bar K^0 and B+,0ϕπ+,0B^{+,0} \to \phi \pi^{+,0} . Since these processes receive dominant contributions due to the {\it top} quark in the loop, direct and mixing-induced CP asymmetry parameters in these processes are expected to be vanishingly small in the standard model. We find that due to the unparticle effect sizable nonzero CP violation could be possible in these channels.Comment: 12 pages, 4 figures, version to appear in Phys. Lett.

    Exploring the Unitarity Triangle through CP violation observables in BsK+KB_s \to K^+ K^-

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    We discuss the determination of the CKM parameters from the forthcoming CPCP violation observables in BsK+KB_s \to K^+ K^- decays. Combining the information on mixing induced CP violation in BsK+KB_s \to K^+ K^-, with the BdJ/ψKsB_d \to J/\psi K_s precision observable sin2β\sin 2\beta and the Bs0B^0_s--Bs0ˉ\bar{B^0_s} mixing phase ϕs\phi_s, we propose a determination of the unitarity triangle (ρˉ,ηˉ)(\bar\rho, \bar\eta). Computing the penguin parameters (r,θ)(r, \theta) within QCD factorization yield precise determination of (ρˉ,ηˉ)(\bar\rho, \bar\eta), reflected by a weak dependence on the θ\theta which is shown as a second order effect. The impact of the direct CP violation observable CKKC_{KK} on the penguin parameters are investigated and a lower bound on CKKC_{KK} is extracted. We also discuss the effect of the Bs0B^0_s--Bs0ˉ\bar{B^0_s} new physics mixing phase on the penguin parameters (r,θ)(r, \theta) and SKKS_{KK}. Using the SU(3)-flavour symmetry argument and the current BB-factories data provided by the Bdπ+πB_d \to \pi^+ \pi^- modes, we complement the BsK+KB_s \to K^+ K^- CP-violating observables in a variety of ways, in particular we find that SKK>0S_{KK}>0. Finally we analyze systematically the SU(3)-symmetry breaking factor within QCD factorization.Comment: 22 pages, 6 figures, typos corrected, reference and some remarks adde

    Study of f_0(980) and f_0(1500) from B_s \to f_0(980)\pi, f_0(1500)\pi Decays

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    In this paper, we analyze the scalar mesons f0(980)f_0(980) and f0(1500)f_0(1500) from the decays Bˉs0f0(980)π0,f0(1500)π0\bar B^0_s \to f_0(980)\pi^0, f_0(1500)\pi^0 within Perturbative QCD approach. From the leading order calculations, we find that (a) in the allowed mixing angle ranges, the branching ratio of Bˉs0f0(980)π0\bar B^0_s\to f_0(980)\pi^0 is about (1.01.6)×107(1.0\sim1.6)\times 10^{-7}, which is smaller than that of Bˉs0f0(980)K0\bar B^0_s\to f_0(980)K^0 (the difference is a few times even one order); (b) the decay Bˉs0f0(1500)π0\bar B^0_s \to f_0(1500)\pi^0 is better to distinguish between the lowest lying state or the first excited state for f0(1500)f_0(1500), because the branching ratios for two scenarios have about one-order difference in most of the mixing angle ranges; and (c) the direct CP asymmetries of Bˉs0f0(1500)π0\bar B^0_s \to f_0(1500)\pi^0 for two scenarios also exists great difference. In scenario II, the variation range of the value ACPdir(Bˉs0f0(1500)π0){\cal A} ^{dir}_{CP}(\bar B^0_s \to f_0(1500)\pi^0) according to the mixing angle is very small, except for the values corresponding to the mixing angles being near 9090^\circ or 270270^\circ, while the variation range of ACPdir(Bˉs0f0(1500)π0){\cal A} ^{dir}_{CP}(\bar B^0_s \to f_0(1500)\pi^0) in scenario I is very large. Compared with the future data for the decay Bˉs0f0(1500)π0\bar B^0_s \to f_0(1500)\pi^0, it is ease to determine the nature of the scalar meson f0(1500)f_0(1500).Comment: 16 pages, 3 figures, Revte

    Analysis of \Lambda_b \rar \Lambda \ell^+ \ell^- transition in SM4 using form factors from Full QCD

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    Using the responsible form factors calculated via full QCD, we analyze the ΛbΛ+\Lambda_{b}\rightarrow \Lambda \ell^{+}\ell^{-} transition in the standard model containing fourth generation quarks (SM4). We discuss effects of the presence of tt' fourth family quark on related observables like branching ratio, forward-backward asymmetry, baryon polarization as well as double lepton polarization asymmetries. We also compare our results with those obtained in the SM as well as with predictions of the SM4 but using form factors calculated within heavy quark effective theory. The obtained results on branching ratio indicate that the ΛbΛ+\Lambda_{b}\rightarrow \Lambda \ell^{+}\ell^{-} transition is more probable in full QCD comparing to the heavy quark effective theory. It is also shown that the results on all considered observables in SM4 deviate considerably from the SM predictions when mt400GeVm_{t'}\geq 400 GeV.Comment: 22 Pages and 21 Figure

    B --> Phi K_S and Supersymmetry

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    The rare decay B --> Phi K_S is a well-known probe of physics beyond the Standard Model because it arises only through loop effects yet has the same time-dependent CP asymmetry as B --> Psi K_S. Motivated by recent data suggesting new physics in B --> Phi K_S, we look to supersymmetry for possible explanations, including contributions mediated by gluino loops and by Higgs bosons. Chirality-preserving LL and RR gluino contributions are generically small, unless gluinos and squarks masses are close to the current lower bounds. Higgs contributions are also too small to explain a large asymmetry if we impose the current upper limit on B(B_s --> mu mu). On the other hand, chirality-flipping LR and RL gluino contributions can provide sizable effects and while remaining consistent with related results in B --> Psi K_S, Delta M_s, B --> X_s gamma and other processes. We discuss how the LR and RL insertions can be distinguished using other observables, and we provide a string-based model and other estimates to show that the needed sizes of mass insertions are reasonable.Comment: 33 pages, 32 figures, Updated version for PRD. Includes discussions of other recent works on this topic. Added discussions & plots for gluino mass dependence and effects of theoretical uncertaintie
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