12 research outputs found

    Equivalence of matter-type modified gravity theories to general relativity with nonminimal matter interaction

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    We show that gravity models, such as f(Lm)f(\mathcal{L}_{\rm m}), f(gμνTμν)f(g_{\mu\nu} T^{\mu\nu}) and f(TμνTμν)f(T_{\mu\nu} T^{\mu\nu}), that modify the introduction of the material source in the usual Einstein-Hilbert action by adding only matter-related terms to the matter Lagrangian density Lm\mathcal{L}_{\rm m} are equivalent to general relativity with nonminimal interactions. Through the redefinition Lm+f→Lmtot\mathcal{L}_{\rm m}+f \rightarrow \mathcal{L}_{\rm m}^{\rm tot}, these models are exactly GR, yet the usual material field TμνT_{\mu\nu} and its accompanying partner, viz., the modification field TμνmodT_{\mu\nu}^{\rm mod} interact nonminimally. That is, ∇μTμν=−Qν=−∇μTμνmod\nabla^{\mu}T_{\mu\nu}=-Q_{\nu}=-\nabla^{\mu}T_{\mu\nu}^{\rm mod}, where QνQ_{\nu} is the interaction kernel that governs the rate of energy transfer. We focus on the particular model, the energy-momentum squared gravity, where the usual material field TμνT_{\mu\nu} brings in an accompanying energy-momentum squared field , TμνemsfT_{\mu\nu}^{\rm emsf} along with a sui generis nonminimal interaction between them. Compared to usual phenomenological nonminimal interaction models in the literature, EMSF gives rise to more intricate interaction kernels having covariant formulation even with simple forms of the ff function. We elaborate upon EMSF via some different aspects: a DE component induced from the interaction of sources such as cold dark matter and relativistic species with their accompanying EMSFs generating interacting DE-DM models, mimicking noncanonical scalar field, etc., or a Hoyle-type creation field generating steady-state universe models extended to fluids other than dust and a mimicker of modified generalized Chaplygin gas. We also demonstrate the proper calculation of second metric variation of Lm\mathcal{L}_{\rm m}, as well as in models that contain scalars like gμνTμν ,RμνTμνg_{\mu\nu} T^{\mu\nu}\,,R_{\mu\nu}T^{\mu\nu} and GμνTμνG_{\mu\nu} T^{\mu\nu}.Comment: 16 pages, no figures and table

    Double-Lepton Polarization Asymmetries and Branching Ratio of the B\rar \gamma l^+ l^- transition in Universal Extra Dimension

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    We study the radiative dileptonic B \rar \gamma l^+ l^- transition in the presence of a universal extra dimension in the Applequist-Cheng-Dobrescu model. In particular, using the corresponding form factors calculated via light cone QCD sum rules, we analyze the branching ratio and double lepton polarization asymmetries related to this channel and compare the results with the predictions of the standard model. We show how the results deviate from predictions of the standard model at lower values of the compactification factor (1/R1/R ) of extra dimension.Comment: 20 Pages and 8 Figure

    B to strange tensor meson transition in a model with one universal extra dimension

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    We analyze the semileptonic B→K2∗(1430)l+l−B\to K_2^*(1430)l^+l^- transition in universal extra dimension model. In particular, we present the sensitivity of related observables such as branching ratio, polarization distribution and forward-backward asymmetry to the compactification factor (1/R) of extra dimension. The obtained results from extra dimension model show overall a considerable deviation from the standard model predictions for small values of the compactification factor. This can be considered as an indication for existence of extra dimensions.Comment: 10 Pges, 6 Figures and 2 Table

    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 Λb→Λℓ+ℓ−\Lambda_{b}\rightarrow \Lambda \ell^{+}\ell^{-} transition in the standard model containing fourth generation quarks (SM4). We discuss effects of the presence of t′t' 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 Λb→Λℓ+ℓ−\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 mt′≥400GeVm_{t'}\geq 400 GeV.Comment: 22 Pages and 21 Figure

    Constraint on compactification scale via recently observed baryonic Λb→Λℓ+ℓ−\Lambda_b\rightarrow \Lambda \ell^+ \ell^- channel and analysis of the Σb→Σℓ+ℓ−\Sigma_b \rightarrow \Sigma \ell^+ \ell^- transition in SM and UED scenario

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    We obtain a lower limit on the compactification scale of extra dimension via comparison of the branching ratio in the baryonic Λb→Λμ+μ−\Lambda_b\rightarrow \Lambda \mu^+ \mu^- decay channel recently measured by CDF collaboration and our previous theoretical study. We also use the newly available form factors calculated via light cone QCD sum rules in full theory to analyze the flavour changing neutral current process of the Σb→Σℓ+ℓ−\Sigma_b \rightarrow \Sigma \ell^+ \ell^- in universal extra dimension scenario in the presence of a single extra compact dimension. We calculate various physical quantities like branching ratio, forward-backward asymmetry, baryon polarizations and double lepton polarization asymmetries defining the decay channel under consideration. We also compare the obtained predictions with those of the standard model.Comment: 32 Pages, 27 Figures and one Tabl
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