36 research outputs found

    The Constraint on FCNC Coupling of the Top Quark with a Gluon from ep Collisions

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    Using the constraint on the single top production cross-section obtained at the HERA collider, σ(ep→etX)\sigma(ep \to e t X), we evaluate an upper limit on oupling constant of the anomalous top quark interaction with a gluon via flavor-changing neutral current: ∣Îștgq/Î›âˆŁâ‰€0.4TeV−1|\kappa_{tgq}/\Lambda| \le 0.4 {TeV}^{-1}, BR(t→gq)<13(t \to gq) < 13 % Comment: Latex, 3 figures, missed references were adde

    Study of ATLAS sensitivity to FCNC top decays

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    The ATLAS experiment sensitivity to top quark Flavour Changing Neutral Current (FCNC) decays was studied at LHC using ttbar events. While one of the top quarks is expected to follow the dominant Standard Model decay t->bW, the other decays through a FCNC channel, i.e. t-> Z u(c), t-> gamma u(c) or t-> g u(c). Different types of analyses, applied to each FCNC decay mode, were compared. The FCNC branching ratio sensitivity (assuming a 5sigma signal significance) and 95% confidence level limits on the branching ratios (in the hypothesis of signal absence) were obtained

    Theory and phenomenology of two-Higgs-doublet models

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    We discuss theoretical and phenomenological aspects of two-Higgs-doublet extensions of the Standard Model. In general, these extensions have scalar mediated flavour changing neutral currents which are strongly constrained by experiment. Various strategies are discussed to control these flavour changing scalar currents and their phenomenological consequences are analysed. In particular, scenarios with natural flavour conservation are investigated, including the so-called type I and type II models as well as lepton-specific and inert models. Type III models are then discussed, where scalar flavour changing neutral currents are present at tree level, but are suppressed by either specific ansatze for the Yukawa couplings or by the introduction of family symmetries. We also consider the phenomenology of charged scalars in these models. Next we turn to the role of symmetries in the scalar sector. We discuss the six symmetry-constrained scalar potentials and their extension into the fermion sector. The vacuum structure of the scalar potential is analysed, including a study of the vacuum stability conditions on the potential and its renormalization-group improvement. The stability of the tree level minimum of the scalar potential in connection with electric charge conservation and its behaviour under CP is analysed. The question of CP violation is addressed in detail, including the cases of explicit CP violation and spontaneous CP violation. We present a detailed study of weak basis invariants which are odd under CP. A careful study of spontaneous CP violation is presented, including an analysis of the conditions which have to be satisfied in order for a vacuum to violate CP. We present minimal models of CP violation where the vacuum phase is sufficient to generate a complex CKM matrix, which is at present a requirement for any realistic model of spontaneous CP violation.Comment: v3: 180 pages, 506 references, new chapter 7 with recent LHC results; referee comments taken into account; submitted to Physics Report

    Grundlagen

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    Deep-Inelastic inclusive ep Scattering at low x and a determination of αs\alpha s

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    Search for single top production via FCNC at LEP at S**(1/2)=189-gev to 208-GEV.

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    A search for single top production ( ) via flavour changing neutral currents (FCNC) was performed using the data taken by the DELPHI detector at LEP2. The data analyzed have been accumulated at center-of-mass energies ranging from 189 to 208 GeV. Limits at 95% confidence level were obtained on the anomalous coupling parameters ÎșÎł and ÎșZ

    Constraints on the KS0→Ό+Ό−K^0_S \rightarrow \mu^+ \mu^- Branching Fraction

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    International audienceA search for the decay KS0→Ό+ÎŒ- is performed using proton-proton collision data, corresponding to an integrated luminosity of 5.6  fb-1 and collected with the LHCb experiment during 2016, 2017, and 2018 at a center-of-mass energy of 13 TeV. The observed signal yield is consistent with zero, yielding an upper limit of B(KS0→Ό+ÎŒ-)<2.2×10-10 at 90% C.L.. The limit reduces to B(KS0→Ό+ÎŒ-)<2.1×10-10 at 90% C.L. once combined with the result from data taken in 2011 and 2012

    Measurement of the electron reconstruction efficiency at LHCb

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    International audienceThe single electron track-reconstruction efficiency is determined using a sample corresponding to 1.3 fb−11.3~\mathrm{fb}^{-1}of pppp collision data recorded with the LHCb detector in 2017. This measurement exploits B+→J/ψ(e+e−)K+B^+\to J/\psi (e^+e^-)K^+ decays, where one of the electrons is fully reconstructed and paired with the kaon, while the other electron is reconstructed using only the information of the vertex detector. Despite this partial reconstruction, kinematic and geometric constraints allow the B+B^+-meson mass to be reconstructed and the signal to be well separated from backgrounds. This in turn allows the electron reconstruction efficiency to be measured by matching the partial track segment found in the vertex detector to tracks found by LHCb's regular reconstruction algorithms. The agreement between data and simulation is evaluated, and corrections are derived for simulated electrons in bins of kinematics. The presented method allows LHCb to measure branching fractions involving single electrons with a an electron reconstruction systematic uncertainty below 1%1\%
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