3,050 research outputs found

    CP\mathbf{\textit{CP}} Violation In The B(s)0\boldsymbol{B^0_{(s)}} System At LHCb

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    The study of C ⁣PC\!P violation in decays of neutral BB mesons provides an important test of the Standard Model (SM) predictions and it is a sensitive probe to search for non-SM physics. In these proceedings I present measurements of C ⁣PC\!P violation in the neutral BB meson system. The discussed analyses are based on pppp-collision data corresponding to an integrated luminosity of 1 fb1\mathrm{fb}^{-1} or 3 fb1\mathrm{fb}^{-1} recorded by the LHCb experiment.Comment: Proceedings of Moriond 2014, EW Interactions and Unified Theories, La Thuile, Aosta valley, Ital

    Measurements of B lifetimes at LHCb

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    Measurements of the Bs0B_s^0 effective lifetime in decays to CP-odd and CP-even flavour specific final states allow to probe the width difference ΔΓs\Delta \Gamma_s and the CP-violating phase ϕs\phi_s of Bs0Bˉs0B^0_s-\bar{B}^0_s mixing box-diagram. Measurements of the effective lifetime in the decay channels Bs0K+KB_s^0 \rightarrow K^+ K^- and Bˉs0J/ψf0(980)\bar{B}_s^0 \rightarrow J/\psi f_0(980) are presented, as well as a measurement of ΔΓs\Delta \Gamma_s and Γs\Gamma_s performed by a tagged time-dependent angular analysis of Bs0J/ψϕB_s^0 \rightarrow J/\psi \phi decays and a measurement of the sign of ΔΓs\Delta \Gamma_s, using data collected during 2011 with the LHCb detector.Comment: Proceedings of CKM 2012, the 7th International Workshop on the CKM Unitarity Triangle, University of Cincinnati, USA, 28 September - 2 October 201

    b-hadrons lifetime measurements using exclusive b -> J/psi(mu(+) mu(-)) X decays at LHCb

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    In the proceeding are reported precision measurement of differ ent b-hadrons lifetimes in the exclusive decays B+ -> J / psi K+ , B-0 -> j / psi K-*0 B-s(0) -> J / psi A, using 1 fb(-1) of data collected in 2011 with the LHCb detector at a centre-of-mass energy of 7 TeV

    Lifetime measurements in bb-hadron decays at LHCb

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    Precision lifetime measurements of bb-flavoured hadrons are an important test of the validity of the theoretical tool used to determine bb-hadrons observables, the Heavy Quark Expansion. Recent measurements of the B+B^+, Λb0\Lambda^0_b, Ξb\Xi^-_b, Ξb0\Xi^0_b and Ωb\Omega^-_b hadrons lifetimes are reported. Moreover, several B0B^0 and Bs0B^0_s effective lifetime measurements are discussed, as well as a measurement of the decay width difference in the B0B^0 system, ΔΓd\Delta \Gamma_d. All the measurements have been performed using pppp collision data collected with the LHCb detector.Comment: Proceedings of the 8th International Workshop on the CKM Unitarity Triangle (CKM 2014), Vienna, Austria, September 8-12, 201

    Lifetime measurements of beauty hadrons at the LHCb experiment

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    This thesis presents several lifetime measurements of b-flavoured hadrons at the LHCb experiment. They represent an important test of the theoretical approach to b-hadron observables known as HeavyQuark Expansion (HQE). This analysis uses data corresponding to an integrated luminosity of 1 fb-1 collected in proton-proton collisions at a centre-of-mass energy of 7 TeV. For the decays B+ -> J/psi K+, B0 -> J/psi K*0, B0 -> J/psi K0S, Lambdab -> J/psi Lambda and B0s -> J/psi phi the lifetimes are measured to be tau(B+ -> J/psi K+) = 1.637 +- 0.004 +- 0.003 ps, tau(B0 -> J/psi K*0) = 1.524 +- 0.006 +- 0.004 ps, tau(B0 -> J/psi K0S) = 1.499 +- 0.013 +- 0.005 ps, tau(Lambdab -> J/psi Lambda) = 1.415 +- 0.027 +- 0.006 ps, tau(B0s -> J/psi phi) = 1.480 +- 0.011 +- 0.005 ps, where the first uncertainty is statistical and the second is systematic. These are the most precise lifetime measurements in these decay modes to date. Ratios of these lifetimes also are reported in this thesis, as they are well-defined quantities where many theoretical or experimental uncertainties cancel. The ratio of the decay width difference, Delta Gamma_d, to the average width, Gamma_d, in the B0 system is found to be Delta Gamma_d/ Gamma_d = - 0.044 +- 0.025 +- 0.011. Using data corresponding to an integrated luminosity of 3 fb-1 collected at centre-of-mass energies of 7 TeV and 8 TeV, the measurements of the decay width difference, Delta Gamma_s, and the average width, Gamma_s, in the B0s system are performed. Using the decay B0s -> J/psi phi, they are measured to be Delta Gamma_s = 0.0805 +- 0.0091 +- 0.0033 ps-1, Gamma_s = 0.6603 +- 0.0027 +- 0.0015 ps-1. These are the most precise determinations of these observables ot date. All measurements are consistent with HQE predictions

    On the impact of the Migdal effect in reactor CEν\nuNS experiments

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    The search for coherent elastic neutrino nucleus scattering (CEν\nuNS) using reactor antineutrinos represents a formidable experimental challenge, recently boosted by the observation of such a process at the Dresden-II reactor site using a germanium detector. This observation relies on an unexpected enhancement at low energies of the measured quenching factor with respect to the theoretical Lindhard model prediction, which implies an extra observable ionization signal produced after the nuclear recoil. A possible explanation for this additional contribution could be provided by the so-called Migdal effect, which however has never been observed. Here, we study in detail the impact of the Migdal contribution to the standard CEν\nuNS signal calculated with the Lindhard quenching factor, finding that the former is completely negligible for observed energies below 0.3keV\sim 0.3\,\mathrm{keV} where the signal is detectable, and thus unable to provide any contribution to CEν\nuNS searches in this energy regime. To this purpose, we compare different formalisms used to describe the Migdal effect that intriguingly show a perfect agreement, making our findings robust.Comment: 5 pages, 2 figure
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