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"Archilli, F."
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Flavour-changing neutral currents making and breaking the standard model
The standard model of particle physics is our best description yet of fundamental particles and their interactions, but it is known to be incomplete. As yet undiscovered particles and interactions might exist. One of the most powerful ways to search for new particles is by studying processes known as flavour-changing neutral current decays, whereby a quark changes its flavour without altering its electric charge. One example of such a transition is the decay of a beauty quark into a strange quark. Here we review some intriguing anomalies in these decays, which have revealed potential cracks in the standard model—hinting at the existence of new phenomena.
The standard model of particle physics is incomplete, but experimental particle decays that occur through a ‘flavour-changing neutral current’ process, which show discrepancies to standard model predictions, may offer hints to the existence of new particles.
Challenging lepton interaction theory
The standard model of particle physics predicts that interactions of leptons (electrons, muons and taus) should differ only because of their different masses. But three collaborations, LHCb at CERN, BaBar at the SLAC National Accelerator Laboratory and Belle at the KEK High Energy Accelerator Research Organization, have recently performed measurements of leptonic and semileptonic decays of the
B
meson that challenge this prediction. Currently, these measurements are at a level of significance of four standard deviations, but the gold standard for particle physics is five. Here, members of all three collaborations review the state of the field and discuss how the standard model might be amended to accommodate the observations.
Journal Article
LHCb data quality monitoring
Data quality monitoring, DQM, is crucial in a high-energy physics experiment to ensure the correct functioning of the experimental apparatus during the data taking. DQM at LHCb is carried out in two phases. The first one is performed on-site, in real time, using unprocessed data directly from the LHCb detector, while the second, also performed on-site, requires the reconstruction of the data selected by the LHCb trigger system and occurs later. For the LHC Run II data taking the LHCb collaboration has re-engineered the DQM protocols and the DQM graphical interface, moving the latter to a web-based monitoring system, called Monet, thus allowing researchers to perform the second phase off-site. In order to support the operator's task, Monet is also equipped with an automated, fully configurable alarm system, thus allowing its use not only for DQM purposes, but also to track and assess the quality of LHCb software and simulation over time.
Journal Article
Precise measurement of Γ(K→e ν(γ))/Γ(K→μ ν(γ)) and study of K→e ν γ
We present a precise measurement of the ratio RK=Γ(K→eν(γ))/Γ(K→μν(γ)) and a study of the radiative process K→eνγ, performed with the KLOE detector. The results are based on data collected at the Frascati e+e− collider DAΦNE for an integrated luminosity of 2.2 fb−1. We find RK=(2.493±0.025stat±0.019syst)×10−5, in agreement with the Standard Model expectation. This result is used to improve constraints on parameters of the Minimal Supersymmetric Standard Model with lepton flavor violation. We also measured the differential decay rate dΓ(K→eνγ)/dEγ for photon energies 10
Journal Article
Precision measurement of the K S meson lifetime with the KLOE detector
Using a large sample of pure, slow, short lived K0 mesons collected with KLOE detector at DAΦNE, we have measured the KS lifetime. From a fit to the proper time distribution we find τ(KS)=(89.562±0.029stat±0.043syst) ps. This is the most precise measurement to date of the short lived K0 meson lifetime, in good agreement with the world average derived from previous measurements. We observe no dependence of the lifetime on the direction of the KS in galactic coordinates.
Journal Article
Measurement of the CKM angleγinB^(±)→ D K^(±)andB^(±) → D π^(±)decays withD → K_(\\mathrm) S⁰ h⁺ h
A measurement of CP-violating observables is performed using the decays B $^{±}$→ DK $^{±}$and B $^{±}$→ Dπ $^{±}$ , where the D meson is reconstructed in one of the self-conjugate three-body final states$ {K}_{\\mathrm{S}}^0 $ π $^{+}$ π $^{−}$and$ {K}_{\\mathrm{S}}^0 $ K $^{+}$ K $^{−}$(commonly denoted$ {K}_{\\mathrm{S}}^0 $ h $^{+}$ h $^{−}$ ). The decays are analysed in bins of the D-decay phase space, leading to a measurement that is independent of the modelling of the D-decay amplitude. The observables are inter- preted in terms of the CKM angle γ. Using a data sample corresponding to an integrated luminosity of 9 fb $^{−1}$collected in proton-proton collisions at centre-of mass energies of 7, 8, and 13 TeV with the LHCb experiment, γ is measured to be$ \\left({68.7}_{-5.1}^{+5.2}\\right){}^{\\circ} $ . The hadronic parameters$ {r}_B^{D K},{r}_B^{D\\pi},{\\delta}_B^{D K},\\kern0.5em \\mathrm{and}\\kern0.5em {\\delta}_B^{D\\pi} $ , which are the ratios and strong-phase differences of the suppressed and favoured B $^{±}$decays, are also reported.[graphic not available: see fulltext]
Journal Article
Measurement ofZ→τ⁺τ⁻production in proton-proton collisions at√s̅ = 8TeV
A measurement of Z → τ ⁺ τ ⁻production cross-section is presented using data, corresponding to an integrated luminosity of 2 fb ⁻¹ , from pp collisions at √s̅=8 TeV collected by the LHCb experiment. The τ ⁺ τ ⁻candidates are reconstructed in final states with the first tau lepton decaying leptonically, and the second decaying either leptonically or to one or three charged hadrons. The production cross-section is measured for Z bosons with invariant mass between 60 and 120 GeV/c ² , which decay to tau leptons with transverse momenta greater than 20 GeV/c and pseudorapidities between 2.0 and 4.5. The cross-section is determined to be σ_(pp)_(→ Z→ τ⁺)_(τ⁻)=95.8 ± 2.1 ± 4.6 ± 0.2 ± 1.1 pb, where the first uncertainty is statistical, the second is systematic, the third is due to the LHC beam energy uncertainty, and the fourth to the integrated luminosity uncertainty. This result is compatible with NNLO Standard model predictions. The ratio of the cross-sections for Z → τ ⁺ τ ⁻to Z → μ ⁺ μ ⁻(Z → e ⁺ e ⁻ ), determined to be 1.01 ± 0.05 (1.02 ± 0.06), is consistent with the lepton-universality hypothesis in Z decays.
Journal Article
Observation of the decayB_(s)⁰ → η_(c) φand evidence forB_(s)⁰ → η_(c) π⁺ π
A study ofB⁰_(s) → η_(c) φandB⁰_(s) → η_(c) π⁺π⁻decays is performed usingppcollision data corresponding to an integrated luminosity of 3.0 \\rm fb⁻¹ , collected with the LHCb detector in Run 1 of the LHC. The observation of the decayB⁰_(s) → η_(c) φis reported, where theη_(c)meson is reconstructed in thepp̄ ,K⁺K⁻π⁺π⁻ ,π⁺π⁻π⁺π⁻andK⁺K⁻K⁺K⁻decay modes and theφ(1020)in theK⁺ K⁻decay mode. The decayB⁰_(s) → J/ψ φis used as a normalisation channel. Evidence is also reported for the decayB⁰_(s) → η_(c) π⁺π⁻ , where theη_(c)meson is reconstructed in thepp̄decay mode, using the decayB⁰_(s) → J/ψ π⁺ π⁻as a normalisation channel. The measured branching fractions are eqnarray* B (B⁰_(s) _(c) ) &=& (5.01 0.53 0.27 0.63 ) 10⁻4 ,
B (B⁰_(s) _(c) ⁺ ⁻) &=& (1.76 0.59 0.12 0.29 ) 10⁻4 , eqnarray* where in each case the first uncertainty is statistical, the second systematic and the third uncertainty is due to the limited knowledge of the external branching fractions.
Journal Article
Evidence for the two-body charmless baryonic decayB⁺ → p Λ
A search for the rare two-body charmless baryonic decayB⁺ → p Λ̄is performed withppcollision data, corresponding to an integrated luminosity of3\\mbox{ fb}{⁻¹}{} , collected by the LHCb experiment at centre-of-mass energies of 7 and 8 TeV. An excess ofB⁺ → p Λ̄candidates with respect to background expectations is seen with a statistical significance of 4.1 standard deviations, and constitutes the first evidence for this decay. The branching fraction, measured using theB⁺ → K⁰_(\\mathrm S) π⁺decay for normalisation, is eqnarray B(B⁺ p ) & = & ( 2.4 ⁺1.0₋0.8 0.3 ) 10⁻7 , eqnarray where the first uncertainty is statistical and the second systematic.
Journal Article
New algorithms for identifying the flavour of Formula: see text mesons using pions and protons
Two new algorithms for use in the analysis of [Formula: see text] collision are developed to identify the flavour of [Formula: see text] mesons at production using pions and protons from the hadronization process. The algorithms are optimized and calibrated on data, using [Formula: see text] decays from [Formula: see text] collision data collected by LHCb at centre-of-mass energies of 7 and 8 TeV . The tagging power of the new pion algorithm is 60% greater than the previously available one; the algorithm using protons to identify the flavour of a [Formula: see text] meson is the first of its kind.
Journal Article