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785 result(s) for "Passeri, A"
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The KLOE-2 experiment at DAΦNE
The KLOE-2 experiment is steadily taking data since November 2014 at the upgraded DAΦNE φ-factory, in Frascati Laboratories, collecting up to now about 2.4 fb-1 at a rate around 10 pb-1/day. Performances of the upgraded KLOE-2 detector, data taking conditions, data quality monitoring and physics perspectives are here discussed.
Measurement of the KS→ πeν branching fraction with the KLOE experiment
A bstract The ratio R = Γ( K S → πeν ) / Γ( K S → π + π − ) has been measured with a sample of 300 million K S mesons produced in ϕ → K L K S decays recorded by the KLOE experiment at the DAΦNE e + e − collider. K S → πeν events are selected by a boosted decision tree built with kinematic variables and time-of-flight measurements. Data control samples of K L → πeν decays are used to evaluate signal selection efficiencies. With 49647 ± 316 signal events we measure R = (1 . 0421 ± 0 . 0066 stat ± 0 . 0075 syst ) × 10 − 3 . The combination with our previous measurement gives R = (1 . 0338 ± 0 . 0054 stat ± 0 . 0064 syst ) × 10 − 3 . From this value we derive the branching fraction B ( K S → πeν ) = (7 . 153 ± 0 . 037 stat ± 0 . 044 syst ) × 10 − 4 and f + (0) |V us | = 0 . 2170 ± 0 . 009.
THU0425 18f-fluorodeoxyglucose positron emission tomography/computed tomography and lung involvement in systemic sclerosis
BackgroundAt early stages, SSc lung involvement is characterised by Ground Glass Opacities (GGO) at High Resolution Computed Tomography (HRCT). However, HRCT scan is not able to provide functional information and to discriminate between an “active inflammatory” and an “established fibrotic” GGO. 18Fluoro-Deoxy-d-Glucose (18F-FDG) Positron Emission Tomography/Computed Tomography (PET/CT) is able to detect metabolic activity picking up inflammation and provides both morphologic and metabolic data.ObjectivesThe aim of this study was to evaluate, if 18F-FDG PET/CT scan may identify the inflammatory component of GGO in SSc interstitial lung disease.MethodsSeven patients with SSc (1 male and 6 females; mean age 59.56 y±9.15 SD; median disease duration 5 years,2–11 who underwent 18F-FDG PET/CT scan because of cancer screening, were retrospectively analysed. HRCT images analysis led to classification of pulmonary segments as “negative” (normal morphology) and ”positive” (GGO). Furthermore, the “Warrick score” was used as a staging tool for SSc-ILD. Mean Standardised Uptake Value (mSUV) of segmental parechima was normalised (nmSUV) by comparison with the values of selected control subjets.ResultsNo SSc patient was affected by cancer. Three patients had a Warrick Score >0, while 4 patients did not had any lung involvement (Warrick Score=0). The 3 patients with a Warrick Score >0 had also skin involvement with a median mRSS 6 (2–7) and pathological lung FDG uptake. In “positive” segments of SSc patients, nmSUV was significantly higher than in the lung segments of the control population (mean estimation 1.53; C.I. 1.42–1.65, p<0.0001). In “negative” segments of SSc patients, with a Warrick score >0, the nmSUV was significantly higher than in segments of the control population (mean estimation 1.29; C.I. 1.22–1.37, p<0.0001). Lung segments with GGO showed an nmSUV higher (21%) than “negative” segments (C.I. 0.13–0.28, p<0.0001) of patients with Warrick score >0. “Negative” lung segments of patients with Warrick Score >0 showed a 32% higher 18F-FDG uptake than “negative” lung segments of patients with Warrick Score=0. (C.I. 0.17–0.48, p<0.0001). (figure 1)Abstract THU0425 – Figure 1a) Differences in 18F-FDG uptake between “positive” segments of Warrick score >0 SSc patients, “negative” segments of Warrick score >0 SSc patients and “negative” segments of Warrick score=0 SSc patients vs attended normalised control value (=1); b) Differences in 18F-FDG uptake between “positive” lung segments of SSc patients with Warrick score>0 vs “negative” segments of the same patients; c) Differences in 18F-FDG uptake “negative” lung segments of patients with Warrick Score>0 vs “negative” lung segments of patients with Warrick Score=0ConclusionsMorphologically “positive” GGO segments show an increased 18F-FDG uptake suggesting the existence of a metabolically active (inflammatory) GGO. However, in patients with GGO, negative lung segments showed a higher nmSUV than negative lung segments in patients without GGO. This may suggest that PET/CT may disclose an underlying inflammatory process, which cannot yet be evidenced by HRCT. Further studies on a larger population are warranted to confirm these data and possibly provide a prognostic significance of PET/CT positivity in SSc patients.Disclosure of InterestNone declared
Prospects for e+e- physics at Frascati between the φ and the ψ
We present a detailed study, done in the framework of the INFN 2006 Roadmap, of the prospects for e+e- physics at the Frascati National Laboratories. The physics case for an e+e- collider running at high luminosity at the φ resonance energy and also reaching a maximum center of mass energy of 2.5 GeV is discussed, together with the specific aspects of a very high luminosity τ-charm factory. Subjects connected to kaon decay physics are not discussed here, being part of another INFN Roadmap working group. The significance of the project and the impact on INFN are also discussed. All the documentation related to the activities of the working group can be found in http://www.roma1.infn.it/people/bini/roadmap.html.
B-flavor tagging at Belle II
We report on new flavor tagging algorithms developed to determine the quark-flavor content of bottom ( ) mesons at Belle II. The algorithms provide essential inputs for measurements of quark-flavor mixing and charge-parity violation. We validate and evaluate the performance of the algorithms using hadronic decays with flavor-specific final states reconstructed in a data set corresponding to an integrated luminosity of 62.8 fb-1, collected at the resonance with the Belle II detector at the SuperKEKB collider. We measure the total effective tagging efficiency to be εeff=(30.0±1.2(stat)±0.4(syst))%for a category-based algorithm and εeff=(28.8±1.2(stat)±0.4(syst))%for a deep-learning-based algorithm.
Combination of KLOE σ (e + e − → π+π−γ(γ)) measurements and determination of a μ π + π − in the energy range 0.10 < s < 0.95 GeV2
The three precision measurements of the cross section σ(e+e− → π+π−γ(γ)) using initial state radiation by the KLOE collaboration provide an important input for the prediction of the hadronic contribution to the anomalous magnetic moment of the muon. These measurements are correlated for both statistical and systematic uncertainties and, therefore, the simultaneous use of these measurements requires covariance matrices that fully describe the correlations. We present the construction of these covariance matrices and use them to determine a combined KLOE measurement for σ(e+e− → π+π−γ(γ)). We find, from this combination, a two-pion contribution to the muon magnetic anomaly in the energy range 0.10 < s < 0.95 GeV2 of aμπ+π−=489.8±1.7stat±4.8sys×10−10.Data vectors and covariance matrices are available at http://www.lnf.infn.it/kloe/ppg/ppg_2017/ppg_2017.html.
Search for lepton-flavor-violating τ decays into a lepton and a vector meson using the full Belle data sample
A bstract Charged-lepton-flavor-violation is predicted in several new physics scenarios. We update the analysis of τ lepton decays into a light charged lepton ( ℓ = e ± or μ ± ) and a vector meson ( V 0 = ρ 0 , ϕ , ω , K *0 , or K ¯ *0 ) using 980 fb − 1 of data collected with the Belle detector at the KEKB collider. No significant excess of such signal events is observed, and thus 90% credibility level upper limits are set on the τ → ℓV 0 branching fractions in the range of (1.7–4 . 3) × 10 − 8 . These limits are improved by 30% on average from the previous results.
Physics with the KLOE-2 experiment at the upgraded DAΦNE
Investigation at a φ -factory can shed light on several debated issues in particle physics. We discuss: (i) recent theoretical development and experimental progress in kaon physics relevant for the Standard Model tests in the flavor sector, (ii) the sensitivity we can reach in probing CPT and Quantum Mechanics from time evolution of entangled-kaon states, (iii) the interest for improving on the present measurements of non-leptonic and radiative decays of kaons and η / η ′ mesons, (iv) the contribution to understand the nature of light scalar mesons, and (v) the opportunity to search for narrow di-lepton resonances suggested by recent models proposing a hidden dark-matter sector. We also report on the e + e − physics in the continuum with the measurements of (multi)hadronic cross sections and the study of γ γ processes.
Search for a pentaquark state decaying into pJ/ψ in Υ(1, 2S) inclusive decays at Belle
A bstract Using the data samples of 102 million Υ(1 S ) and 158 million Υ(2 S ) events collected by the Belle detector, we search for a pentaquark state in the pJ/ψ final state from Υ(1 , 2 S ) inclusive decays. Here, the charge-conjugate is included. We observe clear pJ/ψ production in Υ(1 , 2 S ) decays and measure the branching fractions to be and . We also measure the cross section of inclusive pJ/ψ production in e + e − annihilation to be σ ( e + e − → pJ/ψ + anything ) = [108 ± 11( stat. ) ± 6( syst. )] fb at GeV using an 89 . 5 fb − 1 continuum data sample. There is no significant P c (4312) + , P c (4440) + or P c (4457) + signal found in the pJ/ψ final states in Υ(1 , 2 S ) inclusive decays. We determine the upper limits of to be at the 10 − 6 level.
Measurement of η → π0γγ branching fraction with the KLOE detector
A bstract We present a measurement of the doubly radiative decay η → π 0 γγ based on a sample of 82 million η mesons produced in the e + e − → ϕ → ηγ process at the Frascati ϕ -factory DAΦNE. From the data analysis, 1246 ± 133 signal events were observed. By normalising the signal to the well-known η → 3 π 0 decay the branching fraction is measured to be (0 . 98 ± 0 . 11 stat ± 0 . 14 syst ) × 10 − 4 . This result agrees with a preliminary KLOE measurement, but is a factor of two smaller than the current world average. Results for d Γ( η → π 0 γγ ) /dM 2 ( γγ ) are also presented and compared with the latest theoretical predictions.