911 research outputs found

    Functional imaging in neurodegenerative disorders: past, present and future

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    The present monographic issue of the Quarterly Journal of Nuclear Medicine and Molecular Imaging is dedicated to the role of functional imaging in the broad field of neurodegenerative disorders, with a special focus on some of the most relevant topics of the last decades, of the present time and of the near future. Functional neuroimaging is close to reach the time in which it will be routinely implemented in clinical practice and in which the principles of "molecular imaging" will aid clinical diagnosis disclosing the fine extra- and intracellular deposit of protein aggregates and neuroinflammation markers. The almost simultaneous advancement in nuclear medicine techniques, i.e., PET-MRI, along with the development of new tracers and the implementation of more and more sophisticated image analysis software will assign to neuroimaging a preeminent role in the diagnostic algorithm both in neurological and psychiatric practice

    Recensione di Edoardo Camassa, Quando la logica va in vacanza. Sulle fallacie comiche in letteratura (Quodlibet, 2020)

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    Recensione di Edoardo Camassa, Quando la logica va in vacanza. Sulle fallacie comiche in letteratura (Quodlibet, 2020

    Carmelo Bene, Tamerlano e la Biennale impossibile

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    In January 1988, against all odds, Carmelo Bene was appointed artistic director of Venice Biennale’s International Theatre Festival. The nomination was meant to last four years (1989-1992), but it abruptly ended after only two, with the resignation of Bene himself because of endless controversies with the board. The only notable accomplishment of Biennale’s Theatre section was a multidisciplinary workshop on Christopher Marlowe’s Tamburlain the Great, held on September 1989 under the title La ricerca impossibile ovvero il teatro senza spettacolo. The workshop involved musicians, singers and actors from Italy, France and Belgium. In order to understand that project from an historical and critical perspective, this paper is divided in two parts. The first one aims at retracing the sequence of events surrounding Bene’s appointment and resignation as artistic director. The second one tries to analyse the reasons that led the Italian actor to choose Tamburlaine the Great as his field of research on the concept of “macchina attoriale”. The investigation is founded on his own theoretical premises as expressed in his work La voce di Narciso. Finally, we provide probable reasons for the predictable failure of that impossible workshop.Nel gennaio del 1988 Carmelo Bene viene eletto, a sorpresa, direttore artistico della Biennale di Venezia – Sezione Teatro per il quadriennio 1989-1992. L’esperienza si concluderà con le dimissioni dello stesso Bene due anni dopo, a seguito di innumerevoli polemiche con il consiglio direttivo della Biennale, seguite negli anni successivi da lunghi strascichi legali. Di quella paradossale Biennale Teatro a direzione Bene resterà un Laboratorio multidisciplinare sul Tamerlano il Grande di Christopher Marlowe, tenutosi nel mese di settembre del 1989, intitolato La ricerca impossibile ovvero il teatro senza spettacolo, che ha visto coinvolti musicisti, cantanti e attori provenienti da Italia, Francia e Belgio. Allo scopo di inquadrare tale progetto in una prospettiva storico-critica, il presente articolo si divide in due sezioni: nella prima si ricostruiscono le vicende intorno all’elezione e alla direzione artistica di Bene; nella seconda ci si interroga sulle motivazioni che portarono l’attore salentino a scegliere il Tamerlano il Grande come campo di una ricerca sul concetto di “macchina attoriale”, alla luce dei presupposti teorici della sua drammaturgia espressi nel volume La voce di Narciso. Si propone infine un’analisi critica dell’esito prevedibilmente fallimentare di quel Laboratorio impossibile

    Role of Extracellular Vesicles in Human Papillomavirus-Induced Tumorigenesis

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    Emerging evidence demonstrates a role of extracellular vesicles (EVs) in a variety of fundamental physiological and pathological processes ranging from antigen presentation to T cell to neurodegenerative diseases. In several types of malignancies, a variety of EVs can be isolated from bodily fluids of cancer patients, and it has been reported that the number of circulating EVs seems to be higher than in healthy subjects. This increase correlates with poor prognosis. Data obtained from different groups clearly point out a role of EVs in the transfer of bioactive molecules such as microRNAs and viral oncoproteins in human papillomavirus-induced malignancies of genital and oral tracts. This study summarizes these data in the context of relevant literature considering the EVs as carriers of oncogenic signatures in human cancer as well as their therapeutic potential in HPV-related tumors

    Search for the rare decays B0→J/ÏˆÎłB^{0}\to J/\psi \gamma and Bs0→J/ÏˆÎłB^{0}_{s} \to J/\psi \gamma

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    A search for the rare decay of a B0B^{0} or Bs0B^{0}_{s} meson into the final state J/ÏˆÎłJ/\psi\gamma is performed, using data collected by the LHCb experiment in pppp collisions at s=7\sqrt{s}=7 and 88 TeV, corresponding to an integrated luminosity of 3 fb−1^{-1}. The observed number of signal candidates is consistent with a background-only hypothesis. Branching fraction values larger than 1.7×10−61.7\times 10^{-6} for the B0→J/ÏˆÎłB^{0}\to J/\psi\gamma decay mode are excluded at 90% confidence level. For the Bs0→J/ÏˆÎłB^{0}_{s}\to J/\psi\gamma decay mode, branching fraction values larger than 7.4×10−67.4\times 10^{-6} are excluded at 90% confidence level, this is the first branching fraction limit for this decay.Comment: All figures and tables, along with any supplementary material and additional information, are available at https://lhcbproject.web.cern.ch/lhcbproject/Publications/LHCbProjectPublic/LHCb-PAPER-2015-044.htm

    Les droits disciplinaires des fonctions publiques : « unification », « harmonisation » ou « distanciation ». A propos de la loi du 26 avril 2016 relative à la déontologie et aux droits et obligations des fonctionnaires

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    The production of tt‟ , W+bb‟ and W+cc‟ is studied in the forward region of proton–proton collisions collected at a centre-of-mass energy of 8 TeV by the LHCb experiment, corresponding to an integrated luminosity of 1.98±0.02 fb−1 . The W bosons are reconstructed in the decays W→ℓΜ , where ℓ denotes muon or electron, while the b and c quarks are reconstructed as jets. All measured cross-sections are in agreement with next-to-leading-order Standard Model predictions.The production of tt‟t\overline{t}, W+bb‟W+b\overline{b} and W+cc‟W+c\overline{c} is studied in the forward region of proton-proton collisions collected at a centre-of-mass energy of 8 TeV by the LHCb experiment, corresponding to an integrated luminosity of 1.98 ±\pm 0.02 \mbox{fb}^{-1}. The WW bosons are reconstructed in the decays W→ℓΜW\rightarrow\ell\nu, where ℓ\ell denotes muon or electron, while the bb and cc quarks are reconstructed as jets. All measured cross-sections are in agreement with next-to-leading-order Standard Model predictions

    Physics case for an LHCb Upgrade II - Opportunities in flavour physics, and beyond, in the HL-LHC era

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    The LHCb Upgrade II will fully exploit the flavour-physics opportunities of the HL-LHC, and study additional physics topics that take advantage of the forward acceptance of the LHCb spectrometer. The LHCb Upgrade I will begin operation in 2020. Consolidation will occur, and modest enhancements of the Upgrade I detector will be installed, in Long Shutdown 3 of the LHC (2025) and these are discussed here. The main Upgrade II detector will be installed in long shutdown 4 of the LHC (2030) and will build on the strengths of the current LHCb experiment and the Upgrade I. It will operate at a luminosity up to 2×1034 cm−2s−1, ten times that of the Upgrade I detector. New detector components will improve the intrinsic performance of the experiment in certain key areas. An Expression Of Interest proposing Upgrade II was submitted in February 2017. The physics case for the Upgrade II is presented here in more depth. CP-violating phases will be measured with precisions unattainable at any other envisaged facility. The experiment will probe b → sl+l−and b → dl+l− transitions in both muon and electron decays in modes not accessible at Upgrade I. Minimal flavour violation will be tested with a precision measurement of the ratio of B(B0 → ÎŒ+Ό−)/B(Bs → ÎŒ+Ό−). Probing charm CP violation at the 10−5 level may result in its long sought discovery. Major advances in hadron spectroscopy will be possible, which will be powerful probes of low energy QCD. Upgrade II potentially will have the highest sensitivity of all the LHC experiments on the Higgs to charm-quark couplings. Generically, the new physics mass scale probed, for fixed couplings, will almost double compared with the pre-HL-LHC era; this extended reach for flavour physics is similar to that which would be achieved by the HE-LHC proposal for the energy frontier

    LHCb upgrade software and computing : technical design report

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    This document reports the Research and Development activities that are carried out in the software and computing domains in view of the upgrade of the LHCb experiment. The implementation of a full software trigger implies major changes in the core software framework, in the event data model, and in the reconstruction algorithms. The increase of the data volumes for both real and simulated datasets requires a corresponding scaling of the distributed computing infrastructure. An implementation plan in both domains is presented, together with a risk assessment analysis

    Multidifferential study of identified charged hadron distributions in ZZ-tagged jets in proton-proton collisions at s=\sqrt{s}=13 TeV

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    Jet fragmentation functions are measured for the first time in proton-proton collisions for charged pions, kaons, and protons within jets recoiling against a ZZ boson. The charged-hadron distributions are studied longitudinally and transversely to the jet direction for jets with transverse momentum 20 <pT<100< p_{\textrm{T}} < 100 GeV and in the pseudorapidity range 2.5<η<42.5 < \eta < 4. The data sample was collected with the LHCb experiment at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 1.64 fb−1^{-1}. Triple differential distributions as a function of the hadron longitudinal momentum fraction, hadron transverse momentum, and jet transverse momentum are also measured for the first time. This helps constrain transverse-momentum-dependent fragmentation functions. Differences in the shapes and magnitudes of the measured distributions for the different hadron species provide insights into the hadronization process for jets predominantly initiated by light quarks.Comment: All figures and tables, along with machine-readable versions and any supplementary material and additional information, are available at https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2022-013.html (LHCb public pages

    Study of the B−→Λc+Λˉc−K−B^{-} \to \Lambda_{c}^{+} \bar{\Lambda}_{c}^{-} K^{-} decay

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    The decay B−→Λc+Λˉc−K−B^{-} \to \Lambda_{c}^{+} \bar{\Lambda}_{c}^{-} K^{-} is studied in proton-proton collisions at a center-of-mass energy of s=13\sqrt{s}=13 TeV using data corresponding to an integrated luminosity of 5 fb−1\mathrm{fb}^{-1} collected by the LHCb experiment. In the Λc+K−\Lambda_{c}^+ K^{-} system, the Ξc(2930)0\Xi_{c}(2930)^{0} state observed at the BaBar and Belle experiments is resolved into two narrower states, Ξc(2923)0\Xi_{c}(2923)^{0} and Ξc(2939)0\Xi_{c}(2939)^{0}, whose masses and widths are measured to be m(Ξc(2923)0)=2924.5±0.4±1.1 MeV,m(Ξc(2939)0)=2938.5±0.9±2.3 MeV,Γ(Ξc(2923)0)=0004.8±0.9±1.5 MeV,Γ(Ξc(2939)0)=0011.0±1.9±7.5 MeV, m(\Xi_{c}(2923)^{0}) = 2924.5 \pm 0.4 \pm 1.1 \,\mathrm{MeV}, \\ m(\Xi_{c}(2939)^{0}) = 2938.5 \pm 0.9 \pm 2.3 \,\mathrm{MeV}, \\ \Gamma(\Xi_{c}(2923)^{0}) = \phantom{000}4.8 \pm 0.9 \pm 1.5 \,\mathrm{MeV},\\ \Gamma(\Xi_{c}(2939)^{0}) = \phantom{00}11.0 \pm 1.9 \pm 7.5 \,\mathrm{MeV}, where the first uncertainties are statistical and the second systematic. The results are consistent with a previous LHCb measurement using a prompt Λc+K−\Lambda_{c}^{+} K^{-} sample. Evidence of a new Ξc(2880)0\Xi_{c}(2880)^{0} state is found with a local significance of 3.8 σ3.8\,\sigma, whose mass and width are measured to be 2881.8±3.1±8.5 MeV2881.8 \pm 3.1 \pm 8.5\,\mathrm{MeV} and 12.4±5.3±5.8 MeV12.4 \pm 5.3 \pm 5.8 \,\mathrm{MeV}, respectively. In addition, evidence of a new decay mode Ξc(2790)0→Λc+K−\Xi_{c}(2790)^{0} \to \Lambda_{c}^{+} K^{-} is found with a significance of 3.7 σ3.7\,\sigma. The relative branching fraction of B−→Λc+Λˉc−K−B^{-} \to \Lambda_{c}^{+} \bar{\Lambda}_{c}^{-} K^{-} with respect to the B−→D+D−K−B^{-} \to D^{+} D^{-} K^{-} decay is measured to be 2.36±0.11±0.22±0.252.36 \pm 0.11 \pm 0.22 \pm 0.25, where the first uncertainty is statistical, the second systematic and the third originates from the branching fractions of charm hadron decays.Comment: All figures and tables, along with any supplementary material and additional information, are available at https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2022-028.html (LHCb public pages
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