305 research outputs found

    Time and Meaning in Alfred SchĂŒtz

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    The essay analyses some aspects of the relationship between time and experience in Alfred SchĂŒtz. The first part highlights the role of time in the construction of the significant lived experience and of the subject's identity. It shows how the temporal structure determines the uniqueness of meaning: the latter is a function of lived-through time, of each individual's life-story. The structure of temporality seems to condemn the lived present to being excluded from the possibility of possessing meaning. In fact, the present is the privileged time frame for the construction of fundamental reality, of action, and of identity. The second part of the study investigates the ways in which time contributes to the constitution of sociality. The essay concludes by examining the main limitations of SchĂŒtz's theory

    La intersubjetividad y la esfera “emocional-afectiva”. Apuntes para una relectura del análisis constitutivo

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    In the first part of the essay are highlighted the assumption, in classical sociology, of emotion and rationality as opposing elements, and the presence of the fundamental aspects of the overcoming of such dichotomous view. The second part draws on Schutz’ thought on intersubjectivity as a social basic category. Although Schutz adopts a cognitive perspective, the essay underlines elements in his thought that allow to propose a new conceptualization in which the affective-emotional dimension is present ‘since the beginning

    Schutz, Berger and Luckmann.The question of the natural attitude

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    The purpose of this paper is to highlight different interpretations of the fundamental characteristics of the natural attitude, as formulated by Berger and Luckmann, and Alfred Schutz respectively. The first part of the paper explores the notion of taken-for-granted in the everyday life-world in The Social Construction of Reality by Berger and Luckmann and The Problem of Multiple Realities: Alfred Schutz and Robert Musil by Berger. The two essays show the presence of a articulated vision based on the same theoretical matrix. The second part of the paper analyses the essential characteristics of the natural attitude in the work of Husserl and Schutz. Although Berger and Luckmann are commonly viewed as being Schutzian scholars, their work actually presents significant differences, not only with respect to Husserl, but also to Schutz himself

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    Time, intersubjectivity, and musical relationship in Alfred Schutz

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    In questo lavoro, affronto alcuni aspetti della relazione tra tempo e intersoggettività in Alfred Schutz . Presento una sintesi dell’architettura metodologica del sociologo austriaco, delineando la specificità della relazione tra tempo e coscienza. Prendo in esame la trattazione dell’esperienza musicale come esempio di declinazione peculiare di una serie di dinamiche temporali connesse alla costituzione intersoggettiva dei significati. Infine, espongo alcune tesi di autori che si sono occupati della relazione tra tempo, intersoggettività e musica in Schutz. La relazione musicale ù un esempio di contesto dotato di senso, non oggetto di concettualizzazione, che esemplifica la relazione tra senso soggettivo ed esperienza dell’altro. La teoria dell’appresentazione di Schutz ù il centro del processo di costituzione dei significati della prensione dell’altro. L’emersione dei significati ù legata alle dinamiche dei poli passivi e attivi della coscienza e alla costituzione, nella we-relation, di una dimensione radicalmente intersoggettiva nella quale si supera la distinzione cartesiana tra interno ed esterno.Time, intersubjectivity, and musical relationship in Alfred Schutz Riccardo Venturini In this work I tackle certain aspects of the relationship between time and intersubjectivity in Alfred Schutz. I present a summary of the methodological architecture of the Austrian sociologist, outlining the specificity of the relationship between time and consciousness. I discuss the treatment of the musical experience as an example of the peculiar declination of a series of temporal dynamics connected to the intersubjective creation of meanings. Finally, I set out some thoughts related to the debate on the relationship between time, intersubjectivity and music in Schutz. The musical relationship is a context endowed with meaning, not the object of conceptualization, that allows us to identify in a paradigmatic way the relationship between the subjective sense and experience of the other. The theory of appresentation of Schutz is the center of the process of constitution of meaning of the understanding of the other. The emergence of meaning is related to the dynamics of the passive and active poles of the consciousness and the constitution, in the we-relation, of a radically intersubjective dimension that exceeds the Cartesian distinction between inside and outside

    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

    Measurement of the ratios of branching fractions R(D∗)\mathcal{R}(D^{*}) and R(D0)\mathcal{R}(D^{0})

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    The ratios of branching fractions R(D∗)≡B(Bˉ→D∗τ−Μˉτ)/B(Bˉ→D∗Ό−ΜˉΌ)\mathcal{R}(D^{*})\equiv\mathcal{B}(\bar{B}\to D^{*}\tau^{-}\bar{\nu}_{\tau})/\mathcal{B}(\bar{B}\to D^{*}\mu^{-}\bar{\nu}_{\mu}) and R(D0)≡B(B−→D0τ−Μˉτ)/B(B−→D0Ό−ΜˉΌ)\mathcal{R}(D^{0})\equiv\mathcal{B}(B^{-}\to D^{0}\tau^{-}\bar{\nu}_{\tau})/\mathcal{B}(B^{-}\to D^{0}\mu^{-}\bar{\nu}_{\mu}) are measured, assuming isospin symmetry, using a sample of proton-proton collision data corresponding to 3.0 fb−1{ }^{-1} of integrated luminosity recorded by the LHCb experiment during 2011 and 2012. The tau lepton is identified in the decay mode τ−→Ό−ΜτΜˉΌ\tau^{-}\to\mu^{-}\nu_{\tau}\bar{\nu}_{\mu}. The measured values are R(D∗)=0.281±0.018±0.024\mathcal{R}(D^{*})=0.281\pm0.018\pm0.024 and R(D0)=0.441±0.060±0.066\mathcal{R}(D^{0})=0.441\pm0.060\pm0.066, where the first uncertainty is statistical and the second is systematic. The correlation between these measurements is ρ=−0.43\rho=-0.43. Results are consistent with the current average of these quantities and are at a combined 1.9 standard deviations from the predictions based on lepton flavor universality in the Standard Model.Comment: All figures and tables, along with any supplementary material and additional information, are available at https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2022-039.html (LHCb public pages
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