607 research outputs found

    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

    Simulation de diffusion de l’hydrogĂšne dans les polycrystaux cfc : effet de la dĂ©formation et des joints de grains

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    In the present work, we establish a one-way coupled crystal plasticity – hydrogen diffusion analysis and use this approach to study the hydrogen transport in artificial polycrystalline aggregates of 316L steel with different grain geometries and crystallographic orientation. The data about stress/strain fields computed at the microstructure scaleutilizing the crystal plasticity concept are transferred to the in-house diffusion code which was developed using a new numerical scheme for solving parabolic equations. In the case of initial uniform hydrogen content, the heterogeneity of the mechanical fields is shownto induce a redistribution of hydrogen in the microstructure. The effect of strain rate is clearly revealed. In the second part, hydrogen transport across grain boundaries is investigatedconsidering the specific diffusivity and segregation properties of these interfaces. Using a discrete atomic layer model, the retarding impact of grain boundaries is demonstrated on bicrystals and bamboo type membranes with and without external mechanical loading. To reproduce the effects observed in the atomistic simulations into the crystal plasticity – hydrogen diffusion model, a new physically based multi-scale method is proposed. Using this new approach we study the effect of grain boundary trapping kinetics on hydrogen diffusion and reveal a new grain boundary diffusion regime which has notbeen reported before.Une approche couplĂ©e prenant en compte l’interaction de la plasticitĂ© cristalline et de la diffusion d’hydrogĂšne a Ă©tĂ© Ă©tablie et utilisĂ©e pour Ă©tudier le transport de l’hydrogĂšne dans les agrĂ©gats polycristallins synthĂ©tiques de l’acier 316L avec des gĂ©omĂ©tries de grains and des orientations cristallographiques diffĂ©rentes. Les champs mĂ©caniques calculĂ©s Ă  l’aide du code ZeBuLoN sont transfĂ©rĂ©s dans un code de diffusion dĂ©veloppĂ© dans le cadre de ce travail. Une nouvelle formulation associĂ©e Ă  un nouveau schĂ©ma numĂ©rique permet un calcul qui prĂ©sente une bonne convergence. Les rĂ©sultats des simulations montrent la redistribution de l’hydrogĂšne dans les polycristaux due Ă  la prĂ©sence des hĂ©tĂ©rogĂ©nĂ©itĂ©s des contraintes hydrostatiques Ă  l’échelle intragranulaire. L’effet de la vitesse de dĂ©formation a Ă©tĂ© quantitativement obtenu. Afin d’enrichir l’approche continue, un intĂ©rĂȘt particulier est portĂ© sur le rĂŽle des joints de grains. Des simulations numĂ©riques d’un modĂšle atomique plan par plan ont Ă©tĂ© dĂ©veloppĂ©es et appliquĂ©es aux bicristaux et aux structures de type ”bambou”. Les effets de puits ou de barriĂšre induits par la prĂ©sence des joints de grains sont clairement dĂ©montrĂ©s dans le cas du nickel pur. Pour reproduire ces effets dans les simulations de diffusion avec le modĂšle continue, une approche originale de simulation”multi-Ă©chelles” de la diffusion au joint de grain a Ă©tĂ© dĂ©veloppĂ©e, et un nouveau rĂ©gime de diffusion au joint de grain a Ă©tĂ© modĂ©lisĂ©

    Simulation of hydrogen diffusion in fcc polycrystals. Effect of deformation and grain boundaries : effect of deformation and grain boundaries

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    Une approche couplĂ©e prenant en compte l’interaction de la plasticitĂ© cristalline et de la diffusion d’hydrogĂšne a Ă©tĂ© Ă©tablie et utilisĂ©e pour Ă©tudier le transport de l’hydrogĂšne dans les agrĂ©gats polycristallins synthĂ©tiques de l’acier 316L avec des gĂ©omĂ©tries de grains and des orientations cristallographiques diffĂ©rentes. Les champs mĂ©caniques calculĂ©s Ă  l’aide du code ZeBuLoN sont transfĂ©rĂ©s dans un code de diffusion dĂ©veloppĂ© dans le cadre de ce travail. Une nouvelle formulation associĂ©e Ă  un nouveau schĂ©ma numĂ©rique permet un calcul qui prĂ©sente une bonne convergence. Les rĂ©sultats des simulations montrent la redistribution de l’hydrogĂšne dans les polycristaux due Ă  la prĂ©sence des hĂ©tĂ©rogĂ©nĂ©itĂ©s des contraintes hydrostatiques Ă  l’échelle intragranulaire. L’effet de la vitesse de dĂ©formation a Ă©tĂ© quantitativement obtenu. Afin d’enrichir l’approche continue, un intĂ©rĂȘt particulier est portĂ© sur le rĂŽle des joints de grains. Des simulations numĂ©riques d’un modĂšle atomique plan par plan ont Ă©tĂ© dĂ©veloppĂ©es et appliquĂ©es aux bicristaux et aux structures de type ”bambou”. Les effets de puits ou de barriĂšre induits par la prĂ©sence des joints de grains sont clairement dĂ©montrĂ©s dans le cas du nickel pur. Pour reproduire ces effets dans les simulations de diffusion avec le modĂšle continue, une approche originale de simulation”multi-Ă©chelles” de la diffusion au joint de grain a Ă©tĂ© dĂ©veloppĂ©e, et un nouveau rĂ©gime de diffusion au joint de grain a Ă©tĂ© modĂ©lisĂ©.In the present work, we establish a one-way coupled crystal plasticity – hydrogen diffusion analysis and use this approach to study the hydrogen transport in artificial polycrystalline aggregates of 316L steel with different grain geometries and crystallographic orientation. The data about stress/strain fields computed at the microstructure scaleutilizing the crystal plasticity concept are transferred to the in-house diffusion code which was developed using a new numerical scheme for solving parabolic equations. In the case of initial uniform hydrogen content, the heterogeneity of the mechanical fields is shownto induce a redistribution of hydrogen in the microstructure. The effect of strain rate is clearly revealed. In the second part, hydrogen transport across grain boundaries is investigatedconsidering the specific diffusivity and segregation properties of these interfaces. Using a discrete atomic layer model, the retarding impact of grain boundaries is demonstrated on bicrystals and bamboo type membranes with and without external mechanical loading. To reproduce the effects observed in the atomistic simulations into the crystal plasticity – hydrogen diffusion model, a new physically based multi-scale method is proposed. Using this new approach we study the effect of grain boundary trapping kinetics on hydrogen diffusion and reveal a new grain boundary diffusion regime which has notbeen reported before

    A new algorithm for dense ellipse packing and polygonal structures generation in context of FEM or DEM

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    International audienceA new constructive ellipse packing algorithm is presented. It allows to respect the imposed area, shape and spatial orientation distribution (i.e. the inertia tensor) and achieve high packing densities. The packing density decreases with increasing particles aspect ratio what is in agreement with results reported in the literature. The generated packings with complex imposed area, shape and spatial orientation distributions with densities in the range of 0.74 and 0.8 are presented. The efficiency of the algorithm is demonstrated by comparison with the Optimized Dropping and Rolling method for disk packing. Moreover, the proposed packing strategy enables to generate very easily non-equiaxed polygonal structures by using Laguerre-VoronoĂŻ tessellation of the generated disk-based ellipse packing

    Advancing layer algorithm of dense ellipse packing for generating statistically equivalent polygonal structures

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    International audienceA new constructive algorithm, called Advancing layer algorithm, for the generation of dense ellipse packing is proposed. Compared to existing algorithms for filling a 2D domain by elliptical particles, the method allows to respect the imposed size, shape and spatial orientation distributions (i.e. the inertia tensor) and achieve high packing densities. In particular case of disk packing, the comparison with Optimized Dropping and Rolling method shows that the computational cost of the proposed methodology is lower for moderate polydispersities of particle size while achieving higher packing densities and more homogeneous placing of particles in the domain. Thanks to an approximation of each ellipse by a set of circles, polygonal structures are constructed on the base of obtained ellipse packing by Laguerre–Voronoï Tessellation method in good agreement with desired characteristics of cells (polygons)

    A new algorithm for dense ellipse packing and polygonal structures generation in context of FEM or DEM

    No full text
    International audienceA new constructive ellipse packing algorithm is presented. It allows to respect the imposed area, shape and spatial orientation distribution (i.e. the inertia tensor) and achieve high packing densities. The packing density decreases with increasing particles aspect ratio what is in agreement with results reported in the literature. The generated packings with complex imposed area, shape and spatial orientation distributions with densities in the range of 0.74 and 0.8 are presented. The efficiency of the algorithm is demonstrated by comparison with the Optimized Dropping and Rolling method for disk packing. Moreover, the proposed packing strategy enables to generate very easily non-equiaxed polygonal structures by using Laguerre-VoronoĂŻ tessellation of the generated disk-based ellipse packing

    A new algorithm for dense ellipse packing and polygonal structures generation in context of FEM or DEM

    No full text
    A new constructive ellipse packing algorithm is presented. It allows to respect the imposed area, shape and spatial orientation distribution (i.e. the inertia tensor) and achieve high packing densities. The packing density decreases with increasing particles aspect ratio what is in agreement with results reported in the literature. The generated packings with complex imposed area, shape and spatial orientation distributions with densities in the range of 0.74 and 0.8 are presented. The efficiency of the algorithm is demonstrated by comparison with the Optimized Dropping and Rolling method for disk packing. Moreover, the proposed packing strategy enables to generate very easily non-equiaxed polygonal structures by using Laguerre-VoronoĂŻ tessellation of the generated disk-based ellipse packing

    Corporate innovation ecosystems: challenges and opportunities

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    This article proposes to consider the concepts of an innovation ecosystem and a digital platform. The analysis of world experience in terms of corporate innovative ecosystems contributing to the accelerated implementation of innovations is presented. The article focuses on corporate innovation ecosystems, gives their definition and key functions. The analysis of the management of innovative ecosystems in the world and in Russia is given. Describes the ecosystem approach and the structure of the corporate innovation ecosystem. As part of the study, it is planned to form a scheme for organizing a corporate innovation ecosystem, considering the place of digital platforms in the entire ecosystem
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