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4101por Capriotti, Lorenzo“….\\ The second analysis is a sensitivity study for a test of lepton universality in semileptonic charm decays, aiming to measure the ratio of branching fractions $R^{\mu/e} = \frac{\mathcal{B}(\Dz\to\Km \mup \neum)}{\mathcal{B}(\Dz\to \Km \ep\neue)}$. …”
Publicado 2018
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4102por Jensen, Simon Vindbaek“…Finally, the thermal neutron distribution in the CERN High energy AcceleRator Mixed field (CHARM) facility is investigated in collaboration with a radiation protection team from Japan. …”
Publicado 2018
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4103por Dubla, Andrea“… The magnetic field induces a charge separation in this anisotropy. The charm quark is an ideal candidate to probe the properties of this magnetic field, because its formation time is comparable to the time at which the magnetic field is expected to attain its maximum. …”
Publicado 2019
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4104por Sekihata, Daiki“…In the intermediate-mass region (1.1 $< m_{\rm ee} <$ 2.8 GeV/$c^{2}$), the measurement of thermal dielectrons from the QGP is very challenging at the LHC due to the dominant contribution of correlated e$^{+}$e$^{-}$ pairs from semileptonic decays of charm and beauty hadrons. Finally, at very low pair transverse momenta initial photon annihilation and photonuclear processes, triggered by the coherent electromagnetic fields of the incoming nuclei, are expected to play a role in more peripheral collisions. …”
Publicado 2020
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4105por Cai, Mengke“…In particular, beauty quarks, being four times heavier than charm quarks, can be utilized to study the in-medium mass dependent energy loss. …”
Publicado 2020
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4106por Reynolds, Elliot“…First, a direct search is performed for Higgs boson decays to charm quarks. An upper limit is set at $110\times$ the SM expectation on $\sigma(ZH)\times\text{BR}(H\to cc)$. …”
Publicado 2020
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4107por Gauger, Erin Frances“…The results will be compared with previous measurements of heavy-flavor (charm and beauty) decay electrons and with theoretical predictions. …”
Publicado 2021
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4108por The ATLAS collaboration“…The search targets $H^{\pm}$ decays into a bottom and a charm quark, $H^{\pm} \rightarrow cb$. The analysis focuses on data enriched in top-quark pair production, where one top quark decays into a leptonically decaying $W$ boson and a bottom quark, and the other top quark decays into a charged Higgs boson and a bottom quark. …”
Publicado 2021
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4109por Arcangeletti, Chiara“…This thesis describes my work on the Higgs boson fiducial cross section measurements, both inclusively and differentially, performed with full Run 2 dataset, together with their interpretation in different theoretical frameworks: Pseudo-Observables and $\kappa$-framework to constrain the Yukawa coupling with the charm quark. The Higgs boson CP properties have been also tested, in particular in the VBF production mechanism, looking for possible CP-violation effects in the Higgs sector in an Effective Field Theory (EFT) framework.…”
Publicado 2021
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4110“…This suggests “regeneration” of J/Ψ mesons by formation via coalescence of independently produced charm and anticharm quarks.…”
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4111por Niccoli, F, Garion, C, Maletta, C, Cangialosi, C, Infantino, A, Danzeca, S, Chiggiato, P“…In this preliminary study, a few selected SMA-based prototype UHV chambers, have been exposed to a high-energy mixed particle field (up to ∼140 kGy of absorbed dose) at the CERN high-energy accelerator mixed-field (CHARM) facility. The results, in terms of post-irradiation measurements, have revealed that leak tightness and thermal dismounting are unaffected by irradiation…”
Publicado 2019
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4112por CMS Collaboration“…Final states with a same-sign lepton pair in association with a charm or up quark are considered. New Higgs bosons in the $200-1000~\mathrm{GeV}$ mass range are targeted in the search, for scenarios in which either $\mathrm{H}$ or $\mathrm{A}$ appear alone, or in which they coexist and interfere. …”
Publicado 2023
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4113por The ATLAS collaboration“…This paper presents a search for top-squark pair production in final states with a top quark, charm quark and missing transverse momentum using a dataset collected with the ATLAS detector during LHC Run 2, corresponding to an integrated luminosity of 139 fb$^{-1}$ at a centre-of-mass energy of $\sqrt{s} = 13$ TeV proton-proton collisions. …”
Publicado 2023
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4114“…The LHCb experiment is designed to study differences between particles and anti-particles as well as very rare decays in the beauty and charm sector at the LHC. The detector will be upgraded in 2019 in order to significantly increase its efficiency, by removing the first-level hardware trigger. …”
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4115por Azzi, P“…Discoveries kept confirming this pattern: quark charm in 1974, tau lepton in 1976 and the bound state of the quark b in 1977. …”
Publicado 2015
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4116por Bombonati, Carlo“…Moreover, using previous studies on the charm production measurement, it has been possible to estimate the sensitivity to the mass dependence of the partonic energy loss.…”
Publicado 2017
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4117por Gandini, Paolo“…The LHCb detector is a single-arm spectrometer at the LHC, optimised for beauty and charm flavour physics. As the angle γ is the least experimentally constrained parameter of the Unitary Triangle, its precise experimental determination can be used to test the validity of the Standard Model. …”
Publicado 2017
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4118por Cè, Marco, Gérardin, Antoine, von Hippel, Georg, Hudspith, Renwick J., Kuberski, Simon, Meyer, Harvey B., Miura, Kohtaroh, Mohler, Daniel, Ottnad, Konstantin, Paul Srijit, Risch, Andreas, San José, Teseo, Wittig, Hartmut“…Our result at the physical point is <math display="inline"><msubsup><mi>a</mi><mi>μ</mi><mi>win</mi></msubsup><mo>=</mo><mo stretchy="false">(</mo><mn>237.30</mn><mo>±</mo><mn>0.7</mn><msub><mn>9</mn><mrow><mi>stat</mi></mrow></msub><mo>±</mo><mn>1.2</mn><msub><mn>2</mn><mrow><mi>syst</mi></mrow></msub><mo stretchy="false">)</mo><mo>×</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>10</mn></mrow></msup></math>, where the systematic error includes an estimate of the uncertainty due to the quenched charm quark in our calculation. Our result displays a tension of <math display="inline"><mrow><mn>3.9</mn><mi>σ</mi></mrow></math> with a recent evaluation of <math display="inline"><msubsup><mi>a</mi><mi>μ</mi><mi>win</mi></msubsup></math> based on the data-driven method.…”
Publicado 2022
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4119por LHCb Collaboration“…The relative branching fraction of $B^{-} \to \Lambda_{c}^{+} \bar{\Lambda}_{c}^{-} K^{-}$ with respect to the $B^{-} \to D^{+} D^{-} K^{-}$ decay is measured to be $2.36 \pm 0.11 \pm 0.22 \pm 0.25$, where the first uncertainty is statistical, the second systematic and the third originates from the branching fractions of charm hadron decays.…”
Publicado 2022
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4120por van Leeuwen, M., Afanasiev, S.V., Anticic, T., Baatar, B., Barna, D., Bartke, J., Barton, R.A., Behler, M., Betev, L., Białkowska, H., Billmeier, A., Blume, C., Blyth, C.O., Boimska, B., Botje, M., Bracinik, J., Bramm, R., Brun, R., Buncˇić, P., Cerny, V., Chvala, O., Cramer, J.G., Csató, P., Dinkelaker, P., Eckardt, V., Filip, P., Fischer, H.G., Fodor, Z., Foka, P., Freund, P., Friese, V., Gál, J., Gaździcki, M., Georgopoulos, G., Gładysz, E., Hegyi, S., Höhne, C., Igo, G., Jones, P.G., Kadija, K., Karev, A., Kolesnikov, V.I., Kollegger, T., Kowalski, M., Kraus, I., Kreps, M., Lévai, P., Malakhov, A.I., Margetis, S., Market, C., Mayes, B.W., Melkumov, G.L., Meurer, C., Mischke, A., Mitrovski, M., Molnár, J., Nelson, J.M., Pálla, G., Panagiotou, A.D., Perl, K., Petridis, A., Pikna, M., Pinsky, L., Pühlhofer, F., Reid, J.G., Renfordt, R., Retyk, W., Roland, C., Roland, G., Rybicki, A., Sammer, T., Sandoval, A., Sann, H., Schmitz, N., Seyboth, P., Siklér, F., Sitar, B., Skrzypczak, E., Squier, G.T.A., Stock, R., Ströbele, H., Susa, T., Szentpétery, I., Sziklai, J., Trainor, T.A., Varga, D., Vassiliou, M., Veres, G.I., Vesztergombi, G., Vranić, D., Wenig, S., Wetzler, A., Whitten, C., Yoo, I.K., Zaranek, J., Zimányi, J.“…This maximum could indicate the formation of deconfined matter at energies above 40 $A$GeV. A search for open charm in a large sample of 158 $A$GeV events is presented. …”
Publicado 2002
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