360 research outputs found

    Study of J /ψ production in Jets

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    The production of J/ψ mesons in jets is studied in the forward region of proton-proton collisions using data collected with the LHCb detector at a center-of-mass energy of 13 TeV. The fraction of the jet transverse momentum carried by the J/ψ meson, z(J/ψ)≡pT(J/ψ)/pT(jet), is measured using jets with pT(jet)>20 GeV in the pseudorapidity range 2.5<η(jet)<4.0. The observed z(J/ψ)distribution for J/ψ mesons produced in b-hadron decays is consistent with expectations. However, the results for prompt J/ψ production do not agree with predictions based on fixed-order nonrelativistic QCD. This is the first measurement of the pT fraction carried by prompt J/ψ mesons in jets at any experiment

    Bose-Einstein correlations of same-sign charged pions in the forward region in pp collisions at √s=7 TeV

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    Bose-Einstein correlations of same-sign charged pions, produced in protonproton collisions at a 7 TeV centre-of-mass energy, are studied using a data sample collected by the LHCb experiment. The signature for Bose-Einstein correlations is observed in the form of an enhancement of pairs of like-sign charged pions with small four-momentum difference squared. The charged-particle multiplicity dependence of the Bose-Einstein correlation parameters describing the correlation strength and the size of the emitting source is investigated, determining both the correlation radius and the chaoticity parameter. The measured correlation radius is found to increase as a function of increasing charged-particle multiplicity, while the chaoticity parameter is seen to decreas

    Study of charmonium production in b -hadron decays and first evidence for the decay Bs0

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    Using decays to φ-meson pairs, the inclusive production of charmonium states in b-hadron decays is studied with pp collision data corresponding to an integrated luminosity of 3.0 fb−1, collected by the LHCb experiment at centre-of-mass energies of 7 and 8 TeV. Denoting byBC ≡ B(b → C X) × B(C → φφ) the inclusive branching fraction of a b hadron to a charmonium state C that decays into a pair of φ mesons, ratios RC1C2 ≡ BC1 /BC2 are determined as Rχc0ηc(1S) = 0.147 ± 0.023 ± 0.011, Rχc1ηc(1S) =0.073 ± 0.016 ± 0.006, Rχc2ηc(1S) = 0.081 ± 0.013 ± 0.005,Rχc1 χc0 = 0.50 ± 0.11 ± 0.01, Rχc2 χc0 = 0.56 ± 0.10 ± 0.01and Rηc(2S)ηc(1S) = 0.040 ± 0.011 ± 0.004. Here and below the first uncertainties are statistical and the second systematic.Upper limits at 90% confidence level for the inclusive production of X(3872), X(3915) and χc2(2P) states are obtained as RX(3872)χc1 < 0.34, RX(3915)χc0 < 0.12 andRχc2(2P)χc2 < 0.16. Differential cross-sections as a function of transverse momentum are measured for the ηc(1S) andχc states. The branching fraction of the decay B0s → φφφ is measured for the first time, B(B0s → φφφ) = (2.15±0.54±0.28±0.21B)×10−6. Here the third uncertainty is due to the branching fraction of the decay B0s → φφ, which is used for normalization. No evidence for intermediate resonances is seen. A preferentially transverse φ polarization is observed.The measurements allow the determination of the ratio of the branching fractions for the ηc(1S) decays to φφ and p p asB(ηc(1S)→ φφ)/B(ηc(1S)→ p p) = 1.79 ± 0.14 ± 0.32

    Measurement of the inelastic pp cross-section at a centre-of-mass energy of 13TeV

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    The cross-section for inelastic proton-proton collisions at a centre-of-mass energy of 13TeV is measured with the LHCb detector. The fiducial cross-section for inelastic interactions producing at least one prompt long-lived charged particle with momentum p &gt; 2 GeV/c in the pseudorapidity range 2 &lt; η &lt; 5 is determined to be ϭ acc = 62:2 ± 0:2 ± 2:5mb. The first uncertainty is the intrinsic systematic uncertainty of the measurement, the second is due to the uncertainty on the integrated luminosity. The statistical uncertainty is negligible. Extrapolation to full phase space yields the total inelastic proton-proton cross-section ϭ inel = 75:4 ± 3:0 ± 4:5mb, where the first uncertainty is experimental and the second due to the extrapolation. An updated value of the inelastic cross-section at a centre-of-mass energy of 7TeV is also reported

    ĐĐ”ŃĐżĐ”Ń†ĐžŃ„ĐžŃ‡Đ”ŃĐșОД ĐżŃ€ĐžĐŒĐ”ŃĐž ĐČ Ń„Đ°Ń€ĐŒĐ°Ń†Đ”ĐČтОчДсĐșох ŃŃƒĐ±ŃŃ‚Đ°ĐœŃ†ĐžŃŃ…: ĐŸŃĐŸĐ±Đ”ĐœĐœĐŸŃŃ‚Đž ĐŒĐ”Ń‚ĐŸĐŽĐžĐș ох ĐŸĐżŃ€Đ”ĐŽĐ”Đ»Đ”ĐœĐžŃ

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    One of the prerequisites of efficacy and safety of finished pharmaceutical products is the quality of pharmaceutical substances used in their production. Criteria of assessment of pharmaceutical substance purity are determined by the substance composition and production technology, as well as by specific aspects of the finished pharmaceutical product production and use. It is necessary to control the content of nonspecific organic and inorganic impurities, impurities of microbial origin, and residual solvents. The aim of the study was to analyse characteristics of test methods used to determine nonspecific impurities in pharmaceutical substances. The State Pharmacopoeia of the Russian Federation describes various chemical, physical, physicochemical and biological tests for the analysis of nonspecific impurities. Determination of inorganic cations and anions usually includes comparison of test solutions with solutions of the corresponding reference standards, or checking the absence of a positive reaction in the test solution. Quantitative analysis of trace impurities largely relies on highly specific and sensitive test methods, such as atomic absorption spectrometry, atomic emission spectrometry and inductively coupled plasma mass spectrometry. The content of residual organic solvents is determined by gas chromatography or high-performance liquid chromatography. The purity and safety of pharmaceutical substances are ensured by biological tests: “Microbial quality”, “Sterility”, “Pyrogenicity”, “Bacterial endotoxins”. Specific characteristics of test methods used for determination of the content of nonspecific impurities in various pharmaceutical substances depend on physicochemical properties of the tested substances, toxicity of the analysed impurities, and content limits. The results of the study make it possible to formulate a methodological approach to the development of criteria for assessing the quality of pharmaceutical substances. This approach includes mandatory compliance with the basic principles of substance standardisation, as well as case-by-case selection of quality parameters, specific test conditions and content limits for impurities.ĐžĐŽĐœĐžĐŒ Оз фаĐșŃ‚ĐŸŃ€ĐŸĐČ ŃŃ„Ń„Đ”ĐșтоĐČĐœĐŸŃŃ‚Đž Đž Đ±Đ”Đ·ĐŸĐżĐ°ŃĐœĐŸŃŃ‚Đž ĐłĐŸŃ‚ĐŸĐČых лДĐșарстĐČĐ”ĐœĐœŃ‹Ń… срДЎстĐČ ŃĐČĐ»ŃĐ”Ń‚ŃŃ ĐșачДстĐČĐŸ ĐžŃĐżĐŸĐ»ŃŒĐ·ŃƒĐ”ĐŒŃ‹Ń… Ń„Đ°Ń€ĐŒĐ°Ń†Đ”ĐČтОчДсĐșох ŃŃƒĐ±ŃŃ‚Đ°ĐœŃ†ĐžĐč, ĐșрОтДрОО ĐŸŃ†Đ”ĐœĐșĐž Ń‡ĐžŃŃ‚ĐŸŃ‚Ń‹ ĐșĐŸŃ‚ĐŸŃ€Ń‹Ń… ĐŸĐ±ŃƒŃĐ»ĐŸĐČĐ»Đ”ĐœŃ‹ ох ŃĐŸŃŃ‚Đ°ĐČĐŸĐŒ Đž Ń‚Đ”Ń…ĐœĐŸĐ»ĐŸĐłĐžĐ”Đč ĐżĐŸĐ»ŃƒŃ‡Đ”ĐœĐžŃ, Đ° таĐșжД ĐŸŃĐŸĐ±Đ”ĐœĐœĐŸŃŃ‚ŃĐŒĐž ĐżŃ€ĐŸĐžĐ·ĐČĐŸĐŽŃŃ‚ĐČĐ° Đž ĐżŃ€ĐžĐŒĐ”ĐœĐ”ĐœĐžŃ лДĐșарстĐČĐ”ĐœĐœŃ‹Ń… ĐżŃ€Đ”ĐżĐ°Ń€Đ°Ń‚ĐŸĐČ. ĐžĐ±ŃĐ·Đ°Ń‚Đ”Đ»ŃŒĐœĐŸĐŒŃƒ ĐœĐŸŃ€ĐŒĐžŃ€ĐŸĐČĐ°ĐœĐžŃŽ ĐżĐŸĐŽĐ»Đ”Đ¶Đ°Ń‚ ĐœĐ”ŃĐżĐ”Ń†ĐžŃ„ĐžŃ‡Đ”ŃĐșОД ĐżŃ€ĐžĐŒĐ”ŃĐž ĐŸŃ€ĐłĐ°ĐœĐžŃ‡Đ”ŃĐșĐŸĐč Đž ĐœĐ”ĐŸŃ€ĐłĐ°ĐœĐžŃ‡Đ”ŃĐșĐŸĐč ĐżŃ€ĐžŃ€ĐŸĐŽŃ‹, ĐŒĐžĐșŃ€ĐŸĐ±ĐœĐŸĐłĐŸ ĐżŃ€ĐŸĐžŃŃ…ĐŸĐ¶ĐŽĐ”ĐœĐžŃ, ĐŸŃŃ‚Đ°Ń‚ĐŸŃ‡ĐœŃ‹Đ” растĐČĐŸŃ€ĐžŃ‚Đ”Đ»Đž. ĐŠĐ”Đ»ŃŒ Ń€Đ°Đ±ĐŸŃ‚Ń‹ — Đ°ĐœĐ°Đ»ĐžĐ· ĐŸŃĐŸĐ±Đ”ĐœĐœĐŸŃŃ‚Đ”Đč ĐŒĐ”Ń‚ĐŸĐŽĐžĐș ĐŸĐżŃ€Đ”ĐŽĐ”Đ»Đ”ĐœĐžŃ ĐœĐ”ŃĐżĐ”Ń†ĐžŃ„ĐžŃ‡Đ”ŃĐșох ĐżŃ€ĐžĐŒĐ”ŃĐ”Đč ĐČ Ń„Đ°Ń€ĐŒĐ°Ń†Đ”ĐČтОчДсĐșох ŃŃƒĐ±ŃŃ‚Đ°ĐœŃ†ĐžŃŃ…. Đ”Đ»Ń ĐŸŃ†Đ”ĐœĐșĐž ох ŃĐŸĐŽĐ”Ń€Đ¶Đ°ĐœĐžŃ Đ“ĐŸŃŃƒĐŽĐ°Ń€ŃŃ‚ĐČĐ”ĐœĐœĐ°Ń Ń„Đ°Ń€ĐŒĐ°ĐșĐŸĐżĐ”Ń Đ ĐŸŃŃĐžĐčсĐșĐŸĐč ЀДЎДрацОО ĐżŃ€Đ”ĐŽŃƒŃĐŒĐ°Ń‚Ń€ĐžĐČаДт ĐžŃĐżĐŸĐ»ŃŒĐ·ĐŸĐČĐ°ĐœĐžĐ” Ń€Đ°Đ·Đ»ĐžŃ‡ĐœŃ‹Ń… Ń…ĐžĐŒĐžŃ‡Đ”ŃĐșох, фОзОчДсĐșох, фОзОĐșĐŸ-Ń…ĐžĐŒĐžŃ‡Đ”ŃĐșох Đž Đ±ĐžĐŸĐ»ĐŸĐłĐžŃ‡Đ”ŃĐșох ĐŒĐ”Ń‚ĐŸĐŽĐŸĐČ Đ°ĐœĐ°Đ»ĐžĐ·Đ°. Про ĐŸĐżŃ€Đ”ĐŽĐ”Đ»Đ”ĐœĐžĐž ĐœĐ”ĐŸŃ€ĐłĐ°ĐœĐžŃ‡Đ”ŃĐșох ĐșĐ°Ń‚ĐžĐŸĐœĐŸĐČ Đž Đ°ĐœĐžĐŸĐœĐŸĐČ, ĐșĐ°Đș праĐČĐžĐ»ĐŸ, ĐżŃ€ĐŸĐČĐŸĐŽĐžŃ‚ŃŃ сраĐČĐœĐ”ĐœĐžĐ” с растĐČĐŸŃ€Đ°ĐŒĐž ŃĐŸĐŸŃ‚ĐČДтстĐČующох ŃŃ‚Đ°Đ»ĐŸĐœĐŸĐČ ĐžĐ»Đž фоĐșŃĐžŃ€ŃƒĐ”Ń‚ŃŃ ĐŸŃ‚ŃŃƒŃ‚ŃŃ‚ĐČОД ĐżĐŸĐ»ĐŸĐ¶ĐžŃ‚Đ”Đ»ŃŒĐœĐŸĐč рДаĐșцоо ĐČ ĐžŃĐżŃ‹Ń‚ŃƒĐ”ĐŒĐŸĐŒ растĐČĐŸŃ€Đ”. Đ”Đ»Ń ĐșĐŸĐ»ĐžŃ‡Đ”ŃŃ‚ĐČĐ”ĐœĐœĐŸĐłĐŸ Đ°ĐœĐ°Đ»ĐžĐ·Đ° ĐŒĐžĐșŃ€ĐŸĐżŃ€ĐžĐŒĐ”ŃĐ”Đč ĐŽĐŸŃŃ‚Đ°Ń‚ĐŸŃ‡ĐœĐŸ ŃˆĐžŃ€ĐŸĐșĐŸ ĐžŃĐżĐŸĐ»ŃŒĐ·ŃƒŃŽŃ‚ŃŃ ĐČŃ‹ŃĐŸĐșĐŸŃĐżĐ”Ń†ĐžŃ„ĐžŃ‡ĐœŃ‹Đ” Đž чуĐČстĐČĐžŃ‚Đ”Đ»ŃŒĐœŃ‹Đ” ĐŒĐ”Ń‚ĐŸĐŽŃ‹: Đ°Ń‚ĐŸĐŒĐœĐŸ-Đ°Đ±ŃĐŸŃ€Đ±Ń†ĐžĐŸĐœĐœĐ°Ń спДĐșŃ‚Ń€ĐŸĐŒĐ”Ń‚Ń€ĐžŃ, Đ°Ń‚ĐŸĐŒĐœĐŸ-ŃĐŒĐžŃŃĐžĐŸĐœĐœĐ°Ń Đž ĐŒĐ°ŃŃ-спДĐșŃ‚Ń€ĐŸĐŒĐ”Ń‚Ń€ĐžŃ с ĐžĐœĐŽŃƒĐșтоĐČĐœĐŸ сĐČŃĐ·Đ°ĐœĐœĐŸĐč ĐżĐ»Đ°Đ·ĐŒĐŸĐč. ĐĄĐŸĐŽĐ”Ń€Đ¶Đ°ĐœĐžĐ” ĐŸŃŃ‚Đ°Ń‚ĐŸŃ‡ĐœŃ‹Ń… ĐŸŃ€ĐłĐ°ĐœĐžŃ‡Đ”ŃĐșох растĐČĐŸŃ€ĐžŃ‚Đ”Đ»Đ”Đč ĐŸĐżŃ€Đ”ĐŽĐ”Đ»ŃĐ”Ń‚ŃŃ ĐŒĐ”Ń‚ĐŸĐŽĐ°ĐŒĐž ĐłĐ°Đ·ĐŸĐČĐŸĐč ОлО ĐČŃ‹ŃĐŸĐșĐŸŃŃ„Ń„Đ”ĐșтоĐČĐœĐŸĐč жОЎĐșĐŸŃŃ‚ĐœĐŸĐč Ń…Ń€ĐŸĐŒĐ°Ń‚ĐŸĐłŃ€Đ°Ń„ĐžĐž. Đ”Đ»Ń ĐŸŃ†Đ”ĐœĐșĐž Ń‡ĐžŃŃ‚ĐŸŃ‚Ń‹ Đž ĐŸĐ±Đ”ŃĐżĐ”Ń‡Đ”ĐœĐžŃ Đ±Đ”Đ·ĐŸĐżĐ°ŃĐœĐŸŃŃ‚Đž ĐżŃ€ĐžĐŒĐ”ĐœĐ”ĐœĐžŃ Ń„Đ°Ń€ĐŒĐ°Ń†Đ”ĐČтОчДсĐșох ŃŃƒĐ±ŃŃ‚Đ°ĐœŃ†ĐžĐč ĐžŃĐżĐŸĐ»ŃŒĐ·ŃƒŃŽŃ‚ŃŃ Đ±ĐžĐŸĐ»ĐŸĐłĐžŃ‡Đ”ŃĐșОД ĐžŃĐżŃ‹Ń‚Đ°ĐœĐžŃ: Â«ĐœĐžĐșŃ€ĐŸĐ±ĐžĐŸĐ»ĐŸĐłĐžŃ‡Đ”ŃĐșая Ń‡ĐžŃŃ‚ĐŸŃ‚Đ°Â», Â«ĐĄŃ‚Đ”Ń€ĐžĐ»ŃŒĐœĐŸŃŃ‚ŃŒÂ», Â«ĐŸĐžŃ€ĐŸĐłĐ”ĐœĐœĐŸŃŃ‚ŃŒÂ», «БаĐșŃ‚Đ”Ń€ĐžĐ°Đ»ŃŒĐœŃ‹Đ” ŃĐœĐŽĐŸŃ‚ĐŸĐșŃĐžĐœŃ‹Â». Đ˜ĐœĐŽĐžĐČĐžĐŽŃƒĐ°Đ»ŃŒĐœŃ‹Đ” ĐŸŃĐŸĐ±Đ”ĐœĐœĐŸŃŃ‚Đž ĐŒĐ”Ń‚ĐŸĐŽĐžĐș ĐżŃ€ĐŸĐČĐ”ĐŽĐ”ĐœĐžŃ ĐžŃĐżŃ‹Ń‚Đ°ĐœĐžĐč ĐœĐ° ŃĐŸĐŽĐ”Ń€Đ¶Đ°ĐœĐžĐ” ĐœĐ”ŃĐżĐ”Ń†ĐžŃ„ĐžŃ‡Đ”ŃĐșох ĐżŃ€ĐžĐŒĐ”ŃĐ”Đč ĐČ Ń€Đ°Đ·Đ»ĐžŃ‡ĐœŃ‹Ń… Ń„Đ°Ń€ĐŒĐ°Ń†Đ”ĐČтОчДсĐșох ŃŃƒĐ±ŃŃ‚Đ°ĐœŃ†ĐžŃŃ… ĐŸĐ±ŃƒŃĐ»ĐŸĐČĐ»Đ”ĐœŃ‹ фОзОĐșĐŸ-Ń…ĐžĐŒĐžŃ‡Đ”ŃĐșĐžĐŒĐž сĐČĐŸĐčстĐČĐ°ĐŒĐž ĐžŃŃĐ»Đ”ĐŽŃƒĐ”ĐŒŃ‹Ń… ŃĐŸĐ”ĐŽĐžĐœĐ”ĐœĐžĐč, Ń‚ĐŸĐșŃĐžŃ‡ĐœĐŸŃŃ‚ŃŒŃŽ Đ°ĐœĐ°Đ»ĐžĐ·ĐžŃ€ŃƒĐ”ĐŒŃ‹Ń… ĐżŃ€ĐžĐŒĐ”ŃĐ”Đč Đž ĐŽĐŸĐżŃƒŃŃ‚ĐžĐŒŃ‹ĐŒĐž ĐżŃ€Đ”ĐŽĐ”Đ»Đ°ĐŒĐž ох ŃĐŸĐŽĐ”Ń€Đ¶Đ°ĐœĐžŃ. Đ Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Ń‹ Ń€Đ°Đ±ĐŸŃ‚Ń‹ ĐżĐŸĐ·ĐČĐŸĐ»ŃŃŽŃ‚ ŃŃ„ĐŸŃ€ĐŒŃƒĐ»ĐžŃ€ĐŸĐČать ĐŒĐ”Ń‚ĐŸĐŽĐŸĐ»ĐŸĐłĐžŃ‡Đ”ŃĐșĐžĐč ĐżĐŸĐŽŃ…ĐŸĐŽ Đș Ń€Đ°Đ·Ń€Đ°Đ±ĐŸŃ‚ĐșĐ” ĐșрОтДрОДĐČ ĐŸŃ†Đ”ĐœĐșĐž ĐșачДстĐČĐ° Ń„Đ°Ń€ĐŒĐ°Ń†Đ”ĐČтОчДсĐșох ŃŃƒĐ±ŃŃ‚Đ°ĐœŃ†ĐžĐč, ŃĐŸŃ‡Đ”Ń‚Đ°ŃŽŃ‰ĐžĐč ĐŸĐ±ŃĐ·Đ°Ń‚Đ”Đ»ŃŒĐœĐŸĐ” ŃĐŸĐ±Đ»ŃŽĐŽĐ”ĐœĐžĐ” ĐŸŃĐœĐŸĐČĐœŃ‹Ń… ĐżŃ€ĐžĐœŃ†ĐžĐżĐŸĐČ ŃŃ‚Đ°ĐœĐŽĐ°Ń€Ń‚ĐžĐ·Đ°Ń†ĐžĐž ŃŃƒĐ±ŃŃ‚Đ°ĐœŃ†ĐžĐč, ĐžĐœĐŽĐžĐČĐžĐŽŃƒĐ°Đ»ŃŒĐœŃ‹Đč ĐČŃ‹Đ±ĐŸŃ€ ĐżĐŸĐșазатДлДĐč ĐșачДстĐČĐ°, ĐŸŃĐŸĐ±Ń‹Ń… ŃƒŃĐ»ĐŸĐČĐžĐč ĐżŃ€ĐŸĐČĐ”ĐŽĐ”ĐœĐžŃ ĐžŃĐżŃ‹Ń‚Đ°ĐœĐžĐč Đž ĐœĐŸŃ€ĐŒ ŃĐŸĐŽĐ”Ń€Đ¶Đ°ĐœĐžŃ ĐżŃ€ĐžĐŒĐ”ŃĐ”Đč

    Updated Determination of D⁰–D¯⁰Mixing and CP Violation Parameters with D⁰→Kâșπ⁻ Decays

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    We report measurements of charm-mixing parameters based on the decay-time-dependent ratio of D⁰→Kâșπ⁻ to D⁰→K⁻πâș rates. The analysis uses a data sample of proton-proton collisions corresponding to an integrated luminosity of 5.0  fb⁻Âč recorded by the LHCb experiment from 2011 through 2016. Assuming charge-parity (CP) symmetry, the mixing parameters are determined to be xâ€ČÂČ=(3.9±2.7)×10⁻⁔, yâ€Č=(5.28±0.52)×10⁻³, and R[subscript D]=(3.454±0.031)×10⁻³. Without this assumption, the measurement is performed separately for D⁰ and D[over ÂŻ]⁰ mesons, yielding a direct CP-violating asymmetry A[subscript D]=(-0.1±9.1)×10⁻³, and magnitude of the ratio of mixing parameters 1.00<|q/p|<1.35 at the 68.3% confidence level. All results include statistical and systematic uncertainties and improve significantly upon previous single-measurement determinations. No evidence for CP violation in charm mixing is observed

    Observation of D⁰ Meson Decays to Πâșπ⁻ΌâșΌ⁻ and KâșK⁻ΌâșΌ⁻ Final States

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    The first observation of the D⁰→πâșπ⁻ΌâșΌ⁻ and D⁰→KâșK⁻ΌâșΌ⁻ decays is reported using a sample of proton-proton collisions collected by LHCb at a center-of-mass energy of 8 TeV, and corresponding to 2  fb⁻Âč of integrated luminosity. The corresponding branching fractions are measured using as normalization the decay D⁰→K⁻πâș[ÎŒâșΌ⁻][subscript ρ⁰/ω], where the two muons are consistent with coming from the decay of a ρ⁰ or ω meson. The results are B(D⁰→πâșπ⁻ΌâșΌ⁻)=(9.64±0.48±0.51±0.97)×10⁻⁷ and B(D⁰→KâșK⁻ΌâșΌ⁻)=(1.54±0.27±0.09±0.16)×10⁻⁷, where the uncertainties are statistical, systematic, and due to the limited knowledge of the normalization branching fraction. The dependence of the branching fraction on the dimuon mass is also investigated

    Study of J=ψ Production in Jets

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    The production of J/ψ mesons in jets is studied in the forward region of proton-proton collisions using data collected with the LHCb detector at a center-of-mass energy of 13 TeV. The fraction of the jet transverse momentum carried by the J/ψ meson, z(J/ψ)≡p[subscript T](J/ψ)/p[subscript T](jet), is measured using jets with p[subscript T](jet) > 20  GeV in the pseudorapidity range 2.5<η(jet)<4.0. The observed z(J/ψ) distribution for J/ψ mesons produced in b-hadron decays is consistent with expectations. However, the results for prompt J/ψ production do not agree with predictions based on fixed-order nonrelativistic QCD. This is the first measurement of the p[subscript T] fraction carried by prompt J/ψ mesons in jets at any experiment.National Science Foundation (U.S.

    Search for long-lived scalar particles in B + → K + χ ( ÎŒ + ÎŒ − ) decays

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    A search for a long-lived scalar particle χ is performed, looking for the decay B[superscript +]→K[superscript +]χ with χ→Ό[superscript +]ÎŒ[superscript -] in pp collision data corresponding to an integrated luminosity of 3  fb[superscript -1], collected by the LHCb experiment at center-of-mass energies of √s =7 and 8 TeV. This new scalar particle, predicted by hidden sector models, is assumed to have a narrow width. The signal would manifest itself as an excess in the dimuon invariant mass distribution over the Standard Model background. No significant excess is observed in the accessible ranges of mass 250<m(χ)<4700  MeV/c[superscript 2] and lifetime 0.1<τ(χ)<1000  ps. Upper limits on the branching fraction B(B[superscript +]→K[superscript +]χ(ÎŒ[superscript +]ÎŒ[superscript -])) at 95% confidence level are set as a function of m(χ) and τ(χ), varying between 2×10[superscript -10] and 10[superscript -7]. These are the most stringent limits to date. The limits are interpreted in the context of a model with a light inflaton particle.National Science Foundation (U.S.

    Prompt and nonprompt J/ψ production and nuclear modification in pPb collisions at s<sub>NN</sub>=8.16 TeV

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    The production of J/ψ mesons is studied in proton-lead collisions at the centre-of-mass energy per nucleon pair sNN=8.16 TeV with the LHCb detector at the LHC. The double differential cross-sections of prompt and nonprompt J/ψ production are measured as a function of the J/ψ transverse momentum and rapidity in the nucleon–nucleon centre-of-mass frame. Forward-to-backward ratios and nuclear modification factors are determined. The results are compared with theoretical calculations based on collinear factorisation using nuclear parton distribution functions, on the colour glass condensate or on coherent energy loss models.</p
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