75 research outputs found
Measurement of the cross-section for Z â e<sup>+</sup>e<sup>-</sup> production in pp collisions at √<span style="text-decoration:overline">s</span>=7 TeV
A measurement of the cross-section for ppâââZâââe+eâ is presented using data at sâ=7 TeV corresponding to an integrated luminosity of 0.94 fbâ1. The process is measured within the kinematic acceptance p Tâ>â20 GeV/c and 2â<âηâ<â4.5 for the daughter electrons and dielectron invariant mass in the range 60â120 GeV/c 2. The cross-section is determined to be Ï(ppâZâe+eâ)=76.0±0.8±2.0±2.6pb where the first uncertainty is statistical, the second is systematic and the third is the uncertainty in the luminosity. The measurement is performed as a function of Z rapidity and as a function of an angular variable which is closely related to the Z transverse momentum. The results are compared with previous LHCb measurements and with theoretical predictions from QCD
First measurement of coherent Ï0 photoproduction in ultra-peripheral XeâXe collisions at âsNN = 5.44 TeV
The first measurement of the coherent photoproduction of Ï0 vector mesons in ultra-peripheral XeâXe collisions at sNN=5.44 TeV is presented. This result, together with previous HERA Îłp data and ÎłâPb measurements from ALICE, describes the atomic number (A) dependence of this process, which is particularly sensitive to nuclear shadowing effects and to the approach to the black-disc limit of QCD at a semi-hard scale. The cross section of the Xe+XeâÏ0+Xe+Xe process, measured at midrapidity through the decay channel Ï0âÏ+Ïâ, is found to be dÏ/dy=131.5±5.6(stat.)â16.9+17.5(syst.) mb. The ratio of the continuum to resonant contributions for the production of pion pairs is also measured. In addition, the fraction of events accompanied by electromagnetic dissociation of either one or both colliding nuclei is reported. The dependence on A of cross section for the coherent Ï0 photoproduction at a centre-of-mass energy per nucleon of the ÎłA system of WÎłA,n=65 GeV is found to be consistent with a power-law behaviour Ï(ÎłAâÏ0A)âAα with a slope α=0.96±0.02(syst.). This slope signals important shadowing effects, but it is still far from the behaviour expected in the black-disc limit.publishedVersio
Study of eta-eta ' mixing from measurement of B-(s)(0) -> J/psi eta((')) decay rates
A study of B and Bs meson decays into J/Ï Î· and J/Ï Î·âČ final states is performed using a data set of proton-proton collisions at centre-of-mass energies of 7 and 8 TeV, collected by the LCHb experiment and corresponding to 3.0 fbâ1 of integrated luminosity. The decay B0 â J/Ï Î·âČ is observed for the first time. The following ratios of branching fractions are measured:
B(B0âJ/ÏηâČ)B(B0sâ J/ÏηâČ)=(2.28±0.65 (stat)±0.10 (syst)±0.13 (fs/fd))Ă10â2,B(B0â J/Ïη)B(B0sâ J/Ïη)=(1.85±0.61 (stat)±0.09 (syst)±0.11 (fs/fd))Ă10â2, where the third uncertainty is related to the present knowledge of fs/fd, the ratio between the probabilities for a b quark to form a Bs or a B0 meson. The branching fraction ratios are used to determine the parameters of η â ηâČ meson mixing. In addition, the first evidence for the decay Bs â Ï(2S)ηâČ is reported, and the relative branching fraction is measured,
B(B0sâ Ï(2S)ηâČ)B(B0sâ J/ÏηâČ)=(38.7±9.0 (stat)±1.3 (syst)±0.9(B))Ă10â2, where the third uncertainty is due to the limited knowledge of the branching fractions of J/Ï and Ï(2S) mesons
Measurement of the Z plus b-jet cross-section in pp collisions at root s=7 TeV in the forward region
The associated production of a Z boson or an off-shell photon with
a bottom quark in the forward region is studied using proton-proton collisions
at a centre-of-mass energy of . The Z bosons
are reconstructed in the
final state from muons with a transverse momentum larger than
, while two transverse momentum thresholds are
considered for jets ( and
). Both muons and jets are reconstructed in
the pseudorapidity range . The results are based on data
corresponding to 1.0{\,\mbox{fb}^{-1}} recorded in 2011 with the LHCb
detector. The measurement of the Z+b-jet cross-section is normalized to the
Z+jet cross-section. The measured cross-sections are \begin{equation*}
\sigma(\text{+b-jet}) = 295 \pm
60~(\text{stat}) \pm 51~(\text{syst}) \pm 10~(\text{lumi}) {\,\mbox{fb}}
\end{equation*} for (jet), and
\begin{equation*} \sigma(\text{+b-jet}) =
128 \pm 36~(\text{stat}) \pm 22~(\text{syst}) \pm 5~(\text{lumi}) {\,\mbox{fb}}
\end{equation*} for (jet)
Precise measurements of the properties of the B-1(5721)(0,+) and B-2*(5747)(0,+) states and observation of B-+,B-0 pi(-,+) mass structures
Invariant mass distributions of B+pi- and B0pi+ combinations are investigated
in order to study excited B mesons. The analysis is based on a data sample
corresponding to 3.0 fb-1 of pp collision data, recorded by the LHCb detector
at centre-of-mass energies of 7 and 8 TeV. Precise measurements of the masses
and widths of the B_1(5721)^(0,+) and B_2*(5747)^(0,+) states are reported.
Clear enhancements, particularly prominent at high pion transverse momentum,
are seen over background in the mass range 5850--6000 MeV in both B+pi- and
B0pi+ combinations. The structures are consistent with the presence of four
excited B mesons, labelled B_J(5840)^(0,+) and B_J(5960)^(0,+), whose masses
and widths are obtained under different hypotheses for their quantum numbers.Comment: 29 pages, 5 Figures, 8 Table
A(c)(+) Production and Baryon-to-Meson Ratios in pp and p-Pb Collisions at root S-NN=5.02 TeV at the LHC
The prompt production of the charm baryon \u39bc+ and the \u39bc+/D0 production ratios were measured at midrapidity with the ALICE detector in pp and p-Pb collisions at sNN=5.02 TeV. These new measurements show a clear decrease of the \u39bc+/D0 ratio with increasing transverse momentum (pT) in both collision systems in the range 2<12 GeV/c, exhibiting similarities with the light-flavor baryon-to-meson ratios p/\u3c0 and \u39b/KS0. At low pT, predictions that include additional color-reconnection mechanisms beyond the leading-color approximation, assume the existence of additional higher-mass charm-baryon states, or include hadronization via coalescence can describe the data, while predictions driven by charm-quark fragmentation processes measured in e+e- and e-p collisions significantly underestimate the data. The results presented in this Letter provide significant evidence that the established assumption of universality (colliding-system independence) of parton-to-hadron fragmentation is not sufficient to describe charm-baryon production in hadronic collisions at LHC energies
A(c)(+) Production and Baryon-to-Meson Ratios in pp and p-Pb Collisions at root S-NN=5.02 TeV at the LHC
The prompt production of the charm baryon Î_{c}^{+} and the Î_{c}^{+}/D^{0} production ratios were measured at midrapidity with the ALICE detector in pp and p-Pb collisions at sqrt[s_{NN}]=5.02ââTeV. These new measurements show a clear decrease of the Î_{c}^{+}/D^{0} ratio with increasing transverse momentum (p_{T}) in both collision systems in the range 2<p_{T}<12ââGeV/c, exhibiting similarities with the light-flavor baryon-to-meson ratios p/Ï and Î/K_{S}^{0}. At low p_{T}, predictions that include additional color-reconnection mechanisms beyond the leading-color approximation, assume the existence of additional higher-mass charm-baryon states, or include hadronization via coalescence can describe the data, while predictions driven by charm-quark fragmentation processes measured in e^{+}e^{-} and e^{-}p collisions significantly underestimate the data. The results presented in this Letter provide significant evidence that the established assumption of universality (colliding-system independence) of parton-to-hadron fragmentation is not sufficient to describe charm-baryon production in hadronic collisions at LHC energies
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