24 research outputs found
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Thesis (M.A.)--Boston University, 1933. This item was digitized by the Internet Archive
Observation of and search for decays
The first observation of the decay is reported
using proton-proton collision data corresponding to an integrated luminosity of
recorded by the LHCb experiment at centre-of-mass energies
of 7 and 8 TeV. The resonance is produced in the decay . The product of branching fractions normalised to that for
the intermediate state, , is measured to be
\begin{align*} {\cal R}_{\eta_{c}(2S)}\equiv\frac{{\mathcal B}(B^{+} \to
\eta_{c}(2S) K^{+}) \times {\mathcal B}(\eta_{c}(2S) \to p \bar p)}{{\mathcal
B}(B^{+} \to J/\psi K^{+}) \times {\mathcal B}(J/\psi\to p \bar p)} =~& (1.58
\pm 0.33 \pm 0.09)\times 10^{-2}, \end{align*} where the first uncertainty is
statistical and the second systematic. No signals for the decays and
are seen, and the 95\% confidence level upper limits on their relative
branching ratios are % found to be and
. In addition, the mass differences between the
and the states, between the and the
states, and the natural width of the are measured as
\begin{align*} M_{J/\psi} - M_{\eta_{c}(1S)} =~& 110.2 \pm 0.5 \pm 0.9 \rm \,
MeV, M_{\psi(2S)} -M_{\eta_{c}(2S)} =~ & 52.5 \pm 1.7 \pm 0.6 \rm \, MeV,
\Gamma_{\eta_{c}(1S)} =~& 34.0 \pm 1.9 \pm 1.3 \rm \, MeV. \end{align*}Comment: 16 pages, 2 figures All figures and tables, along with any
supplementary material and additional information, are available at
https://lhcbproject.web.cern.ch/lhcbproject/Publications/LHCbProjectPublic/LHCb-PAPER-2016-016.htm
Measurement of the inelastic pp cross-section at a centre-of-mass energy of root s=7 TeV
The cross-section for inelastic proton-proton collisions, with at least one
prompt long-lived charged particle of transverse momentum
GeV/ in the pseudorapidity range , is measured by the LHCb
experiment at a centre-of-mass energy of TeV. The cross-section in
this kinematic range is determined to be mb within the spectrometer acceptance with an experimental uncertainty
that is dominated by systematic contributions. Extrapolation to the full phase
space, using PYTHIA 6, yields mb,
where the first uncertainty is experimental and the second is due to the
extrapolation.Comment: 15 pages, 2 figure
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
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
Measurement of indirect CP asymmetries in D-0 -> K-K+ and D-0 -> pi(-)pi(+) decays using semileptonic B decays
Time-dependent asymmetries in the decay rates of the singly
Cabibbo-suppressed decays and are measured in collision data corresponding to an integrated
luminosity of 3.0 fb collected by the LHCb experiment. The mesons
are produced in semileptonic -hadron decays, where the charge of the
accompanying muon is used to determine the initial state as or
. The asymmetries in effective lifetimes between and
decays, which are sensitive to indirect violation, are
determined to be \begin{align*}
A_{\Gamma}(K^-K^+) = (-0.134 \pm 0.077 \; {}^{+0.026}_{-0.034})\% \,
A_{\Gamma}(\pi^-\pi^+) = (-0.092\pm 0.145 \; {}^{+0.025}_{-0.033})\% \,
\end{align*} where the first uncertainties are statistical and the second
systematic. This result is in agreement with previous measurements and with the
hypothesis of no indirect violation in decays.Comment: 20 pages, 4 figure
Measurement of the lifetime of the meson using the decay mode
The difference in total widths between the and mesons is
measured using 3.0fb of data collected by the LHCb experiment in 7 and 8
TeV centre-of-mass energy proton-proton collisions at the LHC. Through the
study of the time evolution of and
decays, the width difference is measured to be
where the first uncertainty is statistical and the second
systematic. The known lifetime of the meson is used to convert this to a
precise measurement of the lifetime,
where the first uncertainty is
statistical and the second systematic.Comment: 19 pagers, 3 figure
Measurement of the CP-violating phase in decays and limits on penguin effects
Time-dependent CP violation is measured in the channel for each resonant final state using data
collected with an integrated luminosity of 3.0 fb in collisions
using the LHCb detector. The final state with the largest rate,
, is used to measure the CP-violating angle to be . This result can be used to
limit the size of penguin amplitude contributions to CP violation measurements
in, for example, decays. Assuming approximate
SU(3) flavour symmetry and neglecting higher order diagrams, the shift in the
CP-violating phase is limited to be within the interval
[, +] at 95% confidence level. Changes to the limit
due to SU(3) symmetry breaking effects are also discussed.Comment: 18 pages, 6 figures; v2-updated from reviewers comments and added a
figur