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1993, Physical Review Letters
Physical review letters, 2018
The first measurement of the lifetime of the doubly charmed baryon Ξ_{cc}^{++} is presented, with the signal reconstructed in the final state Λ_{c}^{+}K^{-}π^{+}π^{+}. The data sample used corresponds to an integrated luminosity of 1.7 fb^{-1}, collected by the LHCb experiment in proton-proton collisions at a center-of-mass energy of 13 TeV. The Ξ_{cc}^{++} lifetime is measured to be 0.256_{-0.022}^{+0.024}(stat)±0.014(syst) ps.
Annual Review of Nuclear and Particle Science, 1996
We review recent experimental results on lifetimes and hadronic decays of hadrons that contain c and b quarks. The theoretical implications of these results are also considered. An understanding of hadronic decays of heavy quarks is required to interpret the CP violating asymmetries in B decays that will be observed in experiments planned for the near future.
Annals of the New York Academy of Sciences, 1988
Since the first Symposium on Heavy Flavors, in May, 1986, there have been many important new experimental results in charm physics. Among these have been precise D, and Ac lifetimes, new absolute branching ratios, many 0, branching ratios, confirmation of an excited charmed resonance in the D*u system, and observation of a similar state in the Du system. Discussions of these topics are included in the review that follows. Other&portant results included in other reviews at this conference are new limits on Do-Do mixing' and a new limit on f D from D+-p+ur decays.* CHARM LIFETIMES The basic ideas behind the present picture of charm decays are discussed extensively in the theoretical review.' For reference, FIGURE 1 shows four quark diagrams representing the Cabibbo-allowed decays of charmed mesons. The first two are spectator diagrams in which the light quark is not one of the four fermions at the weak vertex. The last two are nonspectator diagrams-Wexchange for the Do and W annihilation for the 0 , '. Much theoretical effort has been expended in trying to investigate the relative strength of the nonspectator amplitudes. The central experimental fact that must be explained is T(D+)/T(DO) = 2.6. The most obvious candidate to explain the large lifetime ratio is a large contribution from the W-exchange and V-annihilation diagrams because these contribute to Do and D,+, but not D' decays. Theoretically, these diagrams were expected to make rather small contributions to charmed meson decay because of helicity suppression. Experimentally, Mark I11 sets a limit,f, 5 290 MeV, from a search for the decay, D +-p+u,. Unlessjb, the effective decay constant for nonleptonic decays, is much larger than this, the W-exchange diagram should account for a small fraction of the total Do decay rate? The only direct way to measure the contribution of nonspectator diagrams to hadronic decay rates is to look foidecay modes that should be very small for the spectator diagrams. One of these is Do-K04, for which a rather large branching ratio of about 18 has been mea~ured.~ It is not clear, though, to what extent final state interactions are responsible for any single final state. Another decay of this type is 0,'-POT+, which will be discussed later. The second possible cause of the large difference in D lifetimes is suppression of the D
Brazilian Journal of Physics, 2004
The connection between light quark spectroscopy and hadronic decays of D mesons is discussed, with emphasis on the physics of the light scalar mesons. Recent results from charm decays are presented.
Physics Letters B, 1996
We have observed two new decay modes of the charmed baryon + c into + K + and + K 0 using data collected with the CLEO II detector. We also present the rst measurement of the branching fraction for the previously observed decay mode + c ! K + +. The branching fractions for these three modes relative to + c ! + + are measured to be
Physical Review Letters, 2011
2000
The partial decay width R c of the Z into cc quark pair and the number of charm quarks n c per b decay are measured with the DELPHI detector at LEP 1. Particle identification provides clear D 0 , D + , D + s and Λ + c signatures. The charm hadron production rate is measured in each channel by a fit to the scaled energy, impact parameter information and the invariant mass spectrum. Two measurements of R c are presented, from the D * + production rate and from the overall charm counting, including strange charm baryon production, in cc events. The multiplicity n c , which includes hidden cc and strange charm baryon production, is inferred from the charm counting in bb events. The final results are R c = 0.1665 ± 0.0095 and n c = 1.166 ± 0.086. (Submitted to E. Phys. J. C) ii 1 There is no distinction between c-hadron and anti-c hadron in the present definition of P c(b)→D,Λc . 2 Throughout this paper charge-conjugate states are implicitly included.
Journal of High Energy Physics
Using proton-proton collision data, corresponding to an integrated luminosity of 9 fb−1 collected with the LHCb detector, seven decay modes of the $$ {\mathrm{B}}_{\mathrm{c}}^{+} $$ B c + meson into a J/ψ or ψ(2S) meson and three charged hadrons, kaons or pions, are studied. The decays $$ {\mathrm{B}}_{\mathrm{c}}^{+} $$ B c + → (ψ(2S) → J/ψπ+π−)π+, $$ {\mathrm{B}}_{\mathrm{c}}^{+} $$ B c + → ψ(2S)π+π−π+, $$ {\mathrm{B}}_{\mathrm{c}}^{+} $$ B c + → J/ψK+π−π+ and $$ {\mathrm{B}}_{\mathrm{c}}^{+} $$ B c + → J/ψK+K−K+ are observed for the first time, and evidence for the $$ {\mathrm{B}}_{\mathrm{c}}^{+} $$ B c + → ψ(2S)K+K−π+, decay is found, where J/ψ and ψ(2S) mesons are reconstructed in their dimuon decay modes. The ratios of branching fractions between the different $$ {\mathrm{B}}_{\mathrm{c}}^{+} $$ B c + decays are reported as well as the fractions of the decays proceeding via intermediate resonances. The results largely support the factorisation approach used for a theoretical...
Physical Review Letters, 2006
Physical Review Letters, 2011
Physics Letters B, 1998
New measurements of the lifetime and mass of the + c are presented. The + c has been reconstructed through the two decay channels , + + and + K , +. The data were accumulated by the Fermilab high energy photoproduction experiment E687. The lifetime is
Physics Reports, 1997
Introduction 4 4.4. Sample selection 2. Theoretical treatment of charm and beauty 4.5. Lifetime determination lifetimes 5 4.6. S-/I?' lifetimes 2.1. Phenomenology: Legends with truths 5 4.7. B, lifetime 2.2. From phenomenology to theory 8 4.8. Ah and the generic b-Baryon lifetime 2.3. Methodology of the heavy quark expansion 4.9. zh lifetime for fully integrated rates 10 4. IO. Inclusive measurements 3. The lifetimes of weakly decaying charm 4.11. Overall summary of current lifetime hadrons 17 values 3.1. Experimental devices 18 4.12. Predictions and interpretation of existing 3.2. Vertex reconstruction 38 relevant data 3.3. Lifetimes of the charmed mesons 49 5. Summary and outlook 3.4. Lifetimes of charmed baryons 55 5.1. Comments on the underlying concepts 3.5. Theoretical evaluation of the results 68 5.2. What have we learned and 4. The lifetimes of weakly decaying beauty what will we learn? hadrons 81 5.3. Future prospects for further experimental 4.1. Formation of B states in e+e-and pp 83 data 4.2. Identification of B decays 84 References 4.3. Detector requirements 87
Physical Review D, 1998
Physics Letters B, 2000
Using data recorded at centre-of-mass energies around 183 GeV and 189 GeV with the OPAL detector at LEP, the fundamental coupling of the charm quark to the W boson has been studied. The ratio R W c ≡ Γ (W → c X)/Γ (W → hadrons) has been measured from jet properties, lifetime information, and leptons produced in charm decays. A value compatible with the Standard Model expectation of 0.5 is obtained: R W c = 0.481±0.042 (stat.) ±0.032 (syst.). By combining this result with measurements of the W boson total width and hadronic branching ratio, the magnitude of the CKM matrix element |V cs | is determined to be |V cs | = 0.969 ± 0.058.
Physics Letters B, 1993
2022
The Ξ++ cc → Ξ ′+ c π + decay is observed using proton-proton collisions collected by the LHCb experiment at a centre-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 5.4 fb−1. The Ξ++ cc → Ξ ′+ c π + decay is reconstructed partially, where the photon from the Ξ ′+ c → Ξ+ c γ decay is not reconstructed and the pK−π+ final state of the Ξ+ c baryon is employed. The Ξ ++ cc → Ξ ′+ c π + branching fraction relative to that of the Ξ++ cc → Ξ+ c π+ decay is measured to be 1.41±0.17±0.10, where the first uncertainty is statistical and the second systematic.
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