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  • 1990-1994  (4)
  • 1993  (4)
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  • 1990-1994  (4)
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  • 1
    ISSN: 1434-6052
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract From the combined data of 1990 and 1991 of the DELPHI experiment at LEP, 13057 4-jet events are obtained and used for determining the contribution of the triple-gluon vertex. The relevant variables are the generalized Nachtmann Reiter angle θ NR * and the opening angle of the two least energetic jets. A fit to their two-dimensional distribution yields $$C_A /C_F = 2.12 \pm 0.35 and N_C /N_A = 0.46 \pm 0.19,$$ whereC A/C F is the ratio of the coupling strength of the triple-gluon vertex to that of gluon bremsstrahlung from quarks, andN C/N A, the ratio of the number of quark colours to the number of gluons. This constitutes a convincing model-independent proof of the existence of the triple-gluon vertex, since its contribution is directly proportional toC A/C F. The results are in agreement with the values expected from QCD:C A/C F=2.25, andN C/N A=3/8.
    Type of Medium: Electronic Resource
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  • 2
    ISSN: 1434-6052
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract A new measurement of αs is obtained from the distributions in thrust, heavy jet mass, energy-energy correlation and two recently introduced jet broadening variables following a method proposed by Catani, Trentadue, Turnock and Webber. This method includes the full calculation ofO( s 2 ) terms and leading and next-to-leading logarithms resummed to all orders of αs. The analysis is based on data taken with the DELPHI detector at LEP during 1991. I its found that the inclusion of the resummed leading and next-to-leading logarithms reduces the scale dependence of αs and allows an extension of the fit range towards the infrared limit of the kinematical range. The combined value for αs obtained at the scale μ2=M Z 2 is: $$\alpha _s (M_Z^2 ) = 0.123 \pm 0.006.$$
    Type of Medium: Electronic Resource
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  • 3
    ISSN: 1434-6052
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract A study ofB meson decays intoDl X final states is presented. In these events, neutral and chargedD mesons originate predominantly fromB + andB 0 decays, respectively. The dilution of this correlation due toD ** production has been taken into account. From 263 700 hadronicZ 0 decays collected in 1991 with the DELPHI detector at the LEP collider, 92D 0→K -π+, 35D +→K -π+π+ and 61D *0→D 0π+ followed byD 0→K -π+ orD 0→K -π+π+π-, are found with an associated lepton of the same charge as the kaon. From theD 0 l - andD *+ l -, the probabilityf d that ab quark hadronizes into aB − (or $$\bar B^0 $$ ) meson is found to be 0.44 ±0.08±0.09, corresponding to a total (B s+Λ b ) hadronization fraction of 0.12 −0.12 +0.24 . By reconstructing the energy of eachB meson, theb quark fragmentation is directly measured for the first time. The mean value of theB meson energy fraction is: $$\left\langle {X_E (B)} \right\rangle = 0.695 \pm 0.015(stat.) \pm 0.029(syst.)$$ ReconstructingD-lepton vertices, the followingB lifetimes are measured: $$\begin{gathered} \tau (B) = 1.27_{ - 0.18}^{ + 0.22} (stat.) \pm 0.15(syst.)ps, \hfill \\ where\bar B \to D^0 \ell ^ - X, \hfill \\ \tau (B) = 1.18_{ - 0.27}^{ + 0.39} (stat.) \pm 0.15(syst.)ps, \hfill \\ where\bar B \to D^ + \ell ^ - X, \hfill \\ \tau (B) = 1.19_{ - 0.19}^{ + 0.25} (stat.) \pm 0.15(syst.)ps \hfill \\ where\bar B \to D^{* + } \ell ^ - X, \hfill \\ \end{gathered} $$ and an average τ(B)=1.23 −0.13 +0.14 (stat.)±0.15(syst.) ps is found. Allowing for decays into $$D**\ell ^ - \bar v$$ , theB + andB 0 lifetimes are: $$\begin{gathered} \tau (B^ + ) = 1.30_{ - 0.29}^{ + 0.33} (stat.) \pm 0.15(syst.\exp .) \hfill \\ \pm 0.05(syst.D**)ps, \hfill \\ \tau (B^0 ) = 1.17_{ - 0.23}^{ + 0.29} (stat.) \pm 0.51(syst.\exp .) \hfill \\ \pm 0.05(syst.D**)ps, \hfill \\ \tau (B^ + )/\tau (B^0 ) = 1.11_{ - 0.39}^{ + 0.51} (stat.) \pm 0.05(syst.\exp .) \hfill \\ \pm 0.10(syst.D**)ps. \hfill \\ \end{gathered} $$
    Type of Medium: Electronic Resource
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  • 4
    ISSN: 1434-6052
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract A study of the fragmentation properties of charm and bottom quarks intoD mesons is presented. From 263 700Z 0 hadronic decays collected in 1991 with the DELPHI detector at the LEP collider,D 0,D + andD *+ are reconstructed in the modesK − π +,K − π + K + andD 0 π + followed byD 0→K − π +, respectively. The fractional decay widths $$\Gamma {{(Z^0 \to {D \mathord{\left/ {\vphantom {D {\bar D}}} \right. \kern-\nulldelimiterspace} {\bar D}}X)} \mathord{\left/ {\vphantom {{(Z^0 \to {D \mathord{\left/ {\vphantom {D {\bar D}}} \right. \kern-\nulldelimiterspace} {\bar D}}X)} {\Gamma _h }}} \right. \kern-\nulldelimiterspace} {\Gamma _h }}$$ are determined, and first results are presented for the production ofD mesons from $$c\bar c$$ and $$b\bar b$$ events separately. The average energy fraction ofD *± in charm quark fragmentation is found to be 〈X E (D *)〉 c =0.487±0.015 (stat)±0.005 (sys.). Assuming that the fraction ofD s and charm-baryons produced at LEP is similar to that around 10 GeV, theZ 0 partial width into charm quark pairs is determined to beΓ c /Γ h =0.187±0.031 (stat)±0.023 (sys). The probability for ab quark to fragment into $$\bar B_s $$ orb-baryons is inferred to be 0.268±0.094 (stat)±0.100 (sys) from the measured probability that it fragments into a $$\bar B^0 $$ orB −.
    Type of Medium: Electronic Resource
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