A study of the b-quark fragmentation function with the DELPHI detector at LEP I and an averaged distribution obtained at the Z Pole

被引:0
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作者
J. Abdallah
P. Abreu
W. Adam
P. Adzic
T. Albrecht
R. Alemany-Fernandez
T. Allmendinger
P. P. Allport
U. Amaldi
N. Amapane
S. Amato
E. Anashkin
A. Andreazza
S. Andringa
N. Anjos
P. Antilogus
W-D. Apel
Y. Arnoud
S. Ask
B. Asman
J. E. Augustin
A. Augustinus
P. Baillon
A. Ballestrero
P. Bambade
R. Barbier
D. Bardin
G. J. Barker
A. Baroncelli
M. Battaglia
M. Baubillier
K-H. Becks
M. Begalli
A. Behrmann
E. Ben-Haim
N. Benekos
A. Benvenuti
C. Berat
M. Berggren
D. Bertrand
M. Besancon
N. Besson
D. Bloch
M. Blom
M. Bluj
M. Bonesini
M. Boonekamp
P. S. L. Booth
G. Borisov
O. Botner
机构
[1] Iowa State University,Department of Physics and Astronomy
[2] Universiteit Antwerpen,Physics Department
[3] ULB-VUB,IIHE
[4] University of Athens,Physics Laboratory
[5] University of Bergen,Department of Physics
[6] Università di Bologna and INFN,Dipartimento di Fisica
[7] Centro Brasileiro de Pesquisas Físicas,Inst. de Física
[8] Univ. Estadual do Rio de Janeiro,Collège de France, Lab. de Physique Corpusculaire
[9] IN2P3-CNRS,Institut Pluridisciplinaire Hubert Curien
[10] CERN,Institute of Nuclear Physics
[11] Université de Strasbourg,FZU
[12] IN2P3-CNRS,Dipartimento di Fisica
[13] N.C.S.R. Demokritos,Institut des Sciences Nucléaires, IN2P3
[14] Inst. of Phys. of the C.A.S. High Energy Physics Division,CNRS
[15] Università di Genova and INFN,Institut für Experimentelle Kernphysik
[16] Université de Grenoble 1,Faculty of Physics and Nuclear Techniques
[17] Helsinki Institute of Physics and Department of Physical Sciences,LAL
[18] Joint Institute for Nuclear Research,School of Physics and Chemistry
[19] Dubna,LIP, IST
[20] Universität Karlsruhe,Department of Physics
[21] Institute of Nuclear Physics PAN,Dept. of Physics and Astronomy, Kelvin Building
[22] University of Mining and Metallurgy,LPNHE
[23] Univ Paris-Sud,Department of Physics
[24] CNRS/IN2P3,IPNL, IN2P3
[25] University of Lancaster,CNRS
[26] FCUL,Dipartimento di Fisica
[27] University of Liverpool,Dipartimento di Fisica
[28] University of Glasgow,IPNP of MFF
[29] Univ. Pierre et Marie Curie,Physics Department
[30] Univ. Paris Diderot,Physics Department
[31] CNRS/IN2P3,Dpto. Fisica
[32] University of Lund,Department of Physics
[33] Université Claude Bernard de Lyon,Dipartimento di Fisica
[34] Università di Milano and INFN-MILANO,Dipartimento di Fisica
[35] Univ. di Milano-Bicocca and INFN-MILANO,Dipartimento di Fisica
[36] Charles Univ.,DAPNIA/Service de Physique des Particules
[37] NIKHEF,Laboratory for Astroparticle Physics
[38] National Technical University,Department of Physics
[39] University of Oslo,Fysikum
[40] Blindern,Dipartimento di Fisica Sperimentale
[41] Univ. Oviedo,INFN, Sezione di Torino and Dipartimento di Fisica Teorica
[42] University of Oxford,Dipartimento di Fisica
[43] Università di Padova and INFN,Istituto di Fisica
[44] Rutherford Appleton Laboratory,Department of Radiation Sciences
[45] Università di Roma II and INFN,Institut für Hochenergiephysik
[46] Tor Vergata,Fachbereich Physik
[47] Università di Roma III and INFN,undefined
[48] CEA-Saclay,undefined
[49] Instituto de Fisica de Cantabria (CSIC-UC),undefined
[50] Inst. for High Energy Physics,undefined
来源
关键词
Systematic Uncertainty; Fragmentation Function; Parton Shower; Time Projection Chamber; Secondary Vertex;
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摘要
The nature of b-quark jet hadronisation has been investigated using data taken at the Z peak by the DELPHI detector at LEP. Two complementary methods are used to reconstruct the energy of weakly decaying b-hadrons, \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$E_{\mathrm{B}}^{\mathrm{weak}}$\end{document}. The average value of \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$x^{\mathrm{weak}}_{\mathrm{B}} = E_{\mathrm{B}}^{\mathrm{weak}}/E_{\mathrm{beam}}$\end{document} is measured to be 0.699±0.011. The resulting \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$x^{\mathrm{weak}}_{\mathrm{B}}$\end{document} distribution is then analysed in the framework of two choices for the perturbative contribution (parton shower and Next to Leading Log QCD calculation) in order to extract measurements of the non-perturbative contribution to be used in studies of b-hadron production in other experimental environments than LEP. In the parton shower framework, data favour the Lund model ansatz and corresponding values of its parameters have been determined within PYTHIA 6.156 from DELPHI data: \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$a= 1.84^{+0.23}_{-0.21}\quad\mbox{and}\quad b=0.642^{+0.073}_{-0.063}~\mathrm{GeV}^{-2},$$\end{document} with a correlation factor ρ=92.2%.
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