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Study of the process e+eμ+μ in the energy region s=980, 1040–1380 MeV

M. N. Achasov, V. M. Aulchenko, K. I. Beloborodov, A. V. Berdyugin, A. G. Bogdanchikov, A. D. Bukin, D. A. Bukin, T. V. Dimova, V. P. Druzhinin, V. B. Golubev, I. A. Koop, A. A. Korol, S. V. Koshuba, A. P. Lysenko, E. V. Pakhtusova, E. A. Perevedentsev, S. I. Serednyakov, Yu. M. Shatunov, Z. K. Silagadze, A. N. Skrinsky, Yu. A. Tikhonov, and A. V. Vasiljev
Phys. Rev. D 79, 112012 – Published 24 June 2009

Abstract

The cross section of the process e+eμ+μ was measured in the spherical neutral detector experiment at the VEPP-2M e+e collider in the energy region s=980, 1040–1380 MeV. The event numbers of the process e+eμ+μ were normalized to the integrated luminosity measured using e+ee+e and e+eγγ processes. The ratio of the measured cross section to the theoretically predicted value is 1.006±0.007±0.016 and 1.005±0.007±0.018 in the first and second case, respectively. Using results of the measurements, the electromagnetic running coupling constant α in the energy region s=10401380MeV was obtained 1/α=134.1±0.5±1.2 and this is in agreement with theoretical expectation.

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  • Received 5 October 2008

DOI:https://doi.org/10.1103/PhysRevD.79.112012

©2009 American Physical Society

Authors & Affiliations

M. N. Achasov*, V. M. Aulchenko, K. I. Beloborodov, A. V. Berdyugin, A. G. Bogdanchikov, A. D. Bukin, D. A. Bukin, T. V. Dimova, V. P. Druzhinin, V. B. Golubev, I. A. Koop, A. A. Korol, S. V. Koshuba, A. P. Lysenko, E. V. Pakhtusova, E. A. Perevedentsev, S. I. Serednyakov, Yu. M. Shatunov, Z. K. Silagadze, A. N. Skrinsky, Yu. A. Tikhonov, and A. V. Vasiljev

  • Budker Institute of Nuclear Physics, Siberian Branch of the Russian Academy of Sciences, 11 Lavrentyev, Novosibirsk 630090, Russia
  • Novosibirsk State University, Novosibirsk 630090, Russia

  • *achasov@inp.nsk.su

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Vol. 79, Iss. 11 — 1 June 2009

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Images

  • Figure 1
    Figure 1
    Feynman diagrams of the process e+eμ+μ: (a) diagram in the lowest order; (b) vacuum polarization diagram, the loops are due to fermion pairs—electrons, muons, τ leptons, and quarks.Reuse & Permissions
  • Figure 2
    Figure 2
    The Feynman diagrams of the e+ee+e process in lowest order.Reuse & Permissions
  • Figure 3
    Figure 3
    The Feynman diagram of the e+eγγ process in lowest order.Reuse & Permissions
  • Figure 4
    Figure 4
    The Feynman diagrams of the process e+ee+e with vacuum polarization due to virtual fermion pairs (electrons, muons, τ leptons, and quarks).Reuse & Permissions
  • Figure 5
    Figure 5
    The distribution of the z coordinate of the charged particles production point in events selected as e+eμ+μ at the energy s=1370MeV. Dots—all events; dashed distribution—cosmic background events; and curve—the fit by sum of distributions of beam and cosmic events.Reuse & Permissions
  • Figure 6
    Figure 6
    Energy deposition spectra for the muons in experiment (dots) and simulation (histogram).Reuse & Permissions
  • Figure 7
    Figure 7
    Energy deposition spectra for electrons with energies of 490, 590, and 690 MeV in experiment (dots) and simulation (histogram).Reuse & Permissions
  • Figure 8
    Figure 8
    Energy deposition spectra for photons with energies of 490, 590, and 690 MeV in experiment (dots) and simulation (histogram).Reuse & Permissions
  • Figure 9
    Figure 9
    The Δθ distribution of the e+ee+e events. Dots—experiment; histogram—simulation.Reuse & Permissions
  • Figure 10
    Figure 10
    The Δϕ distribution of the e+ee+e events. Dots—experiment; histogram—simulation.Reuse & Permissions
  • Figure 11
    Figure 11
    The Δθ distribution of the e+eγγ events. Dots—experiment; histogram—simulation.Reuse & Permissions
  • Figure 12
    Figure 12
    The Δϕ distribution of the e+eγγ events. Dots—experiment; histogram—simulation.Reuse & Permissions
  • Figure 13
    Figure 13
    The Δθ distribution of the e+eμ+μ events. Dots—experiment; histogram—simulation.Reuse & Permissions
  • Figure 14
    Figure 14
    The Δϕ distribution of the e+eμ+μ events. Dots—experiment; histogram—simulation.Reuse & Permissions
  • Figure 15
    Figure 15
    The θ angle distribution of the e+ee+e events. Dots—experiment; histogram—simulation.Reuse & Permissions
  • Figure 16
    Figure 16
    The θ angle distribution of the e+eμ+μ events. Dots—experiment; histogram—simulation.Reuse & Permissions
  • Figure 17
    Figure 17
    The θ angle distribution of the e+eγγ events. Dots—experiment; histogram—simulation.Reuse & Permissions
  • Figure 18
    Figure 18
    The ratio of the θ distributions of the e+eμ+μ and e+ee+e events. Dots—experiment; histogram—simulation.Reuse & Permissions
  • Figure 19
    Figure 19
    The ratio of the θ distributions of the e+ee+e and e+eγγ events. Dots—experiment; histogram—simulation.Reuse & Permissions
  • Figure 20
    Figure 20
    The e+ee+e cross section in the angular range 30°<θe±<150°. Dots are the SND data obtained in this work; the curve is the result of the fit (χ2/Nd.o.f.=48.1/34).Reuse & Permissions
  • Figure 21
    Figure 21
    The ratio σexp/σthe of the e+eμ+μ cross section measured by SND (, this work) and CMD-2 (●, 4) to theoretical value. The horizontal bars show the energy region s in which the cross section was measured.Reuse & Permissions
  • Figure 22
    Figure 22
    The e+eμ+μ cross section obtained by using ILγγ. Dots are the SND data obtained in this work; the curve is the result of the fit (χ2/Nd.o.f.=37.2/34).Reuse & Permissions
  • Figure 23
    Figure 23
    The α(s)1 values obtained by using different experiment results. The SND (, this work), TOPAZ (▪, 21), and OPAL (●, 22) results are presented. The dots from review 23 obtained using results of experiments at DORIS (◯), PEP (□), and PETRA (△) colliders are presented also. Horizontal line shows the α(0)1 value; curve is theoretical calculation of α(s)1.Reuse & Permissions
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