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Dive into the research topics where A.Yu. Barnyakov is active.

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Featured researches published by A.Yu. Barnyakov.


Jetp Letters | 2007

Measurement of the τ lepton mass at the KEDR detector

V.V. Anashin; V. Aulchenko; Evgenii Baldin; A.K. Barladyan; A.Yu. Barnyakov; M.Yu. Barnyakov; S. E. Baru; I. V. Bedny; O. Beloborodova; A. E. Blinov; V. E. Blinov; A. B. Bobrov; V. S. Bobrovnikov; A.V. Bogomyagkov; A. Bondar; D. V. Bondarev; A. R. Buzykaev; V. P. Cherepanov; S. Eidelman; Yu.M. Glukhovchenko; V.V. Gulevich; S.E. Karnaev; G.V. Karpov; S.V. Karpov; V.A. Kiselev; S.A. Kononov; K.Yu. Kotov; E. A. Kravchenko; E.V. Kremyanskaya; V.F. Kulikov

A precise τ lepton mass measurement performed at the VEPP-4M collider with the KEDR detector is reported. The mass value is evaluated from the τ+τ− cross section behavior around the production threshold. The result based on 6.7 pb−1 of data is mτ = 1776.81−0.23+0.25 ± 0.15 MeV. Using 0.8 pb−1 of data collected at the ψ′ peak, we have also determined that ΓeeBττ(ψ′) = 9.0 ± 2.6 eV.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2002

ASHIPH counters for the KEDR detector

A.Yu. Barnyakov; M.Yu. Barnyakov; V.S. Bobrovnikov; A. R. Buzykaev; A.F. Danilyuk; F.F Guber; G. M. Kolachev; S.A. Kononov; V.A Krasnov; E. A. Kravchenko; A. B. Kurepin; G.D Minakov; A. P. Onuchin; G.A. Savinov; V.A. Tayursky

Abstract The status of the ASHIPH (Aerogel, wavelength SHIfter, and PHotomultipliers) system of the KEDR detector is described. The measurement of the quality of the particle identification with the ASHIPH counters was performed. The π/K separation is 4.5σ for the momentum 1.2 GeV /c and 4.7σ for the momentum 0.86 GeV /c . Timing properties of the ASHIPH counter are measured. The time resolution for pions is 2 ns , and the BBQ decay time is 15 ns . The advantages and disadvantages of Cherenkov counters filled with aerogel crumb are discussed. The process of the mass counter production for the KEDR detector is described.


Physics Letters B | 2012

Measurement of main parameters of the ψ(2S) resonance

V.V. Anashin; V. Aulchenko; Evgenii Baldin; A.K. Barladyan; A.Yu. Barnyakov; M.Yu. Barnyakov; S.E. Baru; I.Yu. Basok; O. Beloborodova; A. E. Blinov; V. E. Blinov; A. Bobrov; V. S. Bobrovnikov; A.V. Bogomyagkov; A. Bondar; A. R. Buzykaev; S. Eidelman; D. N. Grigoriev; Yu.M. Glukhovchenko; V.V. Gulevich; D.V. Gusev; S.E. Karnaev; G.V. Karpov; S.V. Karpov; Tatyana Kharlamova; V.A. Kiselev; V.V. Kolmogorov; S.A. Kononov; K.Yu. Kotov; E.A. Kravchenko

A high-precision determination of the main parameters of th eψ(2S ) resonance has been performed with the KEDR detector at the VEPP-4Me+e− collider in three scans of the ψ(2S )–ψ(3770) energy range. Fitting the energy dependence of the mu ltihadron cross section in the vicinity of theψ(2S ) we obtainedthe mass value M = 3686.114± 0.007± 0.011 +0.002 −0.012 MeV and the product of the electron partial width by the branchin g fraction into hadrons Γee × Bh = 2.233± 0.015± 0.037± 0.020 keV. The third error quoted is an estimate of the model dependence of the result due to assumptions on the interference e ffects in the cross section of the single-photon e+e− annihilation to hadrons explicitly considered in this work . Implicitly, the same assumptions were employed to obtain the charmonium leptonic width and th e absolute branching fractions in many experiments. Usingthe result presented and the world average values of the electron and hadron branchin g fractions, one obtains the electron partial width and the total width of the ψ(2S ): Γee = 2.282± 0.015± 0.038± 0.021 keV, Γ = 296± 2± 8± 3 keV. These results are consistent with and more than two times mor e precise than any of the previous experiments.


Physics Letters B | 2012

Measurement of ψ(3770) parameters

V.V. Anashin; V. Aulchenko; Evgenii Baldin; A.K. Barladyan; A.Yu. Barnyakov; M.Yu. Barnyakov; S.E. Baru; I.Yu. Basok; O. Beloborodova; A. E. Blinov; V. E. Blinov; A. Bobrov; V. S. Bobrovnikov; A.V. Bogomyagkov; A. Bondar; A. R. Buzykaev; S. Eidelman; D. N. Grigoriev; Yu.M. Glukhovchenko; V.V. Gulevich; D.V. Gusev; S.E. Karnaev; G.V. Karpov; S.V. Karpov; Tatyana Kharlamova; V.A. Kiselev; V.V. Kolmogorov; S.A. Kononov; K.Yu. Kotov; E.A. Kravchenko

Abstract We report the final results of a study of the ψ ( 3770 ) meson using a data sample collected with the KEDR detector at the VEPP-4M electron–positron collider. The data analysis takes into account interference between the resonant and nonresonant D D ¯ production, where the latter is related to the nonresonant part of the energy-dependent form factor F D . The vector dominance approach and several empirical parameterizations have been tried for the nonresonant F D N R ( s ) . Our results for the mass and total width of ψ ( 3770 ) are M = 3779.2 − 1.7 + 1.8 − 0.7 + 0.5 − 0.3 + 0.3 MeV , Γ = 24.9 − 4.0 + 4.6 − 0.6 + 0.5 − 0.9 + 0.2 MeV , where the first, second and third uncertainties are statistical, systematic and model, respectively. For the electron partial width two possible solutions have been found: ( 1 ) Γ e e = 154 − 58 + 79 − 9 + 17 − 25 + 13 eV , ( 2 ) Γ e e = 414 − 80 + 72 − 26 + 24 − 10 + 90 eV . Our statistics are insufficient to prefer one solution to another. The Solution (2) mitigates the problem of non- D D ¯ decays but is disfavored by potential models. It is shown that taking into account the resonance–continuum interference in the near-threshold region affects resonance parameters, thus the results presented cannot be directly compared with the corresponding PDG values obtained ignoring this effect.


Physical Review D | 2014

Study of the processe+e−→nn¯at the VEPP-2000e+e−collider with the SND detector

M. N. Achasov; A.Yu. Barnyakov; K. I. Beloborodov; A. V. Berdyugin; Dmitry Berkaev; A. G. Bogdanchikov; A.A. Botov; T. V. Dimova; V. P. Druzhinin; V. B. Golubev; Leonid Kardapoltsev; A. S. Kasaev; Alexey Kharlamov; A. N. Kirpotin; I. A. Koop; A. A. Korol; S. V. Koshuba; D.P. Kovrizhin; A. S. Kupich; K.A. Martin; A. E. Obrazovsky; E. V. Pakhtusova; Yu.A. Rogovsky; A. I. Senchenko; S. I. Serednyakov; Z. K. Silagadze; Yu. M. Shatunov; D.A. Shtol; Dmitry Shwartz; A.N. Skrinsky

The process


Physics Letters B | 2016

Measurement of R uds and R between 3.12 and 3.72 GeV at the KEDR detector

V.V. Anashin; V. Aulchenko; Evgenii Baldin; A.K. Barladyan; A.Yu. Barnyakov; M.Yu. Barnyakov; S.E. Baru; I.Yu. Basok; A.M. Batrakov; A.E. Blinov; Vladimir Blinov; A. Bobrov; V. S. Bobrovnikov; A.V. Bogomyagkov; A. Bondar; A.A. Borodenko; Aleksey Buzykaev; S. Eidelman; D.N. Grigoriev; Yu.M. Glukhovchenko; S.E. Karnaev; G.V. Karpov; S.V. Karpov; P.V. Kasyanenko; Tatyana Kharlamova; V.A. Kiselev; V.V. Kolmogorov; S.A. Kononov; K.Yu. Kotov; E.A. Kravchenko

e^+e^-\to n\bar{n}


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2002

Test of aerogel counters for the KEDR detector

A.Yu. Barnyakov; M.Yu. Barnyakov; V.S. Bobrovnikov; A. R. Buzykaev; A.F. Danilyuk; F.F Guber; G. M. Kolachev; S.A. Kononov; V.A Krasnov; E. A. Kravchenko; A. B. Kurepin; G.D Minakov; A. P. Onuchin; G.A. Savinov; V.A. Tayursky

has been studied at the VEPP-2000


Physics Letters B | 2017

Measurement of R between 1.84 and 3.05 GeV at the KEDR detector

V.V. Anashin; V. Aulchenko; Evgenii Baldin; A.K. Barladyan; A.Yu. Barnyakov; M.Yu. Barnyakov; S.E. Baru; I.Yu. Basok; A.M. Batrakov; A.E. Blinov; Vladimir Blinov; A. Bobrov; V. S. Bobrovnikov; A.V. Bogomyagkov; A. Bondar; Aleksey Buzykaev; S. Eidelman; D.N. Grigoriev; Yu.M. Glukhovchenko; S.E. Karnaev; G.V. Karpov; S.V. Karpov; P.V. Kasyanenko; Tatyana Kharlamova; V.A. Kiselev; V.V. Kolmogorov; S.A. Kononov; K.Yu. Kotov; E.A. Kravchenko; V. Kudryavtsev

e^+e^-


Physics Letters B | 2010

Measurement of Γee(J/ψ)⋅B(J/ψ→e+e−) and Γee(J/ψ)⋅B(J/ψ→μ+μ−)

V.V. Anashin; V. Aulchenko; Evgenii Baldin; A.K. Barladyan; A.Yu. Barnyakov; M.Yu. Barnyakov; S.E. Baru; I. Bedny; O. Beloborodova; A. E. Blinov; V. E. Blinov; A. Bobrov; V. S. Bobrovnikov; A.V. Bogomyagkov; A. Bondar; D. V. Bondarev; A. R. Buzykaev; S. Eidelman; Yu.M. Glukhovchenko; V.V. Gulevich; D.V. Gusev; S.E. Karnaev; G.V. Karpov; S.V. Karpov; Tatyana Kharlamova; V.A. Kiselev; S.A. Kononov; K.Yu. Kotov; E.A. Kravchenko; V.F. Kulikov

collider with the SND detector in the energy range from threshold up to 2 GeV. As a result of the experiment, the


Physics Letters B | 2010

Measurement of D0 and D + meson masses with the KEDR Detector

V.V. Anashin; V. Aulchenko; Evgenii Baldin; A.K. Barladyan; A.Yu. Barnyakov; M.Yu. Barnyakov; S.E. Baru; I. Bedny; O. Beloborodova; A. E. Blinov; V. E. Blinov; A. Bobrov; V. S. Bobrovnikov; A.V. Bogomyagkov; A. Bondar; D. V. Bondarev; A. R. Buzykaev; S. Eidelman; Yu.M. Glukhovchenko; V.V. Gulevich; D.V. Gusev; S.E. Karnaev; G.V. Karpov; S.V. Karpov; Tatyana Kharlamova; V.A. Kiselev; S.A. Kononov; K.Yu. Kotov; E.A. Kravchenko; V.F. Kulikov

e^+e^-\to n\bar{n}

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M.Yu. Barnyakov

Budker Institute of Nuclear Physics

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S.A. Kononov

Budker Institute of Nuclear Physics

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E. A. Kravchenko

Budker Institute of Nuclear Physics

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A. R. Buzykaev

Budker Institute of Nuclear Physics

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V. Aulchenko

Budker Institute of Nuclear Physics

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V. S. Bobrovnikov

Novosibirsk State University

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V. B. Golubev

Budker Institute of Nuclear Physics

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S. I. Serednyakov

Novosibirsk State University

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A. P. Onuchin

Budker Institute of Nuclear Physics

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S.V. Karpov

Budker Institute of Nuclear Physics

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