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Featured researches published by D.N. Shatilov.


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

Status of the KEDR detector

V.V. Anashin; V. Aulchenko; B.O Baibusinov; V Balashov; E.M Baldin; L.M Barkov; A.K. Barladyan; M.Yu. Barnyakov; S. E. Baru; I. V. Bedny; D.M Beilin; A. E. Blinov; V. E. Blinov; D.V Bondarev; A. Bondar; A. R. Buzykaev; P. Cantoni; A.G. Chilingarov; L.V Dneprovsky; Simon I. Eidelman; D.A. Epifanov; P.L. Frabetti; P.B Gaidarev; V.R. Groshev; Sergei V. Karpov; V.A. Kiselev; S. G. Klimenko; G. M. Kolachev; S.A. Kononov; V. Kozlov

Abstract KEDR is a general-purpose detector for experiments at the VEPP-4M e + e − -collider in the energy range 2 E =2.0– 12 GeV . All detector subsystems (except the aerogel Cherenkov counters) have been installed into the detector at VEPP-4M. Some preliminary data have been taken in the energy region of the J/Ψ meson. The tuning of the detector and the VEPP-4M collider is in progress. Preliminary results on the detector performance are presented. The future experimental program for the KEDR detector is discussed.


Physical Review Letters | 2002

Experimental investigation of high-energy photon splitting in atomic fields

Sh. Zh. Akhmadaliev; G.Ya. Kezerashvili; S. G. Klimenko; R. N. Lee; V. M. Malyshev; A. L. Maslennikov; A. M. Milov; A. I. Milstein; N. Yu. Muchnoi; A.I. Naumenkov; V. S. Panin; Sergey Peleganchuk; G.E. Pospelov; I. Ya. Protopopov; L.V Romanov; A. G. Shamov; D.N. Shatilov; E. A. Simonov; V. M. Strakhovenko; Yu. A. Tikhonov

Data analysis of an experiment in which photon splitting in atomic fields was observed is presented. The experiment was performed at the tagged photon beam of the ROKK-1M facility at the VEPP-4M collider. In the energy region of 120-450 MeV, statistics of 1.6x10(9) photons incident on the BGO target was collected. About 400 candidate photon-splitting events were reconstructed. Within the attained experimental accuracy, the experimental results are consistent with the calculated exact atomic-field cross section. The predictions obtained in the Born approximation differ significantly from the experimental results.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2000

A detailed test of the CsI(Tℓ) calorimeter for BELLE with photon beams of energy between 20 MeV and 5.4 GeV

H. Ikeda; A. Satpathy; B.S. Ahn; V.M. Aulchenko; A. Bondar; B.G. Cheon; T.H. Chu; M. Fukushima; A.Yu. Garmash; H. Hayashii; H.K. Jang; K. Kaneyuki; K. Kazui; G.Ya. Kezerashvili; H. J. Kim; E.V. Kremyanskaya; A. Kuzmin; M.H Lee; K. Miyabayashi; N. Yu. Muchnoi; A.I. Naumenkov; S. Noguchi; C.S. Park; V.G. Popov; I. Ya. Protopopov; Yu.A Pogorelov; L.V Romanov; N.I Root; H. Sagawa; D.N. Shatilov

Abstract The results of a beam test of a prototype of the BELLE CsI(Tl) calorimeter are reported. The test used beams of photons with energies spanning the range from 20 MeV to 5.4 GeV, produced at ROKK-1M facility of the Budker Institute of Nuclear Physics. The single-counter energy-equivalent noise was measured to be ∼200 keV. The design goals for the energy resolution, e.g. 4% at 20 MeV and 1.7% at 5.4 GeV, were achieved using the sum of energy deposits in a 5×5 crystal matrices with a single crystal energy threshold of 0.5 MeV; the summed energy deposit measured in the array corresponds to 97±2% of the incident photon energy over the entire energy range. The average position resolution for 470 MeV energy photons was measured to be 8 mm.


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.


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.


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

Absolute calibration of particle energy at VEPP-4M

V. E. Blinov; A.V. Bogomyagkov; S.E. Karnaev; V.A. Kiselev; B.V. Levichev; Evgeny Levichev; O.I. Meshkov; S. I. Mishnev; A.I. Naumenkov; S.A. Nikitin; I.B. Nikolaev; V.G. Popov; A.A Polunin; I. Ya. Protopopov; D.N. Shatilov; E. A. Simonov; Yu. A. Tikhonov; G.M. Tumaikin

We have started a new series of experiments on a precise measurement of J/Ψ-, Ψ′- mesons and τ-lepton masses at VEPP-4M collider with KEDR detector. Features of the method used for an absolute particle energy calibration based on the resonance depolarization are described.


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

Using the KEDR detector at the VEPP-4M e + e − e + e − collider, we have measured the values of R uds R uds and R at seven points of the center-of-mass energy between 3.12 and 3.72 GeV. The total achieved accuracy is about or better than 3.3% 3.3 % at most of energy points with a systematic uncertainty of about 2.1% 2.1 % . At the moment it is the most accurate measurement of R(s) R ( s ) in this energy range.


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

Abstract Using the KEDR detector at the VEPP-4M e + e − collider, we have determined the values of R at thirteen points of the center-of-mass energy between 1.84 and 3.05 GeV. The achieved accuracy is about or better than 3.9 % at most of the energy points with a systematic uncertainty less than 2.4 % .


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

The products of the electron width of the J/ψJ/ψ meson and the branching fraction of its decays to the lepton pairs were measured using data from the KEDR experiment at the VEPP-4M electron–positron collider. The results are Γee×Γee/Γ=0.3323±0.0064(stat.)±0.0048(syst.) keV,Γee×Γee/Γ=0.3323±0.0064(stat.)±0.0048(syst.) keV, Γee×Γμμ/Γ=0.3318±0.0052(stat.)±0.0063(syst.) keV.Γee×Γμμ/Γ=0.3318±0.0052(stat.)±0.0063(syst.) keV. Their combinations Γee×(Γee+Γμμ)/Γ=0.6641±0.0082(stat.)±0.0100(syst.) keV,Γee×(Γee+Γμμ)/Γ=0.6641±0.0082(stat.)±0.0100(syst.) keV, Γee/Γμμ=1.002±0.021(stat.)±0.013(syst.)Γee/Γμμ=1.002±0.021(stat.)±0.013(syst.) can be used to improve the accuracy of the leptonic and full widths and test leptonic universality. Assuming eμ universality and using the world average value of the lepton branching fraction, we also determine the leptonic Γll=5.59±0.12 keVΓll=5.59±0.12 keV and total Γ=94.1±2.7 keVΓ=94.1±2.7 keV widths of the J/ψJ/ψ meson.The products of the electron width of the J/\psi meson and the branching fraction of its decays to the lepton pairs were measured using data from the KEDR experiment at the VEPP-4M electron-positron collider. The results are \Gamma_{ee}(J/\psi)*Br(J/\psi->e^+e^-)=(0.3323\pm0.0064\pm0.0048) keV, \Gamma_{ee}(J/\psi)*Br(J/\psi->\mu^+\mu^-)=(0.3318\pm0.0052\pm0.0063) keV. Their combinations \Gamma_{ee}\times(\Gamma_{ee}+\Gamma_{\mu\mu})/\Gamma=(0.6641\pm0.0082\pm0.0100) keV, \Gamma_{ee}/\Gamma_{\mu\mu}=1.002\pm0.021\pm0.013 can be used to improve theaccuracy of the leptonic and full widths and test leptonic universality. Assuming e\mu universality and using the world average value of the lepton branching fraction, we also determine the leptonic \Gamma_{ll}=5.59\pm0.12 keV and total \Gamma=94.1\pm2.7 keV widths of the J/\psi meson.

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A.V. Bogomyagkov

Budker Institute of Nuclear Physics

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V.A. Kiselev

Budker Institute of Nuclear Physics

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S.A. Kononov

Budker Institute of Nuclear Physics

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A. Bondar

Novosibirsk State University

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S.E. Karnaev

Budker Institute of Nuclear Physics

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S.V. Karpov

Budker Institute of Nuclear Physics

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V. Aulchenko

Budker Institute of Nuclear Physics

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M.Yu. Barnyakov

Budker Institute of Nuclear Physics

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A.K. Barladyan

Budker Institute of Nuclear Physics

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Evgenii Baldin

Novosibirsk State University

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