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Dive into the research topics where V. F. Yakushev is active.

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Featured researches published by V. F. Yakushev.


Physical Review Letters | 2012

Measurement of the velocity of neutrinos from the CNGS beam with the large volume detector.

N. Agafonova; M. Aglietta; P. Antonioli; V. V. Ashikhmin; G. Bari; Bertoni R; E. Bressan; G. Bruno; Dadykin Vl; W. Fulgione; P. Galeotti; M. Garbini; P. L. Ghia; P. Giusti; E. Kemp; A. Malgin; B. Miguez; A. Molinario; R. Persiani; I. A. Pless; V. G. Ryasny; O. G. Ryazhskaya; O. Saavedra; G. Sartorelli; Shakyrianova Ir; M. Selvi; G. Trinchero; C. Vigorito; V. F. Yakushev; A. Zichichi

We report the measurement of the time of flight of ∼17 GeV ν(μ) on the CNGS baseline (732 km) with the Large Volume Detector (LVD) at the Gran Sasso Laboratory. The CERN-SPS accelerator has been operated from May 10th to May 24th 2012, with a tightly bunched-beam structure to allow the velocity of neutrinos to be accurately measured on an event-by-event basis. LVD has detected 48 neutrino events, associated with the beam, with a high absolute time accuracy. These events allow us to establish the following limit on the difference between the neutrino speed and the light velocity: -3.8 × 10(-6) < (v(ν)-c)/c < 3.1 × 10(-6) (at 99% C.L.). This value is an order of magnitude lower than previous direct measurements.


Astroparticle Physics | 1992

Limits on low-energy neutrino fluxes with the Mont Blanc liquid scintillator detector

M. Aglietta; P. Antonioli; G. Badino; G. Bologna; C. Castagnoli; A. Castellina; V. L. Dadykin; W. Fulgione; P. Galeotti; F. F. Khalchukov; E. V. Korolkova; P. V. Kortchaguin; V. B. Kortchaguin; V. A. Kudryavtsev; A. S. Malguin; L. Periale; V. G. Ryassny; O. G. Ryazhskaya; O. Saavedra; G.C. Trinchero; S. Vernetto; V. F. Yakushev; G. T. Zatsepin

Abstract The LSD liquid scintillation detector has been operating since 1985 as an underground neutrino observatory in the Mont Blanc Laboratory with the main objective of detecting antineutrino bursts from collapsing stars. In August 1988 the construction of an additional lead and borex paraffin shield considerably reduced the radioactive background and increased the sensitivity of the apparatus. In this way the search for steady fluxes of low-energy neutrinos of different flavours through their interactions with free protons and carbon nuclei of the scintillator was made possible. No evidence for a galactic collapse was observed during the whole period of measurement. The corresponding 90% c.l. upper limit on the galactic collapses rate is 0.45 y −1 for a burst duration of ΔT ⩽ 10 s. After analysing the last 3 years data, the following 90% c.l. upper limits on the steady neutrino and antineutrino fluxes were obtained: Φ( \ gn e ) 4 \ gn e s −1 cm −2 9 ⩽ E ν ⩽ 50MeV Φ( \ gn e ) 3 \ gn e s −1 cm −2 20 ⩽ E ν ⩽ 50MeV Φ(ν e ) 3 ν e s −1 cm −2 25 ⩽ E ν ⩽ 50 MeV Φ(ν μ + τ ) 7 ν μ + τ s −1 cm −2 20 ⩽ E ν ⩽ 100 MeV Φ( \ gn μ + τ ) 7 \ gn μ + τ s −1 cm −2 20 ⩽ E ν ⩽ 100 MeV In particular comparing the obtained upper limit on the \ gn e flux for 9 ⩽ E ν ⩽ 20 MeV to the solar ν e flux predicted by the standard solar model in the same range of energy, we can exclude the possibility that more than 6.3% of the solar ν e s flux can change to \ gn e . Finally the first limits on the flux of relic supernova neutrinos of all flavours as a function of the neutrino sea temperature are presented.


Astroparticle Physics | 2005

Study of the effect of neutrino oscillations on the supernova neutrino signal in the LVD detector

N. Yu. Agafonova; M. Aglietta; P. Antonioli; G. Bari; V. V. Boyarkin; G. Bruno; W. Fulgione; P. Galeotti; M. Garbini; P. L. Ghia; P. Giusti; E. Kemp; V. V. Kuznetsov; V. A. Kuznetsov; A. S. Malguin; H. Menghetti; A. Pesci; I.A. Pless; A. Porta; V. G. Ryasny; O. G. Ryazhskaya; O. Saavedra; G. Sartorelli; M. Selvi; C. Vigorito; F. Vissani; L. Votano; V. F. Yakushev; G. T. Zatsepin; A. Zichichi

The LVD detector, located in the INFN Gran Sasso National Laboratory (Italy), studies supernova neutrinos through the interactions with protons and carbon nuclei in the liquid scintillator and interactions with the iron nuclei of the support structure. We investigate the effect of neutrino oscillations in the signal expected in the LVD detector. The MSW effect has been studied in detail for neutrinos travelling through the collapsing star and the Earth. We show that the expected number of events and their energy spectrum are sensitive to the oscillation parameters, in particular to the mass hierarchy and the value of


Il Nuovo Cimento C | 1991

Coincidences among the data recorded by the Baksan, Kamioka and Mont Blanc underground neutrino detectors, and by the Maryland and Rome gravitational-wave detectors during Supernova 1987 A

M. Aglietta; A. Castellina; W. Fulgione; G. Trinchero; S. Vernetto; C. Castagnoli; P. Galeotti; O. Saavedra; E. Amaldi; S. Frasca; G. V. Pallottino; G. Pizzella; P. Rapagnani; F. Ricci; P. Astone; C. Cosmelli; M. Bassan; E. Coccia; I. Modena; P. Bonifazi; Maria Gabriella Castellano; M. Visco; G. Badino; G. Bologna; V. L. Dadykin; F. F. Khalchukov; I. V. Korolkova; P. V. Kortchaguin; V. A. Kudryatzev; A. S. Malguin

\theta_{13}


Physical Review D | 1999

Upper limit on the prompt muon flux derived from the LVD underground experiment

M. Aglietta; B. Alpat; E. D. Alyea; P. Antonioli; G. Badino; G. Bari; M. Basile; V. S. Berezinsky; F. Bersani; M. Bertaina; R. Bertoni; G. Bonoli; A. Bosco; G. Bruni; G. Cara Romeo; C. Castagnoli; A. Castellina; A. Chiavassa; J. Chinellato; L. Cifarelli; F. Cindolo; G. Conforto; A. Contin; V. L. Dadykin; A. De Silva; M. Deutsch; P. Dominici; L. G. Dos Santos; L. Emaldi; R. I. Enikeev

, presently unknown. Finally we discuss the astrophysical uncertainties, showing their importance and comparing it with the effect of neutrino oscillations on the expected signal.


arXiv: Astrophysics | 2002

Effects of neutrino oscillations on the supernova signal in LVD

M. Aglietta; P. Antonioli; G. Bari; C. Castagnoli; W. Fulgione; P. Galeotti; P. L. Ghia; P. Giusti; E. Kemp; A. S. Malguin; G. Nurzia; A. Pesci; P. Picchi; I.A. Pless; V. G. Ryasny; O. G. Ryazhskaya; G. Sartorelli; M. Selvi; C. Vigorito; F. Vissani; L. Votano; V. F. Yakushev; G. T. Zatsepin; A. Zichichi

SummaryThe data recorded with the neutrino detectors at Mont Blanc, Kamioka, Baksan and with the gravitational-wave detectors in Maryland and Rome have been analysed searching for correlations associated with SN 1987 A, without presuming or excluding hypotheses for correlations due to neutrinos and gravitational waves. The statistical analysis has been based on a previous analysis that showed a correlation among Maryland, Rome and Mont Blanc with a probability to be accidental less than 10−5. Independent correlations are found during a period of one or two hours, around the Mont Blanc 5ν burst (2h 52 min 36 s UT), among the various sets of data: Mont Blanc-Baksan with a probability to be accidental of the order ofp∼4·10−3, Mont Blanc-Kamioka withp∼4·10−3, Maryland-Rome-Kamioka withp∼5·10−4, Maryland-Rome-Baksan withp∼5·10−2. It is remarkable that the events from all the neutrino detectors follow the signals from the g.w. detectors by a time of the order of 1/2 or 1 s. At present we will not give a physical interpretation of the observed correlations which have strong statistical significance.


Astroparticle Physics | 1994

Search for fractionally charged particles in the Mont Blanc LSD scintillation detector

M. Aglietta; P. Antonioli; G. Badino; C. Castagnoli; A. Castellina; V. L. Dadykin; W. Fulgione; P. Galeotti; F. F. Khalchukov; E. V. Korolkova; P. V. Kortchaguin; V. B. Kortchaguin; V. A. Kudryavtsev; A. S. Malguin; Giorgio Marchetti; L. Periale; V. G. Ryassny; O. G. Ryazhskaya; O. Saavedra; G.C. Trinchero; S. Vernetto; V. F. Yakushev; G. T. Zatsepin

We present the analysis of the muon events with all muon multiplicities collected during 21804 hours of operation of the first LVD tower. The measured depth-angular distribution of muon intensities has been used to obtain the normalization factor, A, the power index, gamma, of the primary all-nucleon spectrum and the ratio, R_c, of prompt muon flux to that of pi-mesons - the main parameters which determine the spectrum of cosmic ray muons at the sea level. The value of gamma = 2.77 +/- 0.05 (68% C.L.) and R_c<2.0 x 10^-3 (95% C.L.) have been obtained. The upper limit to the prompt muon flux favours the models of charm production based on QGSM and the dual parton model.


Physics of Atomic Nuclei | 2003

Study of single muons with the Large Volume Detector at the Gran Sasso Laboratory

M. Aglietta; E. D. Alyea; P. Antonioli; G. Badino; G. Bari; M. Basile; V. S. Berezinsky; F. Bersani; M. Bertaina; R. Bertoni; G. Bruni; G. Cara Romeo; C. Castagnoli; A. Castellina; A. Chiavassa; J. Chinellato; Luisa Cifarelli; F. Cindolo; A. Contin; V. L. Dadykin; L. G. Dos Santos; R. I. Enikeev; W. Fulgione; P. Galeotti; P. L. Ghia; P. Giusti; F. Gomez; R. Granella; F. Grianti; V.I. Gurentsov

We study the impact of neutrino oscillations on the supernova neutrino signal in the Large Volume Detector (LVD). The number of expected events for a galactic supernova (D=10 kpc) is calculated, assuming neutrino masses and mixing that explain solar and atmospheric neutrino results. The possibility to detect neutrinos in different channels makes LVD sensitive to different scenarios for neutrino properties, such as normal or inverted neutrino mass hierarchy, and/or adiabatic or non adiabatic MSW resonances associated to U(e3). Of particular importance are the charged current reactions on carbon: oscillations increase by almost one order of magnitude the number of events expected from this channel.Abstract We study the impact of neutrino oscillations on the supernova neutrino signal in the Large Volume Detector (LVD). The number of expected events for a galactic supernova ( D = 10 kpc) is calculated, assuming neutrino masses and mixing that explain solar and atmospheric neutrino results. The possibility to detect neutrinos in different channels makes LVD sensitive to different scenarios for ν properties, such as normal or inverted ν mass hierarchy, and/or adiabatic or non adiabatic MSW resonances associated to U e3 . Of particular importance are the charged current (c.c.) reactions on 12 C: oscillations increase by almost one order of magnitude the number of events expected from this channel.


Bulletin of The Russian Academy of Sciences: Physics | 2011

Single and multiple muons and the generation of neutrons in the LVD experiment

N. Yu. Agafonova; V. V. Boyarkin; V. L. Dadykin; E. A. Dobrynina; R. I. Enikeev; A. S. Malgin; O. G. Ryazhskaya; V. G. Ryasny; I. R. Shakiryanova; V. F. Yakushev; G. T. Zatsepin

Abstract An analysis of the events recorded by the Mont Blanc Neutrino Scintillation Detector was performed in order to search for fractionally charged particles with |Q| = 1 3 and |Q| = 2 3 . In a live time of 2378 days, the obtained 90% C. L. upper limits on the fluxes of fractionally charged particles in the core of our detector are Φ(|Q| = 1 3 ) −13 cm −2 s −1 sr −1 and Φ(|Q| = 2 3 ) −13 cm −2 s −1 sr −1 , the best available limits obtained by scintillation counters technique.


Bulletin of The Russian Academy of Sciences: Physics | 2009

The energy spectrum of neutrons produced by cosmic ray muons in LVD

N. Yu. Agafonova; V. V. Boyarkin; V. L. Dadykin; E. A. Dobrynina; R. I. Enikeev; V. V. Kuznetsov; A. S. Malgin; O. G. Ryazhskaya; V. G. Ryasny; V. F. Yakushev; N. M. Sobolevsky

The present study is based on the sample of 2.9×106 single muons observed by the Large Volume Detector (LVD) at the underground Gran Sasso Laboratory during 36 500 live hours from June 1992 to February 1998. We have measured the muon intensity at slant depths from 3 to 20 km w.e. Most events are high-energy downward muons produced by meson decay in the atmosphere. The analysis of these muons has revealed the power index γ of the π and K spectrum: γ=2.76±0.05. The remainders are horizontal muons produced by the neutrino interactions in the rock surrounding the LVD. The value of this flux near 90° is (6.1±2.7)×10−13 cm−2 s−1 sr−1. The results are compared with the Monte Carlo simulations and the world data.

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V. L. Dadykin

Russian Academy of Sciences

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O. G. Ryazhskaya

Russian Academy of Sciences

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G. T. Zatsepin

Russian Academy of Sciences

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O. Saavedra

Istituto Nazionale di Fisica Nucleare

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R. I. Enikeev

Russian Academy of Sciences

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A. S. Malguin

Russian Academy of Sciences

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