N. Grigoryan
Yerevan Physics Institute
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Featured researches published by N. Grigoryan.
Physics of Atomic Nuclei | 2010
Y. Song; A. Margaryan; A. Acha; A. Ahmidouch; D. Androic; A. Asaturyan; R. Asaturyan; Oliver Keith Baker; P. Baturin; F. Benmokhtar; R. Carlini; X. Chen; M. E. Christy; L. Cole; S. Danagoulian; A. Daniel; V. Dharmawardane; K. S. Egiyan; M. Elaasar; R. Ent; H. Fenker; Y. Fujii; M. Furic; L. Gan; D. Gaskell; A. Gasparian; E. F. Gibson; N. Grigoryan; P. Gueye; R. Halkyard
The first measurement of proton, pion, and kaon associated fission of Bi nuclei has been performed in a photon energy range 1. 45 < Eγ < 1. 55 GeV. The fission probabilities are compared with an inclusive fission probabilities obtained with photons, protons and pions. The fission probability of Bi nuclei in coincidence with kaons is 0. 18 ± 0. 06 which is ∼3 times larger than the proton and pion associated fission probabilities and ∼2 times larger than inclusive ones. The kaon associated excess fission events are explained in terms of bound Λ residual states and their weak nonmesonic decays.
Physics of Atomic Nuclei | 2007
N. M. Agababyan; V. V. Ammosov; M. Atayan; N. Grigoryan; H. Gulkanyan; A. A. Ivanilov; Zh. Karamyan; V. A. Korotkov
AbstractThe A dependence of the production of K0 and Λ is investigated for the first time in neutrino-nuclear reactions using the data obtained with the SKAT bubble chamber. An exponential parametrization (∼Aβ) of the particle yields results in
Physics of Atomic Nuclei | 2003
N. M. Agababyan; V. V. Ammosov; M. Atayan; N. Grigoryan; G. R. Gulkanyan; A. A. Ivanilov; Zh. Karamyan; V. A. Korotkov
Physics of Atomic Nuclei | 2011
N. M. Agababyan; V. V. Ammosov; N. Grigoryan; H. Gulkanyan; A. A. Ivanilov; Zh. Karamyan; V. A. Korotkov
\beta _{V^0 }
Physics of Atomic Nuclei | 2011
N. M. Agababyan; V. V. Ammosov; N. Grigoryan; H. Gulkanyan; A. A. Ivanilov; Zh. Karamyan; V. A. Korotkov
Physics of Atomic Nuclei | 2011
N. M. Agababyan; V. V. Ammosov; N. Grigoryan; H. Gulkanyan; A. A. Ivanilov; Zh. Karamyan; V. A. Korotkov
= 0.20 ± 0.05 for V0 particles (K0 and Λ), while for π− mesons the A dependence is much weaker (
Physics of Atomic Nuclei | 2011
N. M. Agababyan; V. V. Ammosov; N. Grigoryan; H. Gulkanyan; Zh. Karamyan; V. A. Korotkov
Physics of Atomic Nuclei | 2011
N. M. Agababyan; V. V. Ammosov; N. Grigoryan; H. Gulkanyan; A. A. Ivanilov; Zh. Karamyan; V. A. Korotkov
\beta _{\pi ^ - }
arXiv: High Energy Physics - Experiment | 2009
N. M. Agababyan; V. V. Ammosov; M. Atayan; N. Grigoryan; H. Gulkanyan; A. A. Ivanilov; Zh. Karamyan; V. A. Korotkov
Physics of Atomic Nuclei | 2007
N. M. Agababyan; V. V. Ammosov; M. Atayan; N. Grigoryan; H. Gulkanyan; Zh. Karamyan; V. A. Korotkov
= 0.068 ± 0.007). A nuclear enhancement of the ratio K0/π− is found; this ratio increases from 0.055 ± 0.013 for vN interactions up to 0.070 ± 0.011 at A ≈ 21 and 0.099 ± 0.011 at A ≈ 45. It is observed that the multiplicity rise of V0 occurs predominantly in the backward hemisphere of the hadronic system. It is shown that the A dependence of the Λ0 and π− yields can be reproduced in the framework of a model incorporating the secondary intranuclear interactions of pions originating from the primary vN interactions.