I. Barabanov
Russian Academy of Sciences
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Featured researches published by I. Barabanov.
arXiv: Instrumentation and Detectors | 2017
N. Abgrall; A. Abramov; N. Abrosimov; I. Abt; M. Agostini; M. Agartioglu; A. Ajjaq; S. I. Alvis; F. T. Avignone; X. Bai; M. Balata; I. Barabanov; A. S. Barabash; P. J. Barton; L. Baudis; L. Bezrukov; T. Bode; A. Bolozdynya; D. Borowicz; A. J. Boston; H. Boston; S. T.P. Boyd; R. Breier; V. Brudanin; R. Brugnera; M. Busch; M. Buuck; A. Caldwell; T. S. Caldwell; T. Camellato
The observation of neutrinoless double-beta decay (0νββ) would show that lepton number is violated, reveal that neu-trinos are Majorana particles, and provide information on neutrino mass. A discovery-capable experiment covering the inverted ordering region, with effective Majorana neutrino masses of 15 - 50 meV, will require a tonne-scale experiment with excellent energy resolution and extremely low backgrounds, at the level of ∼0.1 count /(FWHM·t·yr) in the region of the signal. The current generation 76Ge experiments GERDA and the Majorana Demonstrator, utilizing high purity Germanium detectors with an intrinsic energy resolution of 0.12%, have achieved the lowest backgrounds by over an order of magnitude in the 0νββ signal region of all 0νββ experiments. Building on this success, the LEGEND collaboration has been formed to pursue a tonne-scale 76Ge experiment. The collaboration aims to develop a phased 0νββ experimental program with discovery potential at a half-life approaching or at 1028 years, using existing resources as appropriate to expedite physics results.
Physics of Atomic Nuclei | 2006
S. Schönert; I. Abt; Michael F. Altmann; A. M. Bakalyarov; I. Barabanov; C. Bauer; Markus Bauer; Enrico Bellotti; S. Belogurov; S. T. Belyaev; Alessandro Bettini; L. Bezrukov; V. Brudanin; V. P. Bolotsky; A. Caldwell; C. Cattadori; M. V. Chirchenko; Oleg Chkvorets; E. V. Demidova; A. di Vacri; J. Eberth; V. Egorov; E. Farnea; A. M. Gangapshev; J. Gasparro; P. Grabmayr; G. Y. Grigoriev; V. Gurentsov; K. Gusev; W. Hampel
The Germanium Detector Array (GERDA) in the search for neutrinoless ββ decays of 76Ge at LNGS will operate bare germanium diodes enriched in 76Ge in an (optional active) cryogenic fluid shield to investigate neutrinoless ββ decay with a sensitivity of T1/2 > 2 × 1026 yr after an exposure of 100 kg yr. Recent progress includes the installation of the first underground infrastructures at Gran Sasso, the completion of the enrichment of 37.5 kg of germanium material for detector construction, prototyping of low-mass detector support and contacts, and front-end and DAQ electronics, as well as the preparation for construction of the cryogenic vessel and water tank.
Physics of Atomic Nuclei | 2017
I. Barabanov; L. Bezrukov; A. V. Veresnikova; Yu. M. Gavrilyuk; A. M. Gangapshev; V. Yu. Grishina; V. Gurentsov; V. P. Zavarzina; V. V. Kazalov; S. D. Krokhaleva; V. V. Kuz’minov; A. S. Kurlovich; B. K. Lubsandorzhiev; Sultim Lubsandorzhiev; A. K. Mezhokh; V. P. Morgalyuk; P. Yu. Naumov; G. Ya. Novikova; V. B. Petkov; A. M. Pshukov; A. Yu. Sidorenkov; V. V. Sinev; Sh. I. Umerov; E. Yanovich; T. Enquist; P. Kuusiniemi; J. Joutsenvaara; A. Virkajarvi
At the Baksan Neutrino Observatory (Institute for Nuclear Research, Russian Academy of Sciences, Moscow) deployed in the Caucasus mountains, it is proposed to create, at a depth corresponding to 4760 mwe, a large-volume neutrino detector on the basis of a liquid scintillator with a target mass of 10 kt. The detector in question is intended for recording natural fluxes of neutrinos whose energy may be as low as 100MeV. Neutrino fluxes from various sources are considered in the present study, and the expected effect in the proposed detector is estimated. The detector hat is being developed at the Baksan Neutrino Observatorywill become part of the world network of neutrino detectors for studying natural neutrino fluxes.
Instruments and Experimental Techniques | 2017
I. Barabanov; L. Bezrukov; G. Ya. Novikova; E. Yanovich
The light yield in samples of a Nd-loaded scintillator was measured. The scintillator composition differed in the solvent (pseudocumene (PC) and a mixture of PC with linear alkyl benzene), the scintillating dye type (РРО or ВРО), and the Nd concentration. The light yield in the PC (PPO, 1.5 g/L), which was approximately 11500 photons/MeV, was assumed to be the standard. The ionizing-radiation sources were 137Cs, 241Am, and 109Cd radionuclides. It was shown that the light yield in the scintillator with a Nd concentration as high 30 g/L (~3%) in PC made it possible to attain energy resolution at a level of 3% at an energy of 3 MeV (neutrinoless 2β decay of 150Nd).
Physics of Atomic Nuclei | 2010
I. Barabanov; L. Bezrukov; V. Gurentsov; B. L. Zhuykov; S. V. Kianovsky; V. N. Kornoukhov; V. M. Kohanuk; E. Yanovich
The cross sections for the production of the radioactive isotopes 74As, 68Ge, 65Zn, and 60Co in metallic germanium irradiated with 100-MeV protons were measured, the experiments being performed both with germanium of natural isotopic composition and germanium enriched in the isotope 76Ge. The targets were irradiated with a proton beam at the facility for the production of radionuclides at the accelerator of the Institute for Nuclear Research (INR, Moscow). The data obtained will further be used to calculate the background of radioactive isotopes formed by nuclear cascades of cosmic-ray muons in new-generation experiments devoted to searches for the neutrinoless double-beta decay of 76Ge at underground laboratories.
Physics of Atomic Nuclei | 2017
I. Barabanov; L. Bezrukov; A. V. Veresnikova; Yu. M. Gavrilyuk; A. M. Gangapshev; V. Yu. Grishina; V. Gurentsov; V. P. Zavarzina; V. V. Kazalov; S. D. Krokhaleva; V. V. Kuz’minov; A. S. Kurlovich; B. K. Lubsandorzhiev; Sultim Lubsandorzhiev; A. K. Mezhokh; V. P. Morgalyuk; P. Yu. Naumov; G. Ya. Novikova; V. B. Petkov; A. M. Pshukov; A. Yu. Sidorenkov; V. V. Sinev; Sh. I. Umerov; E. Yanovich; T. Enquist; P. Kuusiniemi; J. Joutsenvaara; A. Virkajarvi
A setup for measuring natural-radioactivity backgrounds and ultralow concentrations of the isotope 14C in samples of a liquid organic scintillator was created at the low-background laboratory of the Baksan Neutrino Observatory (Institute for Nuclear Research, Russian Academy of Sciences) at a depth of 4900 mwe. The concentration of the radiocarbon 14C in a sample of a scintillator based on domestically produced linear alkylbenzene was measured, and it was found that 14C/12C (3.3 ± 0.5) × 10−17.
Journal of Physics: Conference Series | 2016
T Enqvist; I. Barabanov; L. Bezrukov; A. M. Gangapshev; Yu. M. Gavrilyuk; V. Yu. Grishina; V. Gurentsov; J. Hissa; J. Joutsenvaara; V. V. Kazalov; S. D. Krokhaleva; Johanna Kutuniva; P. Kuusiniemi; V. V. Kuzminov; A. S. Kurlovich; K. K. Loo; B. K. Lubsandorzhiev; Sultim Lubsandorzhiev; V. P. Morgalyuk; G. Y. Novikova; A. M. Pshukov; V. V. Sinev; M Słupecki; W H Trzaska; Sh. I. Umerov; A. V. Veresnikova; A. Virkajarvi; Y. A. Yanovich; V. P. Zavarzina
We are going to perform a series of measurements where the 14C/12 C ratio will be measured from several liquid scintillator samples with a dedicated setup. The setup is designed with the aim of measuring ratios smaller than 10-18. Measurements take place in two underground laboratories: in the Baksan Neutrino Observatory, Russia and in the Pyhasalmi mine, Finland. In Baksan the measurements started in 2015 and in Pyhasalmi they start in the beginning of 2015. In order to fully understand the operation of the setup and its background contributions a development of simulation packages has also been started. Low-energy neutrino detection with a liquid scintillator requires that the intrinsic 14C content in the liquid is extremely low. In the Borexino CTF detector at Gran Sasso, Italy the 14C/12C ratio of 2 × 10-18 has been achieved being the lowest 14C concentration ever measured. In principle, the older the oil or gas source that the liquid scintillator is derived of and the deeper it situates, the smaller the 14C/12C ratio is supposed to be. This, however, is not generally the case, and the ratio is probably determined by the U and Th content of the local environment.
Physics of Atomic Nuclei | 2010
I. Barabanov; L. Bezrukov; S. V. Kianovsky; V. N. Kornoukhov
The rate of 68Ge production at sea level under the effect of the nuclear component of cosmic rays is calculated. The calculation is based on the experimental values of the cross sections for 68Ge production in natural- and enriched-germanium targets (enrichment in 76Ge) irradiated with high-energy protons. The background from the decays of 68Ge can be a serious problem in new-generation experiments devoted to searches for the 2β0ν decay of 76Ge.
European Physical Journal C | 2014
M. Agostini; M. Allardt; E. Andreotti; A. M. Bakalyarov; I. Barabanov; N. Barros; L. Baudis; C. Bauer; N. Becerici-Schmidt; E. Bellotti; S. Belogurov; S. T. Belyaev; G. Benato; A. Bettini; L. Bezrukov; V. Brudanin; R. Brugnera; A. Caldwell; C. Cattadori; A. Chernogorov; R. Falkenstein; A. D. Ferella; K. Freund; N. Frodyma; A. M. Gangapshev; A. Garfagnini; P. Grabmayr; V. Gurentsov; K. K. Guthikonda; W. Hampel
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2017
V. V. Kuzminov; V. V. Alekseenko; I. Barabanov; R.A. Etezov; A. M. Gangapshev; Yu. M. Gavrilyuk; A. M. Gezhaev; V. V. Kazalov; A. Kh. Khokonov; S. I. Panasenko; S. S. Ratkevich