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Dive into the research topics where V. N. Shvetsov is active.

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Featured researches published by V. N. Shvetsov.


Science | 2010

Hydrogen mapping of the lunar south pole using the LRO neutron detector experiment LEND.

I. G. Mitrofanov; A. B. Sanin; William V. Boynton; G. Chin; James B. Garvin; D. V. Golovin; Larry G. Evans; K. Harshman; A. S. Kozyrev; M. L. Litvak; A. Malakhov; Erwan Mazarico; Timothy P. McClanahan; G. M. Milikh; M. I. Mokrousov; G. Nandikotkur; Gregory A. Neumann; I. Nuzhdin; R. Z. Sagdeev; V.V. Shevchenko; V. N. Shvetsov; David E. Smith; Richard D. Starr; V. I. Tret'yakov; J. Trombka; D. A. Usikov; A. Varenikov; A. A. Vostrukhin; Maria T. Zuber

Watering the Moon About a year ago, a spent upper stage of an Atlas rocket was deliberately crashed into a crater at the south pole of the Moon, ejecting a plume of debris, dust, and vapor. The goal of this event, the Lunar Crater Observation and Sensing Satellite (LCROSS) experiment, was to search for water and other volatiles in the soil of one of the coldest places on the Moon: the permanently shadowed region within the Cabeus crater. Using ultraviolet, visible, and near-infrared spectroscopy data from accompanying craft, Colaprete et al. (p. 463; see the news story by Kerr; see the cover) found evidence for the presence of water and other volatiles within the ejecta cloud. Schultz et al. (p. 468) monitored the different stages of the impact and the resulting plume. Gladstone et al. (p. 472), using an ultraviolet spectrograph onboard the Lunar Reconnaissance Orbiter (LRO), detected H2, CO, Ca, Hg, and Mg in the impact plume, and Hayne et al. (p. 477) measured the thermal signature of the impact and discovered that it had heated a 30 to 200 square-meter region from ∼40 kelvin to at least 950 kelvin. Paige et al. (p. 479) mapped cryogenic zones predictive of volatile entrapment, and Mitrofanov et al. (p. 483) used LRO instruments to confirm that surface temperatures in the south polar region persist even in sunlight. In all, about 155 kilograms of water vapor was emitted during the impact; meanwhile, the LRO continues to orbit the Moon, sending back a stream of data to help us understand the evolution of its complex surface structures. A controlled spacecraft impact into a crater in the lunar south pole plunged through the lunar soil, revealing water and other volatiles. Hydrogen has been inferred to occur in enhanced concentrations within permanently shadowed regions and, hence, the coldest areas of the lunar poles. The Lunar Crater Observation and Sensing Satellite (LCROSS) mission was designed to detect hydrogen-bearing volatiles directly. Neutron flux measurements of the Moon’s south polar region from the Lunar Exploration Neutron Detector (LEND) on the Lunar Reconnaissance Orbiter (LRO) spacecraft were used to select the optimal impact site for LCROSS. LEND data show several regions where the epithermal neutron flux from the surface is suppressed, which is indicative of enhanced hydrogen content. These regions are not spatially coincident with permanently shadowed regions of the Moon. The LCROSS impact site inside the Cabeus crater demonstrates the highest hydrogen concentration in the lunar south polar region, corresponding to an estimated content of 0.5 to 4.0% water ice by weight, depending on the thickness of any overlying dry regolith layer. The distribution of hydrogen across the region is consistent with buried water ice from cometary impacts, hydrogen implantation from the solar wind, and/or other as yet unknown sources.


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

Identification of a new escape channel for UCN from traps

A. V. Strelkov; V. V. Nesvizhevsky; P. Geltenbort; D. G. Kartashov; A. G. Kharitonov; E. V. Lychagin; A. Yu. Muzychka; J.M. Pendlebury; K. Schreckenbach; V. N. Shvetsov; A. P. Serebrov; R.R Taldaev; P Yaidjiev

Abstract Ultra-cold neutrons (UCN) can be stored in a trap if their energy is lower than the trap wall potential. It is well known that the neutron density in a trap decreases due to neutron beta-decay, upscattering and absorption on surfaces but we have identified a complementary escape channel. This arises from a small increase in the energy of UCN during their interaction with a surface. Higher-energy neutrons can then escape into the bulk material or penetrate through the trap wall if it is thin enough.


Journal of Geophysical Research | 2014

Local variations of bulk hydrogen and chlorine‐equivalent neutron absorption content measured at the contact between the Sheepbed and Gillespie Lake units in Yellowknife Bay, Gale Crater, using the DAN instrument onboard Curiosity

M. L. Litvak; I. G. Mitrofanov; A. B. Sanin; D. Lisov; A. Behar; William V. Boynton; Lauren DeFlores; F. Fedosov; D. V. Golovin; Craig Hardgrove; K. Harshman; I. Jun; A. S. Kozyrev; Ruslan O. Kuzmin; A. Malakhov; Ralph E. Milliken; M. Mischna; Jeffrey Edward Moersch; M. I. Mokrousov; V. N. Shvetsov; Kathryn M. Stack; Richard D. Starr; C. Tate; V. I. Tret'yakov; A. A. Vostrukhin

Data gathered with the Dynamic Albedo of Neutron (DAN) instrument onboard rover Curiosity were analyzed for variations in subsurface neutron flux and tested for possible correlation with local geological context. A special DAN observation campaign was executed, in which 18 adjacent DAN active measurements were acquired every 0.75–1.0 m to search for the variations of subsurface hydrogen content along a 15 m traverse across geologic contacts between the Sheepbed and Gillespie Lake members of the Yellowknife Bay formation. It was found that several subunits in Sheepbed and Gillespie Lake could be characterized with different depth distributions of water-equivalent hydrogen (WEH) and different chlorine-equivalent abundance responsible for the distribution of neutron absorption elements. The variations of the average WEH at the top 60 cm of the subsurface are estimated at up to 2–3%. Chlorine-equivalent neutron absorption abundances ranged within 0.8–1.5%. The largest difference in WEH and chlorine-equivalent neutron absorption distribution is found between Sheepbed and Gillespie Lake.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1989

Preliminary results of neutron lifetime measurements with gravitational UCN trap

A.G. Kharitonov; V.V. Nesvizhevsky; A.P. Serebrov; R.R. Taldaev; V.E. Varlamov; A.V. Vasilyev; V. P. Alfimenkov; V.I. Lushchikov; V. N. Shvetsov; A.V. Strelkov

Abstract The first preliminary results of neutron lifetime measurements with a gravitational UCN trap are presented.


Journal of Physics G | 2002

Direct measurement of the neutron–neutron scattering cross section at the reactor YAGUAR

W.I. Furman; E.V. Lychagin; A. Yu. Muzichka; G.V. Nekhaev; Yu. V. Safronov; A.V. Strelkov; E.I. Sharapov; V. N. Shvetsov; B. G. Levakov; V. I. Litvin; A.E. Lyzhin; Edouard P. Magda; C.R. Howell; G. E. Mitchell; W. Tornow; B. E. Crawford; S. L. Stephenson; C. D. Bowman

We propose to perform the first measurement of the neutron–neutron scattering cross section in the through-channel of the pulsed aperiodic reactor YAGUAR (Snezhinsk, Russia). Such a measurement directly determines the neutron–neutron scattering length, and by comparison with the proton–proton scattering length bears upon the issue of charge symmetry of the nuclear force. The proposed experimental set-up, as well as modelling of the neutron density and of the frequency of neutron–neutron collisions is described. Experimental results are reported on the formation and optimization of the thermal neutron field inside the through-channel of the reactor YAGUAR. The instantaneous value of 1.1 × 1018 cm−2 s−1 obtained for the thermal neutron flux density is large enough to perform the first direct neutron–neutron scattering length measurement.


Cosmic Research | 2010

The first stage of the “BTN-Neutron” space experiment onboard the Russian segment of the International Space Station

V. I. Tret’yakov; I. G. Mitrofanov; Yu. I. Bobronitskii; A. V. Vostrukhin; N. A. Gunko; A. S. Kozyrev; A. V. Krylov; M. L. Litvak; M. Lopez-Alegria; V. I. Lyagushin; A. A. Konovalov; M. P. Korotkov; P. V. Mazurov; M. I. Mokrousov; A. V. Malakhov; I. O. Nuzhdin; S. N. Ponomareva; M. A. Pronin; A. B. Sanin; G. N. Timoshenko; T. M. Tomilina; M. V. Tyurin; A. I. Tsygan; V. N. Shvetsov

The aims and tasks of the space experiment “BTN-Neutron” onboard the Russian segment of the International Space Station are described. The experiment deals with detection of fast and epithermal neutrons, X-rays, and gamma rays. Characteristics and a short description of scientific instrumentation BTN-M1 for this experiment are presented, as well as the first results of operation of the apparatus onboard the station during the first two years of flight.


Journal of Physics G | 2004

Calculations of neutron spectra after neutron–neutron scattering

B. E. Crawford; S. L. Stephenson; C.R. Howell; G. E. Mitchell; W. Tornow; W.I. Furman; E.V. Lychagin; A. Yu. Muzichka; G.V. Nekhaev; A.V. Strelkov; E.I. Sharapov; V. N. Shvetsov

A direct neutron–neutron scattering length, ann, measurement with the goal of 3% accuracy (0.5 fm) is under preparation at the aperiodic pulsed reactor YAGUAR. A direct measurement of ann will not only help resolve conflicting results of ann by indirect means, but also in comparison to the proton–proton scattering length, app, shed light on the charge-symmetry of the nuclear force. We discuss in detail the analysis of the nn-scattering data in terms of a simple analytical expression. We also discuss calibration measurements using the time-of-flight spectra of neutrons scattered on He and Ar gases and the neutron activation technique. In particular, we calculate the neutron velocity and time-of-flight spectra after scattering neutrons on neutrons and after scattering neutrons on He and Ar atoms for the proposed experimental geometry, using a realistic neutron flux spectrum—Maxwellian plus epithermal tail. The shape of the neutron spectrum after scattering is appreciably different from the initial spectrum, due to collisions between thermal–thermal and thermal–epithermal neutrons. At the same time, the integral over the Maxwellian part of the realistic scattering spectrum differs by only about 6 per cent from that of a pure Maxwellian nn-scattering spectrum.


Review of Scientific Instruments | 2016

A comparative study of LaBr3(Ce3+) and CeBr3 based gamma-ray spectrometers for planetary remote sensing applications

A. S. Kozyrev; I. G. Mitrofanov; Alan Owens; F. Quarati; J. Benkhoff; B.N. Bakhtin; F. Fedosov; D. V. Golovin; M. L. Litvak; A. Malakhov; M. I. Mokrousov; I. O. Nuzhdin; A. B. Sanin; V. I. Tret'yakov; A. A. Vostrukhin; G. N. Timoshenko; V. N. Shvetsov; Carlos Granja; T. Slavicek; S. Pospisil

The recent availability of large volume cerium bromide crystals raises the possibility of substantially improving gamma-ray spectrometer limiting flux sensitivities over current systems based on the lanthanum tri-halides, e.g., lanthanum bromide and lanthanum chloride, especially for remote sensing, low-level counting applications or any type of measurement characterized by poor signal to noise ratios. The Russian Space Research Institute has developed and manufactured a highly sensitive gamma-ray spectrometer for remote sensing observations of the planet Mercury from the Mercury Polar Orbiter (MPO), which forms part of ESAs BepiColombo mission. The Flight Model (FM) gamma-ray spectrometer is based on a 3-in. single crystal of LaBr3(Ce(3+)) produced in a separate crystal development programme specifically for this mission. During the spectrometers development, manufacturing, and qualification phases, large crystals of CeBr3 became available in a subsequent phase of the same crystal development programme. Consequently, the Flight Spare Model (FSM) gamma-ray spectrometer was retrofitted with a 3-in. CeBr3 crystal and qualified for space. Except for the crystals, the two systems are essentially identical. In this paper, we report on a comparative assessment of the two systems, in terms of their respective spectral properties, as well as their suitability for use in planetary mission with respect to radiation tolerance and their propensity for activation. We also contrast their performance with a Ge detector representative of that flown on MESSENGER and show that: (a) both LaBr3(Ce(3+)) and CeBr3 provide superior detection systems over HPGe in the context of minimally resourced spacecraft and (b) CeBr3 is a more attractive system than LaBr3(Ce(3+)) in terms of sensitivities at lower gamma fluxes. Based on the tests, the FM has now been replaced by the FSM on the BepiColombo spacecraft. Thus, CeBr3 now forms the central gamma-ray detection element on the MPO spacecraft.


Physics of Particles and Nuclei Letters | 2016

Test facility for nuclear planetology instruments

A. A. Vostrukhin; D. V. Golovin; P. V. Dubasov; A. O. Zontikov; A. S. Kozyrev; A. R. Krylov; V. A. Krylov; M. L. Litvak; A. Malakhov; I. G. Mitrofanov; M. I. Mokrousov; I. D. Ponomarev; A. N. Repkin; A. B. Sanin; G. N. Timoshenko; K. V. Udovichenko; V. N. Shvetsov

An experimental facility for testing and calibrating nuclear planetology instruments has been constructed in partnership between the Space Research Institute (Moscow) and the Joint Institute for Nuclear Research. A model of Martian soil with a size of 3.82 × 3.21 m2 and an overall mass of about 30 t is assembled from silicate glass. Glass is chosen in order to imitate absolutely dry soil close in composition to the Martian one. The heterogeneous model allows one to imitate the average elemental composition of Martian soil in the best possible way by adding layers of the necessary materials to it. Near-surface water ice is simulated by polyethylene layers buried at different depths within the glass model. A portable neutron generator is used as the neutron source for testing active neutron and gamma spectrometers. The facility is radiation-hazardous and is thus equipped with interlock and radiation monitoring systems in accordance with the effective regulations.


Physics of Particles and Nuclei Letters | 2015

Multilayer passive shielding of scintillation detectors based on BGO, NaI(Tl), and stilbene crystals operating in intense neutron fields with an energy of 14.1 MeV

V. M. Bystritsky; V. Valkovic; D.N. Grozdanov; A.O. Zontikov; I.Zh. Ivanov; Yu. N. Kopatch; A. R. Krylov; Yu. N. Rogov; I.N. Ruskov; M.G. Sapozhnikov; V.R. Skoy; V. N. Shvetsov

We discuss the issues related to choosing the optimum type of passive shielding of scintillation detectors based on BGO, NaI(Tl), and stilbene crystals from the direct penetration of neutron radiation with an energy of 14.1 MeV that was emitted isotropically into a solid angle of 4π. A series of experimental measurements of the count-rate suppression factor that may be obtained for the indicated detectors through the use of various shielding filters comprising iron, lead, and borated polyethylene layers with a total thickness not exceeding 50 cm are conducted.

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A. S. Kozyrev

Russian Academy of Sciences

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D. V. Golovin

Russian Academy of Sciences

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M. I. Mokrousov

Russian Academy of Sciences

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M. L. Litvak

Russian Academy of Sciences

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A. A. Vostrukhin

Russian Academy of Sciences

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I. G. Mitrofanov

Russian Academy of Sciences

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A.V. Strelkov

Joint Institute for Nuclear Research

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V. I. Tret'yakov

Russian Academy of Sciences

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A. B. Sanin

Russian Academy of Sciences

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