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卷 82, 编号 5 (2019)

Nuclei

Industrial Reactor Power Monitoring Using Antineutrino Counts in the DANSS Detector

Alekseev I., Belov V., Brudanin V., Guzeev G., Danilov M., Egorov V., Zhitnikov I., Zinatulina D., Kazartsev S., Kobyakin A., Kuznetsov A., Machikhiliyan I., Medvedev D., Nesterov V., Olshevsky A., Pogorelov N., Ponomarev D., Rozova I., Rumyantseva N., Rusinov V., Samigullin E., Svirida D., Skrobova N., Starostin A., Tarkovsky E., Filosofov D., Fomina M., Khvatov V., Chapaev V., Shevchik Y., Shirchenko M., Shitov Y.

摘要

Detection of antineutrino by the reaction of the inverse β-decay can be used for an independent monitoring of a nuclear reactor power. DANSS detector is located directly under a commercial WWER-1000 reactor and counts up to 5000 antineutrino per day, providing the accuracy of 1.5% in 2 days of the flux measurement. A powerful system of the passive and active shielding in combination with the fine spatial segmentation of the detector allows to diminish the contribution of the background processes to a level, negligible in comparison to the statistical error. The influence of the nuclear fuel composition on the neutrino flux can be accounted for based on the input from the NPP staff.

Physics of Atomic Nuclei. 2019;82(5):415-424
pages 415-424 views

Nuclear Reactions under Irradiation of Deuterated Structures by X Rays

Dalkarov O., Negodaev M., Rusetskii A., Lyakhov B., Tsehosh V., Saunin E., Bolotokov A., Kudriashov I., Famina N.

摘要

Measurements of emission from nuclear reaction products (neutrons and protons) have been carried out appearing in the deuterated structures of textured CVD diamond, palladium, titanium, and zirconium under irradiation with a beam of X rays using independent methods (neutron detector based on He-3 counters, Si surface-barrier semiconductor detectors and CR-39 track detector). The possibility of enhancement of both DD reaction and multi-particle deuterium fusion by the beam of X rays with energy ranging 20–30 keV in solid deuterated targets has been established. Analysis of X-ray fluorescence spectra of the target bombarded by beams of ions has revealed “additional” peaks, the occurrence of which cannot be related to any of the known elements, and requires separate study.

Physics of Atomic Nuclei. 2019;82(5):425-438
pages 425-438 views

Energy Dependence of the Most Stable Nuclei Production in Proton-Induced 238U and 232Th Fission

Khan F.

摘要

Using the available experimental data, production cross sections of the most stable nuclei have been calculated for the proton-induced fission of 238U and 232Th at 12, 20, 35, 50, 96 MeV in case of 238U and at 8, 9.3, 12, 19.55, 32.2, 44.7, 53 MeV for 232Th. The analysis has been carried out for the fission fragment mass ranges corresponding to N/Z ratios in the ranges 1.33 ± 0.09 and 1.32 ± 0.08 for 238U and 232Th respectively. Results have been compared with the ones generated indirectly by employing GEF nuclear reaction code, version 2017/1.1. From the production cross sections point of view, for the same energy, 232Th is found to be a better target than 238U for producing nuclei A around the symmetric mass peak, while 238U comes out to be a better one than 232Th for producing the fission fragments around the asymmetric peaks of the mass distribution.

Physics of Atomic Nuclei. 2019;82(5):439-449
pages 439-449 views

The Perusal of Photofission Fragments Mass Yields for Actinide Isotopes by Systematics Neutron Models

Mehdipour Kaldiani P.

摘要

Three neutron-induced models have been investigated for photofission phenomena. The fission fragment mass yields were calculated for actinide isotopes by three neutron induced models on a logarithm scale and compared with photofission experimental data. The peak-to-valley ratios for photofission of 232Th, 240Pu and 238U were calculated and compared with the photofission experimental works. There are considerable differences between the calculated results and experimental works for photofission of 232Th. Then, the yields of symmetric and asymmetric fission products for photofission of 232Th were calculated. Comparison of the calculation and experimental results showed that this nucleus should be separated from others in formalism. The average light mass (〈AL〉) and heavy mass (〈AH〉) were calculated for photofission of other Actinide isotopes at different excitation energies. At last, the fission fragment mass yields were studied with changing the number of emitted neutrons for those models with comparing to photofission experimental data. From the carried out calculations, it is to see that all models cannot describe the total set of the experimental data on the photofission of Actinide nuclei. This means that it is necessary to revise the basic theoretical representation about the nature of photofission processes in the dependence on the energy, at least.

Physics of Atomic Nuclei. 2019;82(5):450-461
pages 450-461 views

Reduced Probabilities for E1 and E2 Transitions in Alternating-Parity Spectra of Heavy Even—Even Nuclei

Nadirbekov M., Kudiratov S., Temirov F.

摘要

Reduced probabilities for intra/interband E1 and E2 transitions to alternating-parity states of the yrast and first nonyrast bands in 150Nd, 154Sm, 154, 160Gd, and 162, 164Er lantanide and 232Th and 236,238u actinide nuclei are studied. The values calculated for B(E1) and B(E2) are compared with available experimental data. Variations in the surface deformation of nuclei upon a collective excitation are taken into account.

Physics of Atomic Nuclei. 2019;82(5):462-467
pages 462-467 views

Beta Decay of the 134In Nucleus and Properties of N ≥ 81 Odd-Odd Neutron-Rich Indium Isotopes

Isakov V.

摘要

The beta decay of the 134In nucleus, which is a neutron-rich odd-odd nucleus and which has an anomalously long lifetime, is studied in detail, and an attempt is made to determine its ground-state spin on this basis. The 131Cd → 131In beta-decay process is used as a guideline for finding the required matrix element. An analysis of the features of splitting of the \(\left\{\left(\nu 2 f_{7/ 2} \right)^{n_{\text{odd}}},\left(\pi 1 g_{9 / 2}\right)^{-1}\right\}\) neutron-proton configuration, which is the lowest one and which determines properties of the spectrum of the lowest states of indium isotopes, is also performed for 83 ≤ N ≤ 89 in this connection.

Physics of Atomic Nuclei. 2019;82(5):468-476
pages 468-476 views

Cross Sections for Solar-Neutrino Capture by the 76Ge Nucleus and High-Lying Gamow—Teller Resonances

Vyborov A., Inzhechik L., Koroteev G., Lutostansky Y., Tikhonov V., Fazliakhmetov A.

摘要

The cross section σ(Eν) for solar-neutrino capture by the 76Ge nucleus is calculated. The effect of Gamow-Teller resonances on the rate of neutrino capture in the reaction 76Ge (ν, e)76 As is studied. It is shown that the contribution of high-lying Gamow-Teller resonances to the charge-exchange strength function increases the rate of solar-neutrino capture by 25% to 50%, depending on the normalization method and on the inclusion of the quenching effect.

Physics of Atomic Nuclei. 2019;82(5):477-482
pages 477-482 views

Light Neutral Clusters in Supernova Matter

Panov I., Yudin A.

摘要

The role of weakly bound neutral clusters, such as dineutrons and tetraneutrons, in matter of high density and high temperature is discussed. Under such conditions, which are characteristic of core-collapse supernovae, the lifetime of multineutrons may prove to be sufficiently long for them to have a pronounced effect on the formation of the chemical composition. The influence of the multineutron binding energy and other nuclear properties on the magnitude of the effect being considered is examined.

Physics of Atomic Nuclei. 2019;82(5):483-490
pages 483-490 views

Elementary Particles and Fields

Influence of Cosmic-Ray Spectrum and Hadron—Nucleus Interaction Model on the Properties of High-Energy Atmospheric-Neutrino Fluxes

Morozova A., Kochanov A., Sinegovskaya T., Sinegovsky S.

摘要

The neutrino/antineutrino flux ratios (\({\nu _e}/{\overline \nu _e}\) and \({\nu _\mu }/{\overline \nu _\mu }\)) and the flavor ratio \(\left( {{\nu _\mu } + {{\overline \nu }_\mu }} \right)/\left( {{\nu _e} + {{\overline \nu }_e}} \right)\) clearly demonstrate the distinctions between the predictions of hadronic-interaction models for the production spectra of pions and kaons, which are the main sources of atmospheric neutrinos in the region of Eν ≲ 500 TeV. The values of the \({\nu /\overline \nu }\) ratio are sensitive to variations in the π+/π, π/K, and K+/K meson ratios, which are determined by the cross sections for inclusive meson-production processes in hadron-nucleus (hA) collisions; the elemental composition of cosmic rays also exerts influence, through the p/n ratio, on the development of hadronic cascades and on the neutrino ratios. The difference in \({\nu /\overline \nu }\) and in the flavor ratio for a number of hadronic-interaction models is shown on the basis of calculating neutrino fluxes at energies in the range between 102 and 108 GeV. A comparison of the calculated results with new experimental data shows the reliability of this calculation, which, on the whole, reflects correctly the mechanism of atmospheric-neutrino production. The spectra of atmospheric muon neutrinos from calculations based on the Kimel-Mokhov, SIBYLL 2. 1, and EPOS LHC models describe fairly well experimental results. At energies in the range of 1–500 TeV, the curves calculated within these models combined with the Hillas-Gaisser spectrum are close to the best fit to data from measurements in the IceCube experiment.

Physics of Atomic Nuclei. 2019;82(5):491-497
pages 491-497 views

Estimation of the Upper Limit for the Amplitude of the Dipole Anisotropy of the Total Flux of 25-Gev to 1-Tev Cosmic-Ray Electrons and Positrons

Karelin A., Voronov S., .

摘要

Searches for the anisotropy of the total electron and positron fluxes in high-energy galactic cosmic rays are performed. Data collected by the PAMELA magnetic spectrometer from June 2006, when it was launched into Earth’s orbit, to 2016 were used for the respective analysis. The main event selection and a determination of particle arrival directions were accomplished by means of a position-sensitive microstrip calorimeter. A neutron detector was used to suppress additionally the background of protons and nuclei. An analysis of information obtained over a nearly ten-year period of measurements made it possible to set upper limits on the amplitude of the dipole anisotropy of the total electron and positron fluxes for two energy ranges, between 25 and 100 GeV and between 100 GeV and 1 TeV. These results supplement data from other satellite-borne experiments, AMS-02 and Fermi.

Physics of Atomic Nuclei. 2019;82(5):498-502
pages 498-502 views

Affine-Goldstone/Quartet-Metric Gravity and Beyond

Pirogov Y.

摘要

As a group—theoretic foundation of gravity, it is considered an affine-Goldstone nonlinear model based upon the nonlinear realization of the global affine symmetry spontaneously broken at the Planck scale to the Poincaré symmetry. It is shown that below this scale the model justifies and elaborates an earlier introduced effective field theory of the quartet-metric gravity incorporating the gravitational dark substances emerging in addition to the tensor graviton. The prospects for subsequent going beyond the nonlinear model above the Planck scale are indicated.

Physics of Atomic Nuclei. 2019;82(5):503-512
pages 503-512 views

Proceedings of International Conference NUCLEI-2018 (LXVIII International Conference on Nuclear Spectroscopy and Nuclear Structure, Voronezh, Russia, July 2–6, 2018)/Nuclei

Prospects of Development of Radiation Technologies in Russia

Chernyaev A., Varzar S., Belousov A., Zheltonozhskaya M., Lykova E.

摘要

The present review article describes the role of radiation technologies in various realms of human activities, including fundamental science, industry, agriculture, and medicine. The development of radiation technologies in the world and in Russia is compared. The total number of ionizing-radiation sources in the world is approximately 11 million units, most of them being radioactive sources (about six to seven million units) and x-ray facilities (about four million units). The number of high-technology facilities (such as accelerators and tomography units of various types) that employ ionizing radiation does not exceed 200 thousand units. In Russia, there are more than 153 thousand units of such instruments and facilities. They include about 64700 units employing x-ray radiation; about 79700 radioisotope devices and setups, reactors, and radioactive-waste storage facilities; and 471 accelerators. The most promising lines of development of radiation technologies in Russia are analyzed from the strategic and economic points of view.

Physics of Atomic Nuclei. 2019;82(5):513-527
pages 513-527 views

Resonance Structure of the Charge-Exchange Strength Function

Lutostansky Y.

摘要

The resonance structure of the charge-exchange strength function S(E) is studied. Three types of isobaric resonances are considered within the self-consistent theory of finite Fermi systems and within its model approximation. These are giant Gamow-Teller, analog, and pygmy resonances (GTR, AR, and PR, respectively). The energies calculated for GTR, AR and three PRs agree well with experimental data. In heavy nuclei, the energy difference ΔEG-A = EGTREAR tends to zero, which corresponds to restoration of Wigner’s SU(4) symmetry. The average deviation of the calculated values of ΔEG-A from known experimental data for 33 nuclei is 0.30 MeV. The root-mean-square deviations of the calculated energies of pygmy resonances from experimental data are also moderately small, δE < 0.40 MeV. The strength function S(E) is calculated for the isotopes 71Ga, 98Mo, 118Sn, and 127I. The calculated values of the resonance energies and resonance-peak parameters are close to their experimental counterparts. A strong effect of charge-exchange resonances on neutrino-capture cross sections, including those for solar neutrinos, is demonstrated.

Physics of Atomic Nuclei. 2019;82(5):528-536
pages 528-536 views

Description of Continuum States within the No-Core Shell Model: Single-State HORSE Method

Mazur A., Shirokov A., Mazur I., Blokhintsev L., Kim Y., Shin I., Vary J.

摘要

The Single-State HORSE (SS-HORSE) method is applied to studying resonant scattering. The method relies on microscopic calculations of nuclear spectra on the basis of the No-Core Shell Model with realistic nucleon-nucleon interactions and does not involve model approximations. The 3/2 and 1/2 resonances of the 5Li and 5He nuclei are investigated within the SS-HORSE method. The possible existence of a resonance in the four-neutron system is explored.

Physics of Atomic Nuclei. 2019;82(5):537-548
pages 537-548 views

Erratum

Erratum to: Analytic Calculations of the Branching Ratio and CP Violation in \(B_s^0 \to {K^{*0}}{\overline K ^{*0}}\) Decay

Kamal A., Khan H., Alhendi H.

摘要

  1. Page 299, right column, line 7 from the top (1.08 ± 0.21) × 10−5 should read (1.08 ± 0.21(stat.) ± 0.14(syst.) ± 0.06(fd/fs)) × 10−5.

  2. Page 307, Table 4, first column: The phrase in brackets (These values are basically form LHCb result based on two independent measurements. For simplicity, only the statistical errors are cited here.) should be added after “Experimental Value”.

  3. Page 307, Reference [8]: LHCb Collab. (R. Aaij et al.), CERN-PH-EP-2011-183 should read LHCb Collab. (R. Aaij et al.), Phys. Lett. B 709, 50 (2012).

  4. Page 307, Reference [9]: LHCb Collab. (R. Aaij et al.), CERN-PH-EP-2015-058 should read LHCb Collab. (R. Aaij et al.), JHEP 1507, 166 (2015).

  5. Page 307, Reference [10]: C. Wang, Q.-A. Zhang, Y. Li, and C.-D. Lu, Eur. Phys. J. C 77, 33 (2017) should read LHCb Collab. (R. Aaij et al.), JHEP 1803, 140 (2018).

Physics of Atomic Nuclei. 2019;82(5):549-549
pages 549-549 views