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Dive into the research topics where Yu.A. Nemilov is active.

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Featured researches published by Yu.A. Nemilov.


Nuclear Physics | 1964

(d, p) stripping reaction and (d, d) elastic scattering on Cr50, Cr52, Cr53, Cr54 and Fe54, Fe56 and Fe57

V.P. Bochin; K.I. Zherebtsova; V.S. Zolotarev; V.A. Komarov; L.V. Krasnov; V.F. Litvin; Yu.A. Nemilov; B.G. Novatsky; Sh. Piskorzh

Abstract A method is described for determining the absolute differential cross sections for reactions using a multi-angle magnetic analyser. The energy spectra and angular distributions of protons from the (d, p) reactions on the targets of enriched Cr50, 52, 53, 54 and Fe54, 55, 57 are studied. Altogether 153 levels of final nuclei are studied, including 48 new ones. The l and Θ2 values are obtained for 93 levels, including 58 new ones. A well-pronounced dependence of the cross sections for the (d, p) reaction on the parameter of the target nucleus symmetry is established. The occupation numbers of the neutron 2p subshell are found from the treatment of the experimental data using the sum rule and the results are compared with other data concerning the the (d, t) reaction. The isobaric spin constant of the nuclear optical potential is estimated by the shift of single-particle neutron levels after the addition of two neutrons.


Nuclear Physics | 1972

Coulomb stripping in 58,62,64Ni(d, p)59,63,65Ni

V.F. Litvin; Yu.A. Nemilov; L.V. Krasnov; K.A. Gridnev; K.I. Zherebtzova; Yu.A. Lakomkin; T.V. Orlova; V.P. Bochin; V.S. Romanov

Abstract The 58,62,64 Ni(d, p) stripping reactions have been studied up to a high excitation energy at an incident deuteron energy of E d = 2.9MeV. The spectroscopic factors (2 J +1) S for some excited states differ from those measured at an incident deuteron energy above the Coulomb barrier. For high excited states these anomalies can be explained by the wrong assignment of l n in previous investigations. For low-lying levels of the residual nuclei, the proton energy exceeds the Coulomb barrier and the anomalies observed are apparently due to multistep stripping.


Nuclear Physics | 1973

Symmetric and asymmetric fission of 226Ra induced by 5 to 15 MeV neutrons

E.A. Zhagrov; I.M. Kuks; Yu.A. Nemilov; Yu. A. Selitskii; V.B. Funstein

Abstract Kinetic energy spectra of fragments in the 5–15 MeV neutron-induced fission of 226 Ra are obtained. The fraction of fragments corresponding to the central peak of the mass yield curve is determined for each neutron energy used. It is shown that at low excitation energies of the 227 Ra compound nucleus precluding second-chance fission the mass yield curve retains its triple-peaked nature. At still lower excitations, near the fission threshold, radium undergoes asymmetric fission, just as the heavier nuclei.


Atomic Energy | 1988

Absolute measurements of the cross section for fission of235U by 1.9-MeV and 2.4-MeV neutrons using the method of time-correlated associated particles

V. A. Kalinin; S. S. Kovalenko; V. N. Kuzmin; Yu.A. Nemilov; L. M. Solin; V. I. Shpakov

This paper presents the results of absolute TCAP measurements of 235U fission cross sections at neutron energies E n of 1.9 and 2.4 MeV. These energy points lie in the range 1-5 MeV, where the existing experimental data have the greatest discrepancy (10% or more) and are in two groups: with higher values of oj and a convex form of the dependence oj (En) and with lower values of oj and a concave form (i.e., the values of the cross sections cannot be brought into agreement by renormalization). The ENDF/BVlibrary estimate that is accepted at the present time is midway between the two. The results of previous TCAP measurements for 2.6-MeV neutrons belong to the group with lower values of aj. In this study, the D(d, n) 3He reaction at a deuteron-beam energy E d = 3 MeV was used to obtain neutrons. The reaction kinematics in this case is such that neutrons of the required energy are emitted into the rear hemisphere and the associated helions are emitted


Atomic Energy | 1986

Cross section of the237Np(n, 2n)236Np(22.5 h) reaction, caused by252Cf spontaneous fission neutrons

E. A. Gromova; S. S. Kovalenko; Yu.A. Nemilov; Yu. A. Selitskii; B. I. Tarler; V. B. Funshtein; V. A. Yakovlev

The authors used the direct method of determining sigma /sub n,2n/ on /sup 252/Cf spontaneous fission neutrons. The cross section of the reaction was measured by means of the relative method using activation threshold detectors with known cross sections for neutrons from the Cf spectrum. A figure shows response functions of various threshold reactions with respect to the spectrum of /sup 252/Cf spontaneous fission neutrons. It was necessary for the authors to determine which of the cross sections contained the larger systematic error.


Atomic Energy | 1986

The long-lived236Np isomer's fission cross section for thermal neutrons

B. N. Belyaev; E. A. Gromova; S. S. Kovalenko; A. V. Lovtsyus; Yu.A. Nemilov; Yu. A. Selitskii; A. V. Stepanov; A. M. Fridkin; V. B. Funshtein; V. A. Yakovlev; V.N. Okolovich; G. A. Petrov

Conflicting findings on the correlations between fission cross section and target-nucleus spin for several nuclei, viz., a large cross section corresponding to a high spin, prompted the authors to verify such a correlation by repeating the measurement of the familiar fission cross section of Np 236 (zeta) by using analogous methods of chemical purification of the substance and identification of the fragments as were used in the case of Np(s) 236.


Atomic Energy | 1985

Measurement of the cross sections of the reaction237Np(n, 2n)236Np (22.5 h) for neutron energies in the range 7–10 MeV

N. V. Kornilov; V. Ya. Baryba; A. V. Balitskii; A. P. Rudenko; B. D. Kuz'minov; O. A. Sal'nikov; E. A. Gromova; S. S. Kovalenko; L. D. Preobrazhenskaya; A. V. Stepanov; Yu.A. Nemilov; Yu. A. Selitskii; B. I. Tarler; V. B. Funshtein; V. A. Yakovlev; Sh. Darotsi; P. Raich; I. Chikai

This paper presents experimental results of the study of the energy dependence of the cross section for the formation of /sup 236/PU in the reaction /sup 237/Np (n, 2n). Together with the results for neutron energies near 14 MeV, they present the possibility for describing this cross section in the entire energy interval of importance for fast reactors. The urgency of a theoretical study of the reaction examined here remains, taking into account the quantum characterisitics of the low-lying levels.


Atomic Energy | 1984

Thermal-neutron fission cross section of the short-lived isomer of236Np

E. A. Gromova; S. S. Kovalenko; Yu.A. Nemilov; Yu. A. Selitskii; A. V. Stepanov; A. M. Fridkin; V. B. Funshtein; V. A. Yakovlev; G. V. Val'skii; G. A. Petrov


Atomic Energy | 1983

Measurements of the cross section of the237Np (n, 2n) reaction at neutron energies of 14.8 MeV

E. A. Gromova; S. S. Kovalenko; Yu.A. Nemilov; L. D. Preobrazhenskaya; Yu. A. Selitskii; B. I. Tarler; Yu. N. Trofimov; V. B. Funshtein; S. V. Khlebnikov


Archive | 1986

Cross section of the ²³â·Np(n,2n) ²³â¶Np(22. 5 h) reaction, caused by ²âµÂ²Cf spontaneous fission neutrons

E. A. Gromova; S. S. Kovalenko; Yu.A. Nemilov; Yu. A. Selitskii; B. I. Tarler

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V.F. Litvin

Saint Petersburg State University

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K.I. Zherebtsova

Saint Petersburg State University

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L.V. Krasnov

Saint Petersburg State University

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V.P. Bochin

Saint Petersburg State University

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Sh. Piskorzh

Saint Petersburg State University

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G. A. Petrov

Petersburg Nuclear Physics Institute

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V.A. Komarov

Saint Petersburg State University

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V.S. Zolotarev

Saint Petersburg State University

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B.G. Novatsky

Saint Petersburg State University

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