Q-dependence of the quasifree peak maximum position in ²Н(e,e')-reaction

The problem of the quasifree peak position of energy spectra at scattering electrons in inclusive ²H(e,e')- reaction is discussed. ε(q) dependence of the lightest deuterium nucleus is investigated. The fitting experimental points are realized by a 6-th power polynomial. It is proposed the new m...

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Published in:Вопросы атомной науки и техники
Date:2002
Main Authors: Krasil’nikov, V.V., Kuplennikov, E.L., Levashov, I.A., Ranyuk, Yu.N.
Format: Article
Language:English
Published: Національний науковий центр «Харківський фізико-технічний інститут» НАН України 2002
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Online Access:https://nasplib.isofts.kiev.ua/handle/123456789/80102
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Cite this:Q-dependence of the quasifree peak maximum position in ²Н(e,e')-reaction / V.V. Krasil’nikov, E.L. Kuplennikov, I.A. Levashov, Yu.N. Ranyuk // Вопросы атомной науки и техники. — 2002. — № 2. — С. 7-8. — Бібліогр.: 4 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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author Krasil’nikov, V.V.
Kuplennikov, E.L.
Levashov, I.A.
Ranyuk, Yu.N.
author_facet Krasil’nikov, V.V.
Kuplennikov, E.L.
Levashov, I.A.
Ranyuk, Yu.N.
citation_txt Q-dependence of the quasifree peak maximum position in ²Н(e,e')-reaction / V.V. Krasil’nikov, E.L. Kuplennikov, I.A. Levashov, Yu.N. Ranyuk // Вопросы атомной науки и техники. — 2002. — № 2. — С. 7-8. — Бібліогр.: 4 назв. — англ.
collection DSpace DC
container_title Вопросы атомной науки и техники
description The problem of the quasifree peak position of energy spectra at scattering electrons in inclusive ²H(e,e')- reaction is discussed. ε(q) dependence of the lightest deuterium nucleus is investigated. The fitting experimental points are realized by a 6-th power polynomial. It is proposed the new method of finding maxima of energy spectra and its errors at the polynomial fitting.
first_indexed 2025-12-07T17:04:14Z
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fulltext Q- DEPENDENCE OF THE QUASIFREE PEAK MAXIMUM POSITION IN 2Н(e,e')- REACTION V.V. Krasil’nikova), E.L. Kuplennikovb), I.A. Levashova), Yu.N. Ranyukb) a)Belgorod State University, Belgorod, Russia e-mail: kras@bsu.edu.ru b) National Science Center “Kharkov Institute of Physics and Technology”, Kharkov, Ukraine The problem of the quasifree peak position of energy spectra at scattering electrons in inclusive 2H(e,e′)- reaction is discussed. ε(q) dependence of the lightest deuterium nucleus is investigated. The fitting experimental points are realized by a 6-th power polynomial. It is proposed the new method of finding maxima of energy spectra and its errors at the polynomial fitting. PACS: 25.30.Fj INTRODUCTION At large momentum transfer q, dominant feature in the inclusive spectrum of electrons inelastically scattered by nuclei is a wide so-called quasielastic or quasifree peak (QFP) resulting from elastic scattering from individual nucleons. Previous experiments have shown that (see for example [1, 2]) the location of the QFP ωmax on light, middle weight and heavy nuclei differs from that of a free nucleon ωеN and shifted to the higher energy loss ωmax > ωеN side at a certain value of ε. The shift value is a specific function of the kinematical conditions of measurement and cannot be explained by the introducing an average nucleon separation energy that must be supplied to knock the nucleon out of the nucleus. The ε(q)- dependence has a minimum in the momentum near the nuclear Fermi momentum and don’t predict saturation at the large values of q. Consequently this shift cannot be directly related to the average nucleon separation energy. There were difficulties in describing the experimental ε (q)- dependences for A ≥ 3 by the different theoretical models. So a logical step toward understanding the observed differences between calculations and actual behavior of the ε(q)- dependences is the investigation of the quasielastic 2H(e,e′) cross section over the same kinematical region in which problems exist in explaining results found for heavier nuclei. First of all the deuteron is the simplest nuclear system consisting of two nucleons. Estimates of a nuclear density show deuteron is a friable formation enough. Therefore, influence of residual interaction effects and dynamical short-range NN- correlations that grow with increasing nuclear density must be minimum. Besides, weak nucleons couple in deuterium allows considering their as free particles in a certain approximation, which facilitates the theoretical interpretation of the experimental data. RESULTS AND DISCUSSIONS In this work the experimental data are analyzed and the transfer momentum dependence is obtained for the shift of the quasifree peak maximum position on the 2Н nucleus relatively elastic eN- peak location. The energy spectra were taken at the Bates Linear Accelerator Center [3, 4]. The inclusive differential cross section was measured with high accuracy for different initial electron energies and scattering angles of 600 and 134,5° . All data presented have been corrected for radiative effects. We have analyzed five energy spectra inelastically scattered electrons from the deuteron in the quasifree peak region at initial energies Еi = (292,8±0,4; 366,0±0,6; 465,3±0,7; 510,2±0,8; 596,8±0,9) МeV and scattering angle 60°. The shift value of the QFP maximum position in 2Н(е,е′)- reaction relative to the point corresponding to free eN- kinematics is determined as ε = ωmax - ωеN. As the peak on a free proton wasn’t measured in the experiments [2, 3] and the initial electron energy is determined independently, the kinetic energy ωeN of a recoil nucleon with its error dωeN for every concrete spectrum are calculated as ωeN = Ei - EH, where EH = Ei/(1+2Ei/M Sin2 (θ/2)), M is a nucleon mass, at the given value of the initial energy (Ei ± dEi) and the scattering angle θ. The most value of the absolute error ± dε is calculated by the standard procedure of finding errors. To increase precision of finding transferred energy in QFP maximum and to decrease a fit error that, in particular, is determined by a number of the points for fitting and a fit function form the points are taken only in vicinity of the spectrum maximum. Beforehand, the control of a finished result dependence on the fit function form was fulfilled. On Fig.1, it is shown the fitting ought to the polynomial of 6-th power for one of the spectra. It is seen that the plot describes well the spectrum in the QFP maximum region. It is proposed a new method for the maximum and its error to be found in the fitting by a 6-th power PROBLEMS OF ATOMIC SCIENCE AND TECHNOLOGY. 2002, № 2. Series: Nuclear Physics Investigations (40), p. 7-8. 7 polynomial. The method can be shortly described by the following way. As the polynomial coefficients are determined with their errors, it is possible to draw the polynomial curves very much through experimental points. So the control experimental points (xi, yi) with their errors dyi are taken for limiting the 6-th power polynomial set. We select only the polynomials values of which must be equal yi ± dyi in point xi. The maximums of different polynomials with the coefficients within the errors of the initial polynomial are found. The polynomial coefficients are picked up at random. The more a number of the polynomials, the more accurate the result we get. Among the maxima of these random polynomials, we select two ones: one with the most low maximum value x1max and another with the highest value x2max. The required maximum xmax is the arithmetical mean of these two numbers. The absolute value of difference of xmax and x1max (or xmax and x2max) is taken as the error of xmax. The polynomial maxima are found by the method of half dividing. Fig. 1. The dependence of 2Н(е,е′)- reaction cross section on transferred energy. ■ is experimental points for Еi = 292,8 MeV, θ = 60°. The plot is fitting by the 6- th power polynomial The analysis results of the experimental data at the angle 60° are represented on Fig. 2 and in the table. The Kinematical conditions and results of analysis Еi, MeV ωmax, MeV ωеN, MeV ε, MeV q, Fm-1 292,8±0,4 40,9±0,5 39,5±0,5 1,37±0,71 1,39 366,0±0,5 60,6±0,2 59,7±0,7 0,86±0,70 1,72 465,3±0,7 94,5±0,3 92,5±0,8 2,01±0,87 2,16 510,2±0,8 111,9±0,4 109,1±0,9 2,83±0,97 2,35 596,8±0,9 146,9±1,0 144,0±1,0 2,93±1,47 2,73 error of the quantity ε takes into account the measurement error of the initial energy, the fitting error and the error of finding the quantity ωeN. From Fig. 2, it is seen well dynamics of the QFP maximum shift in 2Н(е,е′)- reaction relative to the peak of the elastic еN- scattering in dependence on the kinematical conditions of measurement. As seen from Fig. 2, polynomial fitting experimental data points out that the shift quantity ε increases from the value 1,37 up to 2,93 MeV with increasing transferred momentum in the interval 1,39- 2,73 Fm-1. No obvious anomaly like a minimum appears at low energy loss. Nevertheless, the final result is considered not to be completely determined because of a low number of the investigated spectra and the relatively high experimental errors. The available data are failed for conclusion to be reliable on behaving the investigated dependence on the kinematical conditions of measurement. Fig. 2. The QFP maximum shift dependence for 2Н nucleus relative to the peak of the elastic eN- scattering on transferred 3- momentum. The scattering angle is θ = 60°.  is the experimental points at fitting QFP by the 6-th polynomial. The straight line is the result of the linear fitting CONCLUSIONS The shift of the QFP maximum relatively elastic eN- kinematic increases from the value 1,37 up to 2,93 MeV with increasing transferred momentum in the interval 1,39-2,73 Fm-1. The shift cannot be directly related to the average nucleon separation energy. Specific behavior of the ε(q)- dependence for deuterium may indicate that another process is competing with the single nucleon knockout process and altering the perceived quasielastic peak location. In order that progress be made in the solution of the problem additional experimental investigations over a large range of momentum transfer and modern theoretical calculations are need. REFERENCES 1. J.S. O’Connel, B. Schroder. Quasifree Electron Scattering on Nucleons in a Momentum-Dependent Potential // Phys. Rev. 1988, v. C38, №5, p. 2447- 2449. 2. E.L. Kuplennikov, A.Yu. Korchin, A.V. Shebeko To Question on Maximum Position of Quasfree Peak in (е, е')- Reaction on Atom Nuclei // Yadern. Fiz. 1984, v. 39, is. 4, p. 1047-1049 (in Russian). 3. S.A. Ditman, A.M. Bernstein, K.I. Blomqvist et al. Inclusive Electron Scattering from 2H, 3He and 4He // Phys. Rev. 1988, v. C38, №2, p. 800-812. 4. B.P. Quinn, A.M. Bernstein, K.I. Blomqvist et al. Measurements of Total and Separated Response 8 9 Functions of the Deuteron Through the Quasi- Elastic Peak Region for q∼300 - 500 MeV/c // Phys. Rev. 1988, v. C37, № 4, p. 1609-1623. 9
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institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
issn 1562-6016
language English
last_indexed 2025-12-07T17:04:14Z
publishDate 2002
publisher Національний науковий центр «Харківський фізико-технічний інститут» НАН України
record_format dspace
spelling Krasil’nikov, V.V.
Kuplennikov, E.L.
Levashov, I.A.
Ranyuk, Yu.N.
2015-04-11T19:09:05Z
2015-04-11T19:09:05Z
2002
Q-dependence of the quasifree peak maximum position in ²Н(e,e')-reaction / V.V. Krasil’nikov, E.L. Kuplennikov, I.A. Levashov, Yu.N. Ranyuk // Вопросы атомной науки и техники. — 2002. — № 2. — С. 7-8. — Бібліогр.: 4 назв. — англ.
1562-6016
PACS: 25.30.Fj
https://nasplib.isofts.kiev.ua/handle/123456789/80102
The problem of the quasifree peak position of energy spectra at scattering electrons in inclusive ²H(e,e')- reaction is discussed. ε(q) dependence of the lightest deuterium nucleus is investigated. The fitting experimental points are realized by a 6-th power polynomial. It is proposed the new method of finding maxima of energy spectra and its errors at the polynomial fitting.
en
Національний науковий центр «Харківський фізико-технічний інститут» НАН України
Вопросы атомной науки и техники
Nuclear reactions
Q-dependence of the quasifree peak maximum position in ²Н(e,e')-reaction
Q-зависимость положения максимума квазиупругого пика в ²Н(е,е')-реакции
Article
published earlier
spellingShingle Q-dependence of the quasifree peak maximum position in ²Н(e,e')-reaction
Krasil’nikov, V.V.
Kuplennikov, E.L.
Levashov, I.A.
Ranyuk, Yu.N.
Nuclear reactions
title Q-dependence of the quasifree peak maximum position in ²Н(e,e')-reaction
title_alt Q-зависимость положения максимума квазиупругого пика в ²Н(е,е')-реакции
title_full Q-dependence of the quasifree peak maximum position in ²Н(e,e')-reaction
title_fullStr Q-dependence of the quasifree peak maximum position in ²Н(e,e')-reaction
title_full_unstemmed Q-dependence of the quasifree peak maximum position in ²Н(e,e')-reaction
title_short Q-dependence of the quasifree peak maximum position in ²Н(e,e')-reaction
title_sort q-dependence of the quasifree peak maximum position in ²н(e,e')-reaction
topic Nuclear reactions
topic_facet Nuclear reactions
url https://nasplib.isofts.kiev.ua/handle/123456789/80102
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