Quasielastic electron scattering on ⁶³Cu in the giant resonance energy region

The result of the extraction of the quasielastic part from the electron scattered spectra on ⁶³Cu is reported. The position of the peak maximum was determined for each quasielastic spectrum and the momentum transfer dependence of its shift with respect to the case of scattering on a free nucleon is...

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Опубліковано в: :Вопросы атомной науки и техники
Дата:2009
Автори: Denyak, V.V., Khvastunov, V.M., Paschuk, S.A., Schelin, H.R.
Формат: Стаття
Мова:Англійська
Опубліковано: Національний науковий центр «Харківський фізико-технічний інститут» НАН України 2009
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Онлайн доступ:https://nasplib.isofts.kiev.ua/handle/123456789/111150
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Цитувати:Quasielastic electron scattering on ⁶³Cu in the giant resonance energy region / V.V. Denyak, V.M. Khvastunov, S.A. Paschuk, H.R. Schelin // Вопросы атомной науки и техники. — 2009. — № 3. — С. 24-27. — Бібліогр.: 2 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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author Denyak, V.V.
Khvastunov, V.M.
Paschuk, S.A.
Schelin, H.R.
author_facet Denyak, V.V.
Khvastunov, V.M.
Paschuk, S.A.
Schelin, H.R.
citation_txt Quasielastic electron scattering on ⁶³Cu in the giant resonance energy region / V.V. Denyak, V.M. Khvastunov, S.A. Paschuk, H.R. Schelin // Вопросы атомной науки и техники. — 2009. — № 3. — С. 24-27. — Бібліогр.: 2 назв. — англ.
collection DSpace DC
container_title Вопросы атомной науки и техники
description The result of the extraction of the quasielastic part from the electron scattered spectra on ⁶³Cu is reported. The position of the peak maximum was determined for each quasielastic spectrum and the momentum transfer dependence of its shift with respect to the case of scattering on a free nucleon is presented in the momentum transfer range of q = 0.5...1.2 fm⁻¹. Представлено результат виділення квазіпружної частини перерізу з спектрів розсіяних на ⁶³Cu електронів. У кожному з отриманих квазіпружних спектрів визначено положення максимуму та представлено залежність зсуву його енергетичного положення відносно кінематики розсіяння на вільному нуклоні в диапазоні переданих імпульсів q = 0.5...1.2 фм⁻¹. Представлен результат выделения квазиупругой части сечения из спектров рассеянных на ⁶³Cu электронов. В каждом из полученных квазиупругих спектров определено положение максимума и представлена зависимость сдвига его энергетического положения относительно кинематики рассеяния на свободном нуклоне в диапазоне переданных импульсов q = 0.5...1.2 фм⁻¹.
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fulltext QUASIELASTIC ELECTRON SCATTERING ON 63Cu IN THE GIANT RESONANCE ENERGY REGION V.V. Denyak1∗, V.M. Khvastunov1, S.A. Paschuk2, H.R. Schelin2 1National Science Center ”Kharkov Institute of Physics and Technology”, 61108, Kharkov, Ukraine 2Federal University of Technology - Parana, Curitiba, 80230-901, Brazil (Received May 30, 2008) The result of the extraction of the quasielastic part from the electron scattered spectra on 63Cu is reported. The position of the peak maximum was determined for each quasielastic spectrum and the momentum transfer dependence of its shift with respect to the case of scattering on a free nucleon is presented in the momentum transfer range of q = 0.5 ... 1.2 fm−1. PACS: 25.30.Fj 1. INTRODUCTION The method of the separation of the resonance and quasielastic parts of the spectrum of scattered elec- trons elaborated recently [1] opens possibility to in- vestigate the properties of the qusielastic electron scattering process at small momentums transfer. In this work we are continuing to elaborate the proposed method. The last one was used to obtain the spectra of quasielastically scattered electrons on 63Cu nuclei in the momentum transfer range q = 0.5 ... 1.2 fm−1. Obtained pure quasielastic spectra were analyzed by means of three phenomenological methods to de- termine the position of the quasielastic peak maxi- mum and its shift with respect to the peak of elastic scattering on a proton. 2. EXPERIMENT The spectra under consideration were measured at electron initial energy of E0 = 150 MeV for scatter- ing angles of θ = 39◦ and 46◦and at E0 = 225 MeV in the angular range θ = 34◦ ... 74◦ . The experimental equipment and the procedure used for data processing are described in [1] and ref- erences therein. The principal idea of the method applied consists in the simultaneous multipole analy- sis of the mixture of resonance and quasielastic parts with their subsequent separation in the obtained mul- tipole spectra. 3. QUASIELASTIC SPECTRA The result of such analysis applied to the spectra of scattered on 63Cu electrons is shown in Fig.1. The uncertainty of each point of the reconstructed qua- sielastic cross section should be treated as the confi- dence interval. The points themselves are not statis- tically independent that follows from the reconstruc- tion method. As in the case of 65Cu quasielastic cross section is practically absent at excitations energies below 20 MeV . 4. SHIFT OF THE QUSIELASTIC PEAK ENERGY POSITION The shift (ε0) of the quasielastic peak maximum with respect to that in the kinematics of scattering on a free nucleon at the same momentum transfer was de- termined for each quasielastic spectrum according to the formula: εmax = q2 2M − q2 2AM + ε0, (1) where εmax - the energy position of the quasielastic peak maximum, A - the atomic number of the ele- ment, M - the nucleon mass. To determine the energy position of the quasi- elastic peak maximum the quasiellastic spectra were transformed into spectra with statistically indepen- dent points. The value of the quasielastic cross sec- tion at given energy was determined with Gauss ran- dom number generator considering its value in pri- mary quasielastic spectrum as a maximum of Gauss distribution and the error of this value as a Gauss half-width. As can be seen from Fig.1 in some spectra the reconstruction errors are not small enough to give distinct maximum position. Therefore three differ- ent methods were used to find the quasielastic peak maxim in the transformed spectra. ∗Corresponding author E-mail address: denyak@gmail.com 24 PROBLEMS OF ATOMIC SCIENCE AND TECHNOLOGY, 2009, N3. Series: Nuclear Physics Investigations (51), p.24-27. Fig.1. Differential cross section of scattered electrons. Closed circles - measured spectrum. Open circles - reconstructed quasielastic part of the spectrum. Line - result of the log-normal curve fitting 25 In the first method the peak maximum was ap- proximated by the Gauss function. Taking into con- sideration essential asymmetry of the quasielastic cross section, only points, where this maximum may be located with the probability corresponding to two standard deviations, participated in the fitting process - points between line 1 and line 2 in Fig.2. It means that points that have the upper limit of the error bar lower than the highest bottom limit among all points were excluded from the adjustment. Fig.2. Choice of points for the Gauss function fitting. Numbers 1 and 2 indicates upper and bottom limits of the peak maximum position. Line - result of the log-normal curve fitting In the second method all points of the spectrum par- ticipated in fitting process but the fitting curve was chosen as log-normal function: y = A(1)exp(− ln2( x A(2) ) 2A(3)2 ), (2) where A(1), A(2), A(3) - fitting parameters. As it can be see from Fig. 1 this curve describes the ex- perimental points quite enough. In the third method the Gauss function was also used but only points from the low energy front of the spectrum took part in fitting as it is shown in Fig.3. Fig.3. Choice of points for third method. Line - result of the Gauss function fitting The result of the determination of the energy posi- tion shift is presented in Fig.4. Fist two methods gives similar results and shows distinctly that shift value has maximum at the momentum transferred q ∼ 0.8 ... 1.0 fm−1. The third method doesn’t show such maximum. Fig.4. Sift of the quasielastic peak maximum energy position with respect to that for kinematics of scattering on free nucleon: a) All methods used. Closed circles - Gauss function fitting, open circles - log-normal function fitting, open squares - fitting to the front of spectrum. Curves 1 and 2 - upper and bottom limits correspondingly, obtained from the energy position of the points that participated in the Gauss function fitting. b) Average of three methods 26 In is necessary to mentioned that such dependence of the shift value is based on the idea that quasi- elastic cross section energy dependence has distinct maximum. Such idea is rather probable but was not proved in this momentum transfer region. The value of the shift of quasielastic peak maximum averaged over the hole interval of q is 28.6 ± 0.6 MeV . This value is somewhat smaller than for 65Cu - 25.4 ± 1.6 MeV [1]. According to the investigation presented in [2] it is unlikely that 63Cu and 65Cu has such big difference in ε0. More probably that such difference shows the accuracy of the method of the electron spectrum division into resonance and quasielastic parts. 5. CONCLUSION The carried out investigation shows that as in the case of 65Cu in the excitation energy range 10 ... 30 MeV the quasielastic cross section in consid- erably smaller than that previously used in the stud- ding of giant resonances. There is an indication that the momentum trans- fer dependence of the shift of the quasielastic peak energy position has maximum at q ∼ 0.8 ... 1.0 fm−1. The estimated value of the error of the absolute value of the quasielastic peak shift is about 3 MeV . References 1. V.V. Denyak, V.M. Khvastunov, S.A. Paschuk, H.R. Schelin. Qusielastic Electron Scattering in the Giant-Resonance Energy Region // Physics of Atomic Nuclei. 2007, v.70, p.1985-1990. 2. R.R. Whitney, I Sick, J.R. Ficenec, et al. Quasi- elastic electron scattering //Phys.Rev. 1974, C9, p.2230-2235. КВАЗИУПРУГОЕ РАССЕЯНИЕ ЭЛЕКТРОНОВ НА 63Cu В ОБЛАСТИ ЭНЕРГИЙ ГИГАНТСКИХ РЕЗОНАНСОВ В.В. Деняк, В.М. Хвастунов, С.А. Пащук, У.Р.Счелин Представлен результат выделения квазиупругой части сечения из спектров рассеянных на 63Cu электронов. В каждом из полученных квазиупругих спектров определено положение максимума и представлена зависимость сдвига его энергетического положения относительно кинематики рассеяния на свободном нуклоне в диапазоне переданных импульсов q = 0.5 ... 1.2фм−1. КВАЗIПРУЖНЕ РОЗСIЯННЯ ЕЛЕКТРОНIВ НА 63Cu В ОБЛАСТI ЕНЕРГIЙ ГIГАНТСЬКИХ РЕЗОНАНСIВ В.В. Деняк, В.М. Хвастунов, С.А. Пащук, У.Р.Счелiн Представлено результат видiлення квазiпружної частини перерiзу з спектрiв розсiяних на 63Cu електронiв. У кожному з отриманих квазiпружних спектрiв визначено положення максимуму та пред- ставлено залежнiсть зсуву його енергетичного положення вiдносно кiнематики розсiяння на вiльному нуклонi в диапазонi переданих iмпульсiв q = 0.5 ... 1.2фм−1. 27
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institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
issn 1562-6016
language English
last_indexed 2025-11-30T21:53:07Z
publishDate 2009
publisher Національний науковий центр «Харківський фізико-технічний інститут» НАН України
record_format dspace
spelling Denyak, V.V.
Khvastunov, V.M.
Paschuk, S.A.
Schelin, H.R.
2017-01-08T16:07:17Z
2017-01-08T16:07:17Z
2009
Quasielastic electron scattering on ⁶³Cu in the giant resonance energy region / V.V. Denyak, V.M. Khvastunov, S.A. Paschuk, H.R. Schelin // Вопросы атомной науки и техники. — 2009. — № 3. — С. 24-27. — Бібліогр.: 2 назв. — англ.
1562-6016
PACS: 25.30.Fj
https://nasplib.isofts.kiev.ua/handle/123456789/111150
The result of the extraction of the quasielastic part from the electron scattered spectra on ⁶³Cu is reported. The position of the peak maximum was determined for each quasielastic spectrum and the momentum transfer dependence of its shift with respect to the case of scattering on a free nucleon is presented in the momentum transfer range of q = 0.5...1.2 fm⁻¹.
Представлено результат виділення квазіпружної частини перерізу з спектрів розсіяних на ⁶³Cu електронів. У кожному з отриманих квазіпружних спектрів визначено положення максимуму та представлено залежність зсуву його енергетичного положення відносно кінематики розсіяння на вільному нуклоні в диапазоні переданих імпульсів q = 0.5...1.2 фм⁻¹.
Представлен результат выделения квазиупругой части сечения из спектров рассеянных на ⁶³Cu электронов. В каждом из полученных квазиупругих спектров определено положение максимума и представлена зависимость сдвига его энергетического положения относительно кинематики рассеяния на свободном нуклоне в диапазоне переданных импульсов q = 0.5...1.2 фм⁻¹.
en
Національний науковий центр «Харківський фізико-технічний інститут» НАН України
Вопросы атомной науки и техники
Ядерная физика и элементарные частицы
Quasielastic electron scattering on ⁶³Cu in the giant resonance energy region
Квазіпружне розсіяння електронів на ⁶³Cu в області енергій гігантських резонансів
Квазиупругое рассеяние электронов на ⁶³Cu в области энергий гигантских резонансов
Article
published earlier
spellingShingle Quasielastic electron scattering on ⁶³Cu in the giant resonance energy region
Denyak, V.V.
Khvastunov, V.M.
Paschuk, S.A.
Schelin, H.R.
Ядерная физика и элементарные частицы
title Quasielastic electron scattering on ⁶³Cu in the giant resonance energy region
title_alt Квазіпружне розсіяння електронів на ⁶³Cu в області енергій гігантських резонансів
Квазиупругое рассеяние электронов на ⁶³Cu в области энергий гигантских резонансов
title_full Quasielastic electron scattering on ⁶³Cu in the giant resonance energy region
title_fullStr Quasielastic electron scattering on ⁶³Cu in the giant resonance energy region
title_full_unstemmed Quasielastic electron scattering on ⁶³Cu in the giant resonance energy region
title_short Quasielastic electron scattering on ⁶³Cu in the giant resonance energy region
title_sort quasielastic electron scattering on ⁶³cu in the giant resonance energy region
topic Ядерная физика и элементарные частицы
topic_facet Ядерная физика и элементарные частицы
url https://nasplib.isofts.kiev.ua/handle/123456789/111150
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