Atomic nucleus Coulomb energy and modification of protons

The problem of the experimental determination of the atomic nucleus Coulomb energy is discussed. The expression for the contribution of the proton modification to Coulomb energy is proposed.

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Datum:2001
1. Verfasser: Buki, A.Yu.
Format: Artikel
Sprache:English
Veröffentlicht: Національний науковий центр «Харківський фізико-технічний інститут» НАН України 2001
Schriftenreihe:Вопросы атомной науки и техники
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Online Zugang:http://dspace.nbuv.gov.ua/handle/123456789/78447
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Zitieren:Atomic nucleus Coulomb energy and modification of protons / A.Yu. Buki // Вопросы атомной науки и техники. — 2001. — № 1. — С. 59. — Бібліогр.: 7 назв. — англ.

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spelling irk-123456789-784472015-03-18T03:01:55Z Atomic nucleus Coulomb energy and modification of protons Buki, A.Yu. Nuclear reactions The problem of the experimental determination of the atomic nucleus Coulomb energy is discussed. The expression for the contribution of the proton modification to Coulomb energy is proposed. 2001 Article Atomic nucleus Coulomb energy and modification of protons / A.Yu. Buki // Вопросы атомной науки и техники. — 2001. — № 1. — С. 59. — Бібліогр.: 7 назв. — англ. 1562-6016 PACS: 21.10 Sf. http://dspace.nbuv.gov.ua/handle/123456789/78447 en Вопросы атомной науки и техники Національний науковий центр «Харківський фізико-технічний інститут» НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
topic Nuclear reactions
Nuclear reactions
spellingShingle Nuclear reactions
Nuclear reactions
Buki, A.Yu.
Atomic nucleus Coulomb energy and modification of protons
Вопросы атомной науки и техники
description The problem of the experimental determination of the atomic nucleus Coulomb energy is discussed. The expression for the contribution of the proton modification to Coulomb energy is proposed.
format Article
author Buki, A.Yu.
author_facet Buki, A.Yu.
author_sort Buki, A.Yu.
title Atomic nucleus Coulomb energy and modification of protons
title_short Atomic nucleus Coulomb energy and modification of protons
title_full Atomic nucleus Coulomb energy and modification of protons
title_fullStr Atomic nucleus Coulomb energy and modification of protons
title_full_unstemmed Atomic nucleus Coulomb energy and modification of protons
title_sort atomic nucleus coulomb energy and modification of protons
publisher Національний науковий центр «Харківський фізико-технічний інститут» НАН України
publishDate 2001
topic_facet Nuclear reactions
url http://dspace.nbuv.gov.ua/handle/123456789/78447
citation_txt Atomic nucleus Coulomb energy and modification of protons / A.Yu. Buki // Вопросы атомной науки и техники. — 2001. — № 1. — С. 59. — Бібліогр.: 7 назв. — англ.
series Вопросы атомной науки и техники
work_keys_str_mv AT bukiayu atomicnucleuscoulombenergyandmodificationofprotons
first_indexed 2025-07-06T02:32:36Z
last_indexed 2025-07-06T02:32:36Z
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fulltext ATOMIC NUCLEUS COULOMB ENERGY AND MODIFICATION OF PROTONS A.Yu. Buki National Science Center “Kharkov Institute of Physics and Technology”, Kharkov, Ukraine The problem of the experimental determination of the atomic nucleus Coulomb energy is discussed. The expres- sion for the contribution of the proton modification to Coulomb energy is proposed. PACS: 21.10 Sf. Coulomb energy EC of nucleus (the total electro-stat- ic energy of the interaction of the intranuclear charges) can be determined from calculation relied on the func- tion of density charge distribution in the nucleus ρ(r). Since usually the explicit form of the function ρ(r) fol- lows from any model of nucleus then the calculation of the EC is model in character. The single known equation for Coulomb energy of nucleus expressing this quantity in terms of the experimental data at once can be taken from paper [1]. In the representation of paper [2] this equation has the form EC = e2 π−1{I1 + I2}, (1) I1 ≅ Z2 ∫ ∞ 0 2 d)( qqF , (1a) I2 ≅ ∫ ∞ − 0 22 d)](Z)([ qqGqSin . (1b) Here e is the elementary electric charge, Z is charge number of the nucleus, q is the 3-momentum transfer, F(q) is the longitudinal nuclear form-factor, G(q2) is proton electric form-factor, Sin(q) is longitudinal re- sponse function zero moment (The moment Sin(q), as in [1] and [2], is not normalized on G2(q2)). The equation (1) was practically used in the experi- mental papers [2] and [3], where the EC of the 6Li and 12C nuclei were evaluated. The subsequent measure- ments of the Sin(q) in the region of high momentum show the necessity of the revision of the Eq.(1) interpre- tation. One can see from Eq. (1), the problem of the EC evaluation is that to calculate I1 and I2 integrals. So, it is necessary to have the F2(q)- and Sin(q)-data in the wide momentum region. The F2(q) quickly decreases with elevation of q, that permits to bound the range of necessary F2(q)-data and, consequently, the upper limit of the integral I1 to bound by q ≈ 1.5 Fm−1. In the case q ≥ 2 Fm−1 the electron scat- tering on nucleus is quasi-elastic ones scattering on nu- cleons, and therefore it would be expected that Sin(q) = ZG2(q2) at these momenta. So, the range of the neces- sary Sin(q)-data can be bounded by q ≈ 2 Fm−1. In this approximation the papers [2] and [3] were fulfilled. However, later experiments (e.g. see [4]) performed as high as q ≈ 3 Fm−1 show that even thought the ratio Sin(q)/[ZG2(q2)] = const at q ≥ 2 Fm−1, but it is less than unity and decreases with elevation of the atomic num- ber. This phenomenon may be explained by modifica- tion of all or part nuclear protons, in the result of which the square on the form-factor of such protons g2(q2) < G2(q2) (see [5]). In this case the term ZG2(q2) in Eq.(1b) transforms into some function f(g) to which tends the Sin(q) with elevation of q. In approach of [6] f(g) = Z[(1 − D)G2(q2) + Dg2(q2)], (2) where D is the relative part of modified protons in the nucleus. The contribution of the protons modification in the EC according to Eq.(2) has form ∆EC = ∫ ∞ − 0 2222 2 d)]()([Z π qqgqGDe . (3) Using this equation and results of paper [6], we evaluate that ∆EC > 0 and it equals to 0.04, 0.27, 9.1 MeV for the nuclei 4He, 12C, 208Pb, correspondingly, that accounts for ∼ 5-50 % of the early e2π−1I2 value of the considerable nuclei or 2.5-1 % of the total Coulomb energy EC. Other models of the protons modification (D = 1) show the same order of value ∆EC. The principal conclusion following from analysis of the nucleus Coulomb energy problem is that the accura- cy of the EC determination immediately depends on the accuracy of the f(g) function, i.e. on the validity of our insight about the protons properties in the nucleus. REFERENCES 1. V.D. Efros. Sum rules in the electron scattering by nuclei // Yad. Fiz. 1973, v. 18, p. 1184-1202 (in Russian). 2. A.Yu. Buki et al. Experimental determination of 6Li nucleus coulomb energy. // Yad.Fiz., 1977, v. 25, p. 457-459 (in Russian). 3. A.Yu. Buki et al. Determination of the coulomb en- ergy from electron scattering experiment. “Particles and Nuclei − Tenth International Conference”, Hei- delberg, July 30 -August 3, 1984, v. I, p. A21. 4. A.Yu. Buki et al. Determination of 12C nucleus coulomb energy from electron scattering // Ukr. Fiz. Zhurn, 1985, v. 30. p. 499-501 (in Russian). 5. A. Zghiche et al. Longitudinal and transverse re- sponses in quasi-elastic electron scattering from 208Pb and 4He // Nucl. Phys., 1994, v. A572, p. 513- 559. 6. G. Orlandini and M. Traini. Sum rules for electron- nucleus scattering // Rep. Prog. Phys. 1991, v. 54, p. 257-338. 7. A.Yu. Buki. Coulomb sums and modification of nu- cleons in the atomic nucleus. “Proc. of the 9th Semi- nar Electromagnetic Interactions of Nuclei at Low and Medium Energies”, Moscow (to be published). PROBLEMS OF ATOMIC SCIENCE AND TECHNOLOGY. 2001, № 1. Series: Nuclear Physics Investigations (37), p. 59. 59 National Science Center “Kharkov Institute of Physics and Technology”, Kharkov, Ukraine REFERENCES