CGC/saturation approach: re-visiting the problem of odd harmonics in angular correlations

Abstract In this paper we demonstrate that the selection of events with different multiplicities of produced particles, leads to the violation of the azimuthal angular symmetry, $$\phi \rightarrow \pi - \phi $$ ϕ→π-ϕ . We find for LHC and lower energies, that this violation can be so large for the e...

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Main Authors: E. Gotsman, E. Levin
Format: Article
Language:English
Published: SpringerOpen 2018-09-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-018-6257-3
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spelling doaj-24305c85189b4d4ca341bf2047f066972020-11-25T01:24:04ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522018-09-0178911810.1140/epjc/s10052-018-6257-3CGC/saturation approach: re-visiting the problem of odd harmonics in angular correlationsE. Gotsman0E. Levin1Department of Particle Physics, School of Physics and Astronomy, Raymond and Beverly Sackler Faculty of Exact Science, Tel Aviv UniversityDepartment of Particle Physics, School of Physics and Astronomy, Raymond and Beverly Sackler Faculty of Exact Science, Tel Aviv UniversityAbstract In this paper we demonstrate that the selection of events with different multiplicities of produced particles, leads to the violation of the azimuthal angular symmetry, $$\phi \rightarrow \pi - \phi $$ ϕ→π-ϕ . We find for LHC and lower energies, that this violation can be so large for the events with multiplicities $$n \ge 2 \bar{n}$$ n≥2n¯ , where $$\bar{n}$$ n¯ is the mean multiplicity, that it leads to almost no suppression of $$v_n$$ vn , with odd n. However, this can only occur if the typical size of the dipole in DIS with a nuclear target is small, or $$Q^2 \,>\,Q^2_s\left( A; Y_{\mathrm{min}},b\right) $$ Q2>Qs2A;Ymin,b , where $$Q_s$$ Qs is the saturation momentum of the nucleus at $$Y = Y_{\mathrm{min}}$$ Y=Ymin . In the case of large sizes of dipoles, when $$Q^2 \,<\,Q^2_s\left( A; Y_{\mathrm{min}},b\right) $$ Q2<Qs2A;Ymin,b , we show that $$v_n =0$$ vn=0 for odd n. Hadron-nucleus scattering is discussed.http://link.springer.com/article/10.1140/epjc/s10052-018-6257-3
collection DOAJ
language English
format Article
sources DOAJ
author E. Gotsman
E. Levin
spellingShingle E. Gotsman
E. Levin
CGC/saturation approach: re-visiting the problem of odd harmonics in angular correlations
European Physical Journal C: Particles and Fields
author_facet E. Gotsman
E. Levin
author_sort E. Gotsman
title CGC/saturation approach: re-visiting the problem of odd harmonics in angular correlations
title_short CGC/saturation approach: re-visiting the problem of odd harmonics in angular correlations
title_full CGC/saturation approach: re-visiting the problem of odd harmonics in angular correlations
title_fullStr CGC/saturation approach: re-visiting the problem of odd harmonics in angular correlations
title_full_unstemmed CGC/saturation approach: re-visiting the problem of odd harmonics in angular correlations
title_sort cgc/saturation approach: re-visiting the problem of odd harmonics in angular correlations
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2018-09-01
description Abstract In this paper we demonstrate that the selection of events with different multiplicities of produced particles, leads to the violation of the azimuthal angular symmetry, $$\phi \rightarrow \pi - \phi $$ ϕ→π-ϕ . We find for LHC and lower energies, that this violation can be so large for the events with multiplicities $$n \ge 2 \bar{n}$$ n≥2n¯ , where $$\bar{n}$$ n¯ is the mean multiplicity, that it leads to almost no suppression of $$v_n$$ vn , with odd n. However, this can only occur if the typical size of the dipole in DIS with a nuclear target is small, or $$Q^2 \,>\,Q^2_s\left( A; Y_{\mathrm{min}},b\right) $$ Q2>Qs2A;Ymin,b , where $$Q_s$$ Qs is the saturation momentum of the nucleus at $$Y = Y_{\mathrm{min}}$$ Y=Ymin . In the case of large sizes of dipoles, when $$Q^2 \,<\,Q^2_s\left( A; Y_{\mathrm{min}},b\right) $$ Q2<Qs2A;Ymin,b , we show that $$v_n =0$$ vn=0 for odd n. Hadron-nucleus scattering is discussed.
url http://link.springer.com/article/10.1140/epjc/s10052-018-6257-3
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