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Nucleon spin structure, topological susceptibility and the $\eta$' singlet axial vector coupling
The observed small value of the first moment of the polarized nucleon spin structure function g_1 may be interpreted, in the Veneziano--Shore approach, as a suppression of the first moment \chi^\prime(0) of the QCD topological susceptibility. I give an extension of the Witten--Veneziano argument for...
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Lenguaje: | eng |
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1996
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Acceso en línea: | https://dx.doi.org/10.1016/0370-2693(96)01132-X http://cds.cern.ch/record/306453 |
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author | Grunberg, G. |
author_facet | Grunberg, G. |
author_sort | Grunberg, G. |
collection | CERN |
description | The observed small value of the first moment of the polarized nucleon spin structure function g_1 may be interpreted, in the Veneziano--Shore approach, as a suppression of the first moment \chi^\prime(0) of the QCD topological susceptibility. I give an extension of the Witten--Veneziano argument for the U(1) problem, which yields the O(1/N) correction to the N = \infty relation \chi^\prime(0)/F^2_0 = 1 (where F_0 is the \eta^\prime axial vector coupling).The correction, although negative, seems too small to account for the data. I further argue that the (\eta,\eta^\prime)\rightarrow\gamma\gam ma and J/\psi\rightarrow (\eta , \eta^\prime)\gamma decays indicate an enhancement rather than a suppression of F_0. A substantial gluon-like contribution in \langle 0\vert\partial^\mu j^{(0)}_{\mu_5} \vert\gamma\gamma \rangle \vert_{q^2=0},which could parallel a similar one in the corresponding nucleon matrix element,is suggested. |
id | cern-306453 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1996 |
record_format | invenio |
spelling | cern-3064532023-03-14T18:18:52Zdoi:10.1016/0370-2693(96)01132-Xhttp://cds.cern.ch/record/306453engGrunberg, G.Nucleon spin structure, topological susceptibility and the $\eta$' singlet axial vector couplingParticle Physics - PhenomenologyThe observed small value of the first moment of the polarized nucleon spin structure function g_1 may be interpreted, in the Veneziano--Shore approach, as a suppression of the first moment \chi^\prime(0) of the QCD topological susceptibility. I give an extension of the Witten--Veneziano argument for the U(1) problem, which yields the O(1/N) correction to the N = \infty relation \chi^\prime(0)/F^2_0 = 1 (where F_0 is the \eta^\prime axial vector coupling).The correction, although negative, seems too small to account for the data. I further argue that the (\eta,\eta^\prime)\rightarrow\gamma\gam ma and J/\psi\rightarrow (\eta , \eta^\prime)\gamma decays indicate an enhancement rather than a suppression of F_0. A substantial gluon-like contribution in \langle 0\vert\partial^\mu j^{(0)}_{\mu_5} \vert\gamma\gamma \rangle \vert_{q^2=0},which could parallel a similar one in the corresponding nucleon matrix element,is suggested.The observed small value of the first moment of the polarized nucleon spin structure function $g_1$ may be interpreted, in the Veneziano--Shore approach, as a suppression of the first moment $\chi~\prime(0)$ of the QCD topological susceptibility. I give an extension of the Witten--Veneziano argument for the $U(1)$ problem, which yields the $O(1/N)$ correction to the $N = \infty$ relation $\chi~\prime(0)/F~2_0 = 1$ (where $F_0$ is the $\eta~\prime$ axial vector coupling).The correction, although negative, seems too small to account for the data. I further argue that the $(\eta,\eta~\prime)\rightarrow\gamma\gamma$ and $J/\psi\rightarrow (\eta , \eta~\prime)\gamma$ decays indicate an enhancement rather than a suppression of $F_0$. A substantial gluon-like contribution in $\langle 0\vert\partial~\mu j~{(0)}_{\mu_5} \vert\gamma\gamma \rangle \vert_{q~2=0}$,which could parallel a similar one in the corresponding nucleon matrix element,is suggested.The observed small value of the first moment of the polarized nucleon spin structure function $g_1$ may be interpreted, in the Veneziano--Shore approach, as a suppression of the first moment $\chi~\prime(0)$ of the QCD topological susceptibility. I give an extension of the Witten--Veneziano argument for the $U(1)$ problem, which yields the $O(1/N)$ correction to the $N = \infty$ relation $\chi~\prime(0)/F~2_0 = 1$ (where $F_0$ is the $\eta~\prime$ axial vector coupling).The correction, although negative, seems too small to account for the data. I further argue that the $(\eta,\eta~\prime)\rightarrow\gamma\gamma$ and $J/\psi\rightarrow (\eta , \eta~\prime)\gamma$ decays indicate an enhancement rather than a suppression of $F_0$. A substantial gluon-like contribution in $\langle 0\vert\partial~\mu j~{(0)}_{\mu_5} \vert\gamma\gamma \rangle \vert_{q~2=0}$,which could parallel a similar one in the corresponding nucleon matrix element,is suggested.The observed small value of the first moment of the polarized nucleon spin structure function g 1 may be interpreted, in the Veneziano-Shore approach, as a suppression of the first moment χ ′(0) of the QCD topological susceptibility. I give an extension of the Witten-Veneziano argument for the U (1) problem, which yields the O( 1 N ) correction to the N = ∞ relation χ′(0) F 0 2 = 1 (where F 0 is the η′ axial vector coupling). The correction, although negative, seems too small to account for the data. I further argue that the (η, η′) → γγ and J ψ → (η, η′)γ decays indicate an enhancement rather than a suppression of F 0 . A substantial gluon-like contribution in 〈0| ϖ μ j μ 5 (0) | γγ 〉 q 2 =0 , whi parallel a similar one in the corresponding nucleon matrix element, is suggested.hep-ph/9607204CERN-TH-96-161CERN-TH-96-161oai:cds.cern.ch:3064531996-07-01 |
spellingShingle | Particle Physics - Phenomenology Grunberg, G. Nucleon spin structure, topological susceptibility and the $\eta$' singlet axial vector coupling |
title | Nucleon spin structure, topological susceptibility and the $\eta$' singlet axial vector coupling |
title_full | Nucleon spin structure, topological susceptibility and the $\eta$' singlet axial vector coupling |
title_fullStr | Nucleon spin structure, topological susceptibility and the $\eta$' singlet axial vector coupling |
title_full_unstemmed | Nucleon spin structure, topological susceptibility and the $\eta$' singlet axial vector coupling |
title_short | Nucleon spin structure, topological susceptibility and the $\eta$' singlet axial vector coupling |
title_sort | nucleon spin structure, topological susceptibility and the $\eta$' singlet axial vector coupling |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1016/0370-2693(96)01132-X http://cds.cern.ch/record/306453 |
work_keys_str_mv | AT grunbergg nucleonspinstructuretopologicalsusceptibilityandtheetasingletaxialvectorcoupling |