Higher moments of nucleon spin structure functions in heavy baryon chiral perturbation theory and in a resonance model
Phys.Rev.D69:056004,2004 The third moment $d_2$ of the twist-3 part of the nucleon spin structure function $g_2$ is generalized to arbitrary momentum transfer $Q^2$ and is evaluated in heavy baryon chiral perturbation theory (HBChPT) up to order ${\mathcal{O}}(p^4)$ and in a unitary isobar model (MA...
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creator | Kao, Chung-Wen Drechsel, Dieter Kamalov, Sabit Vanderhaeghen, Marc |
description | Phys.Rev.D69:056004,2004 The third moment $d_2$ of the twist-3 part of the nucleon spin structure
function $g_2$ is generalized to arbitrary momentum transfer $Q^2$ and is
evaluated in heavy baryon chiral perturbation theory (HBChPT) up to order
${\mathcal{O}}(p^4)$ and in a unitary isobar model (MAID). We show how to link
$d_2$ as well as higher moments of the nucleon spin structure functions $g_1$
and $g_2$ to nucleon spin polarizabilities. We compare our results with the
most recent experimental data, and find a good description of these available
data within the unitary isobar model. We proceed to extract the twist-4 matrix
element $f_2$ which appears in the $1/Q^2$ suppressed term in the twist
expansion of the spin structure function $g_1$ for proton and neutron. |
doi_str_mv | 10.48550/arxiv.hep-ph/0312102 |
format | Article |
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function $g_2$ is generalized to arbitrary momentum transfer $Q^2$ and is
evaluated in heavy baryon chiral perturbation theory (HBChPT) up to order
${\mathcal{O}}(p^4)$ and in a unitary isobar model (MAID). We show how to link
$d_2$ as well as higher moments of the nucleon spin structure functions $g_1$
and $g_2$ to nucleon spin polarizabilities. We compare our results with the
most recent experimental data, and find a good description of these available
data within the unitary isobar model. We proceed to extract the twist-4 matrix
element $f_2$ which appears in the $1/Q^2$ suppressed term in the twist
expansion of the spin structure function $g_1$ for proton and neutron.</description><identifier>DOI: 10.48550/arxiv.hep-ph/0312102</identifier><language>eng</language><subject>Physics - High Energy Physics - Phenomenology</subject><creationdate>2003-12</creationdate><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,780,885</link.rule.ids><linktorsrc>$$Uhttps://arxiv.org/abs/hep-ph/0312102$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.1103/PhysRevD.69.056004$$DView published paper (Access to full text may be restricted)$$Hfree_for_read</backlink><backlink>$$Uhttps://doi.org/10.48550/arXiv.hep-ph/0312102$$DView paper in arXiv$$Hfree_for_read</backlink></links><search><creatorcontrib>Kao, Chung-Wen</creatorcontrib><creatorcontrib>Drechsel, Dieter</creatorcontrib><creatorcontrib>Kamalov, Sabit</creatorcontrib><creatorcontrib>Vanderhaeghen, Marc</creatorcontrib><title>Higher moments of nucleon spin structure functions in heavy baryon chiral perturbation theory and in a resonance model</title><description>Phys.Rev.D69:056004,2004 The third moment $d_2$ of the twist-3 part of the nucleon spin structure
function $g_2$ is generalized to arbitrary momentum transfer $Q^2$ and is
evaluated in heavy baryon chiral perturbation theory (HBChPT) up to order
${\mathcal{O}}(p^4)$ and in a unitary isobar model (MAID). We show how to link
$d_2$ as well as higher moments of the nucleon spin structure functions $g_1$
and $g_2$ to nucleon spin polarizabilities. We compare our results with the
most recent experimental data, and find a good description of these available
data within the unitary isobar model. We proceed to extract the twist-4 matrix
element $f_2$ which appears in the $1/Q^2$ suppressed term in the twist
expansion of the spin structure function $g_1$ for proton and neutron.</description><subject>Physics - High Energy Physics - Phenomenology</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2003</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNqNjk0KwjAQhbNxIeoRhAHX1f5YcC-KB3BfpunUBNIkTNJib2-UHsDNPBg-3vuE2Bf58Xyp6_yE_NbTUZHPvDrlVVEWebkW00O_FDEMbiAbA7ge7CgNOQvB63QijzKOTNCPVkbtbID0VoTTDC3ynECpNKMBT5zAFr8QREWOZ0DbfXEEpuAsWklpqSOzFaseTaDdkhtxuN-e10f2s2w86yF1N8m28apZbKv_qA8HXlGJ</recordid><startdate>20031208</startdate><enddate>20031208</enddate><creator>Kao, Chung-Wen</creator><creator>Drechsel, Dieter</creator><creator>Kamalov, Sabit</creator><creator>Vanderhaeghen, Marc</creator><scope>GOX</scope></search><sort><creationdate>20031208</creationdate><title>Higher moments of nucleon spin structure functions in heavy baryon chiral perturbation theory and in a resonance model</title><author>Kao, Chung-Wen ; Drechsel, Dieter ; Kamalov, Sabit ; Vanderhaeghen, Marc</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-arxiv_primary_hep_ph_03121023</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2003</creationdate><topic>Physics - High Energy Physics - Phenomenology</topic><toplevel>online_resources</toplevel><creatorcontrib>Kao, Chung-Wen</creatorcontrib><creatorcontrib>Drechsel, Dieter</creatorcontrib><creatorcontrib>Kamalov, Sabit</creatorcontrib><creatorcontrib>Vanderhaeghen, Marc</creatorcontrib><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Kao, Chung-Wen</au><au>Drechsel, Dieter</au><au>Kamalov, Sabit</au><au>Vanderhaeghen, Marc</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Higher moments of nucleon spin structure functions in heavy baryon chiral perturbation theory and in a resonance model</atitle><date>2003-12-08</date><risdate>2003</risdate><abstract>Phys.Rev.D69:056004,2004 The third moment $d_2$ of the twist-3 part of the nucleon spin structure
function $g_2$ is generalized to arbitrary momentum transfer $Q^2$ and is
evaluated in heavy baryon chiral perturbation theory (HBChPT) up to order
${\mathcal{O}}(p^4)$ and in a unitary isobar model (MAID). We show how to link
$d_2$ as well as higher moments of the nucleon spin structure functions $g_1$
and $g_2$ to nucleon spin polarizabilities. We compare our results with the
most recent experimental data, and find a good description of these available
data within the unitary isobar model. We proceed to extract the twist-4 matrix
element $f_2$ which appears in the $1/Q^2$ suppressed term in the twist
expansion of the spin structure function $g_1$ for proton and neutron.</abstract><doi>10.48550/arxiv.hep-ph/0312102</doi><oa>free_for_read</oa></addata></record> |
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subjects | Physics - High Energy Physics - Phenomenology |
title | Higher moments of nucleon spin structure functions in heavy baryon chiral perturbation theory and in a resonance model |
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