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Bjorken polarized sum rule and infrared-safe QCD couplings
Experimental data obtained for the polarized Bjorken sum rule (BSR) Γ 1 p - n ( Q 2 ) are fitted by using predictions derived within a truncated operator product expansion (OPE) approach to QCD. Four QCD versions are considered: perturbative QCD (pQCD) in the MS ¯ scheme, Analytic Perturbation Theor...
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Published in: | The European physical journal. C, Particles and fields Particles and fields, 2018-12, Vol.78 (12), p.1-25, Article 1002 |
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creator | Ayala, César Cvetič, Gorazd Kotikov, Anatoly V. Shaikhatdenov, Binur G. |
description | Experimental data obtained for the polarized Bjorken sum rule (BSR)
Γ
1
p
-
n
(
Q
2
)
are fitted by using predictions derived within a truncated operator product expansion (OPE) approach to QCD. Four QCD versions are considered: perturbative QCD (pQCD) in the
MS
¯
scheme, Analytic Perturbation Theory (APT), and 2
δ
and 3
δ
analytic QCD versions. In contrast to pQCD, these QCD variants do not have Landau singularities at low positive
Q
2
, which facilitates the fitting procedure significantly. The fitting procedure is applied first to the experimental data of the inelastic part of BSR, and the known elastic contributions are added after the fitting. In general, when 2
δ
and 3
δ
QCD coupling is used the fitted curves give the best results, within the
Q
2
-range of the fit as well as in extended
Q
2
-intervals. When the fitting procedure is applied to the total BSR, i.e., to the sum of the experimental data and the elastic contribution, the quality of the results deteriorates significantly. |
doi_str_mv | 10.1140/epjc/s10052-018-6490-9 |
format | article |
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Γ
1
p
-
n
(
Q
2
)
are fitted by using predictions derived within a truncated operator product expansion (OPE) approach to QCD. Four QCD versions are considered: perturbative QCD (pQCD) in the
MS
¯
scheme, Analytic Perturbation Theory (APT), and 2
δ
and 3
δ
analytic QCD versions. In contrast to pQCD, these QCD variants do not have Landau singularities at low positive
Q
2
, which facilitates the fitting procedure significantly. The fitting procedure is applied first to the experimental data of the inelastic part of BSR, and the known elastic contributions are added after the fitting. In general, when 2
δ
and 3
δ
QCD coupling is used the fitted curves give the best results, within the
Q
2
-range of the fit as well as in extended
Q
2
-intervals. When the fitting procedure is applied to the total BSR, i.e., to the sum of the experimental data and the elastic contribution, the quality of the results deteriorates significantly.</description><identifier>ISSN: 1434-6044</identifier><identifier>EISSN: 1434-6052</identifier><identifier>DOI: 10.1140/epjc/s10052-018-6490-9</identifier><language>eng</language><publisher>Berlin/Heidelberg: Springer Berlin Heidelberg</publisher><subject>Astronomy ; Astrophysics and Cosmology ; Couplings ; Elementary Particles ; Hadrons ; Heavy Ions ; Measurement Science and Instrumentation ; Nuclear Energy ; Nuclear Physics ; Perturbation methods ; Perturbation theory ; Physics ; Physics and Astronomy ; Quantum Field Theories ; Quantum Field Theory ; Regular Article - Theoretical Physics ; Singularities ; String Theory</subject><ispartof>The European physical journal. C, Particles and fields, 2018-12, Vol.78 (12), p.1-25, Article 1002</ispartof><rights>The Author(s) 2018</rights><rights>COPYRIGHT 2018 Springer</rights><rights>The European Physical Journal C is a copyright of Springer, (2018). All Rights Reserved. © 2018. This work is published under http://creativecommons.org/licenses/by/4.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c518t-17c9635745c13df74e75c109442ce1ba0958bca734f11f99a9779a6015cf3c413</citedby><cites>FETCH-LOGICAL-c518t-17c9635745c13df74e75c109442ce1ba0958bca734f11f99a9779a6015cf3c413</cites><orcidid>0000-0003-4564-5796</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://www.proquest.com/docview/2154017583/fulltextPDF?pq-origsite=primo$$EPDF$$P50$$Gproquest$$Hfree_for_read</linktopdf><linktohtml>$$Uhttps://www.proquest.com/docview/2154017583?pq-origsite=primo$$EHTML$$P50$$Gproquest$$Hfree_for_read</linktohtml><link.rule.ids>314,776,780,25732,27903,27904,36991,44569,74873</link.rule.ids></links><search><creatorcontrib>Ayala, César</creatorcontrib><creatorcontrib>Cvetič, Gorazd</creatorcontrib><creatorcontrib>Kotikov, Anatoly V.</creatorcontrib><creatorcontrib>Shaikhatdenov, Binur G.</creatorcontrib><title>Bjorken polarized sum rule and infrared-safe QCD couplings</title><title>The European physical journal. C, Particles and fields</title><addtitle>Eur. Phys. J. C</addtitle><description>Experimental data obtained for the polarized Bjorken sum rule (BSR)
Γ
1
p
-
n
(
Q
2
)
are fitted by using predictions derived within a truncated operator product expansion (OPE) approach to QCD. Four QCD versions are considered: perturbative QCD (pQCD) in the
MS
¯
scheme, Analytic Perturbation Theory (APT), and 2
δ
and 3
δ
analytic QCD versions. In contrast to pQCD, these QCD variants do not have Landau singularities at low positive
Q
2
, which facilitates the fitting procedure significantly. The fitting procedure is applied first to the experimental data of the inelastic part of BSR, and the known elastic contributions are added after the fitting. In general, when 2
δ
and 3
δ
QCD coupling is used the fitted curves give the best results, within the
Q
2
-range of the fit as well as in extended
Q
2
-intervals. When the fitting procedure is applied to the total BSR, i.e., to the sum of the experimental data and the elastic contribution, the quality of the results deteriorates significantly.</description><subject>Astronomy</subject><subject>Astrophysics and Cosmology</subject><subject>Couplings</subject><subject>Elementary Particles</subject><subject>Hadrons</subject><subject>Heavy Ions</subject><subject>Measurement Science and Instrumentation</subject><subject>Nuclear Energy</subject><subject>Nuclear Physics</subject><subject>Perturbation methods</subject><subject>Perturbation theory</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Quantum Field Theories</subject><subject>Quantum Field Theory</subject><subject>Regular Article - Theoretical Physics</subject><subject>Singularities</subject><subject>String Theory</subject><issn>1434-6044</issn><issn>1434-6052</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><sourceid>PIMPY</sourceid><sourceid>DOA</sourceid><recordid>eNqFUU1r3DAUNKWFpmn_QjH01IOzevaTJfWWbNpkIVD6dRZa-cnY9VqOZEPaX19tHRJyCjroMcwM895k2XtgZwDINjT1dhOBMV4WDGRRo2KFepGdAFZY1Al--TAjvs7exNgzxkpk8iT7dNH78JvGfPKDCd1favK4HPKwDJSbscm70QUTqCmicZR_217m1i_T0I1tfJu9cmaI9O7-P81-ffn8c3td3Hy92m3PbwrLQc4FCKvqigvkFqrGCSSRJqYQS0uwN0xxubdGVOgAnFJGCaFMzYBbV1mE6jTbrb6NN72eQncw4Y_2ptP_AR9abcLc2YE0KOXS9qYSDSAi2wtJVtq6BNhTqUTy-rB6TcHfLhRn3fsljCm-LoEjA8FllVhnK6s1yTSdwM_B2PQaOnTWj-S6hJ_zWpSyRHmM-PGJIHFmuptbs8Sodz--P-XWK9cGH2Mg97ASMH0sVB8L1WuhOhWqj4VqlYRiFcYkGFsKj9mfUf4D6JCilQ</recordid><startdate>20181201</startdate><enddate>20181201</enddate><creator>Ayala, César</creator><creator>Cvetič, Gorazd</creator><creator>Kotikov, Anatoly V.</creator><creator>Shaikhatdenov, Binur G.</creator><general>Springer Berlin Heidelberg</general><general>Springer</general><general>Springer Nature B.V</general><general>SpringerOpen</general><scope>C6C</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>ISR</scope><scope>7U5</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>H8D</scope><scope>HCIFZ</scope><scope>L7M</scope><scope>P5Z</scope><scope>P62</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>DOA</scope><orcidid>https://orcid.org/0000-0003-4564-5796</orcidid></search><sort><creationdate>20181201</creationdate><title>Bjorken polarized sum rule and infrared-safe QCD couplings</title><author>Ayala, César ; Cvetič, Gorazd ; Kotikov, Anatoly V. ; Shaikhatdenov, Binur G.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c518t-17c9635745c13df74e75c109442ce1ba0958bca734f11f99a9779a6015cf3c413</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Astronomy</topic><topic>Astrophysics and Cosmology</topic><topic>Couplings</topic><topic>Elementary Particles</topic><topic>Hadrons</topic><topic>Heavy Ions</topic><topic>Measurement Science and Instrumentation</topic><topic>Nuclear Energy</topic><topic>Nuclear Physics</topic><topic>Perturbation methods</topic><topic>Perturbation theory</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Quantum Field Theories</topic><topic>Quantum Field Theory</topic><topic>Regular Article - Theoretical Physics</topic><topic>Singularities</topic><topic>String Theory</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ayala, César</creatorcontrib><creatorcontrib>Cvetič, Gorazd</creatorcontrib><creatorcontrib>Kotikov, Anatoly V.</creatorcontrib><creatorcontrib>Shaikhatdenov, Binur G.</creatorcontrib><collection>SpringerOpen</collection><collection>CrossRef</collection><collection>Gale in Context: Science</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>ProQuest Central (Alumni)</collection><collection>ProQuest Central</collection><collection>Advanced Technologies & Aerospace Database (1962 - current)</collection><collection>ProQuest Central Essentials</collection><collection>AUTh Library subscriptions: ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central</collection><collection>Aerospace Database</collection><collection>SciTech Premium Collection</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>ProQuest Advanced Technologies & Aerospace Database</collection><collection>ProQuest Advanced Technologies & Aerospace Collection</collection><collection>Publicly Available Content (ProQuest)</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>DOAJ Directory of Open Access Journals</collection><jtitle>The European physical journal. C, Particles and fields</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ayala, César</au><au>Cvetič, Gorazd</au><au>Kotikov, Anatoly V.</au><au>Shaikhatdenov, Binur G.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Bjorken polarized sum rule and infrared-safe QCD couplings</atitle><jtitle>The European physical journal. C, Particles and fields</jtitle><stitle>Eur. Phys. J. C</stitle><date>2018-12-01</date><risdate>2018</risdate><volume>78</volume><issue>12</issue><spage>1</spage><epage>25</epage><pages>1-25</pages><artnum>1002</artnum><issn>1434-6044</issn><eissn>1434-6052</eissn><abstract>Experimental data obtained for the polarized Bjorken sum rule (BSR)
Γ
1
p
-
n
(
Q
2
)
are fitted by using predictions derived within a truncated operator product expansion (OPE) approach to QCD. Four QCD versions are considered: perturbative QCD (pQCD) in the
MS
¯
scheme, Analytic Perturbation Theory (APT), and 2
δ
and 3
δ
analytic QCD versions. In contrast to pQCD, these QCD variants do not have Landau singularities at low positive
Q
2
, which facilitates the fitting procedure significantly. The fitting procedure is applied first to the experimental data of the inelastic part of BSR, and the known elastic contributions are added after the fitting. In general, when 2
δ
and 3
δ
QCD coupling is used the fitted curves give the best results, within the
Q
2
-range of the fit as well as in extended
Q
2
-intervals. When the fitting procedure is applied to the total BSR, i.e., to the sum of the experimental data and the elastic contribution, the quality of the results deteriorates significantly.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer Berlin Heidelberg</pub><doi>10.1140/epjc/s10052-018-6490-9</doi><tpages>25</tpages><orcidid>https://orcid.org/0000-0003-4564-5796</orcidid><oa>free_for_read</oa></addata></record> |
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language | eng |
recordid | cdi_doaj_primary_oai_doaj_org_article_199f490a37d14440b78ec8c6211be297 |
source | Springer Nature - SpringerLink Journals - Fully Open Access; Publicly Available Content (ProQuest) |
subjects | Astronomy Astrophysics and Cosmology Couplings Elementary Particles Hadrons Heavy Ions Measurement Science and Instrumentation Nuclear Energy Nuclear Physics Perturbation methods Perturbation theory Physics Physics and Astronomy Quantum Field Theories Quantum Field Theory Regular Article - Theoretical Physics Singularities String Theory |
title | Bjorken polarized sum rule and infrared-safe QCD couplings |
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