Next-to-leading-order correction to pion form factor in k{sub T} factorization
We calculate the next-to-leading-order (NLO) correction to the pion electromagnetic form factor at leading twist in the k{sub T} factorization theorem. Partons off-shell by k{sub T}{sup 2} are considered in both quark diagrams and effective diagrams for the transverse-momentum-dependent pion wave fu...
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Veröffentlicht in: | Physical review. D, Particles and fields Particles and fields, 2011-03, Vol.83 (5) |
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creator | Li Hsiangnan Department of Physics, National Cheng-Kung University, Tainan, Taiwan 701 Department of Physics, National Tsing-Hua University, Hsinchu, Taiwan 300 Shen Yuelong College of Information Science and Engineering, Ocean University of China, Qingdao, Shandong 266100 Wang Yuming Institute of High Energy Physics and Theoretical Physics Center for Science Facilities, Post Office Box 918 Zou Hao |
description | We calculate the next-to-leading-order (NLO) correction to the pion electromagnetic form factor at leading twist in the k{sub T} factorization theorem. Partons off-shell by k{sub T}{sup 2} are considered in both quark diagrams and effective diagrams for the transverse-momentum-dependent pion wave function. The light-cone singularities in the transverse-momentum-dependent pion wave function are regularized by rotating the Wilson lines away from the light cone. The soft divergences from gluon exchanges among initial- and fal-state partons cancel exactly. We derive the infrared-finite k{sub T}-dependent NLO hard kernel for the pion electromagnetic form factor by taking the difference of the above two sets of diagrams. Varying the renormalization and factorization scales, we find that the NLO correction is smaller, when both the scales are set to the invariant masses of internal particles: it becomes lower than 40% of the leading-order contribution for momentum transfer squared Q{sup 2}>7 GeV{sup 2}. It is observed that the NLO leading-twist correction does not play an essential role in explaining the experimental data, but the leading-order higher-twist contribution does. |
doi_str_mv | 10.1103/PHYSREVD.83.054029 |
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fullrecord | <record><control><sourceid>osti</sourceid><recordid>TN_cdi_osti_scitechconnect_21537434</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>21537434</sourcerecordid><originalsourceid>FETCH-LOGICAL-o113t-217089c3c94d6b7b4612a69004a5fb59c75b8aa03dbcdc9627797130af9a33be3</originalsourceid><addsrcrecordid>eNotjkFLAzEYRIMouFb_gKeA59QkX7LZHKXWVihVtAqeSpLNarRuJIkgiv_dLXYuD4ZheAidMjpmjML57fzp_m76eDluYEyloFzvoYrRRhOhWbOPKiplTXjD2SE6yvmVDuE1VGi59F-FlEg23rShfyYxtT5hF1PyroTY4xLxx5ZdTO-4M67EhEOP337yp8Wr310Vvs12fYwOOrPJ_mTHEXq4mq4mc7K4mV1PLhYkMgaFcKYGNwdOi7a2yoqacVNrSoWRnZXaKWkbYyi01rVO11wprRhQ02kDYD2M0Nn_b8wlrLMLxbsXF_t-kF5zJkEJEPAHIWdRrA</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Next-to-leading-order correction to pion form factor in k{sub T} factorization</title><source>American Physical Society Journals</source><creator>Li Hsiangnan ; Department of Physics, National Cheng-Kung University, Tainan, Taiwan 701 ; Department of Physics, National Tsing-Hua University, Hsinchu, Taiwan 300 ; Shen Yuelong ; College of Information Science and Engineering, Ocean University of China, Qingdao, Shandong 266100 ; Wang Yuming ; Institute of High Energy Physics and Theoretical Physics Center for Science Facilities, Post Office Box 918 ; Zou Hao</creator><creatorcontrib>Li Hsiangnan ; Department of Physics, National Cheng-Kung University, Tainan, Taiwan 701 ; Department of Physics, National Tsing-Hua University, Hsinchu, Taiwan 300 ; Shen Yuelong ; College of Information Science and Engineering, Ocean University of China, Qingdao, Shandong 266100 ; Wang Yuming ; Institute of High Energy Physics and Theoretical Physics Center for Science Facilities, Post Office Box 918 ; Zou Hao</creatorcontrib><description>We calculate the next-to-leading-order (NLO) correction to the pion electromagnetic form factor at leading twist in the k{sub T} factorization theorem. Partons off-shell by k{sub T}{sup 2} are considered in both quark diagrams and effective diagrams for the transverse-momentum-dependent pion wave function. The light-cone singularities in the transverse-momentum-dependent pion wave function are regularized by rotating the Wilson lines away from the light cone. The soft divergences from gluon exchanges among initial- and fal-state partons cancel exactly. We derive the infrared-finite k{sub T}-dependent NLO hard kernel for the pion electromagnetic form factor by taking the difference of the above two sets of diagrams. Varying the renormalization and factorization scales, we find that the NLO correction is smaller, when both the scales are set to the invariant masses of internal particles: it becomes lower than 40% of the leading-order contribution for momentum transfer squared Q{sup 2}>7 GeV{sup 2}. It is observed that the NLO leading-twist correction does not play an essential role in explaining the experimental data, but the leading-order higher-twist contribution does.</description><identifier>ISSN: 0556-2821</identifier><identifier>EISSN: 1089-4918</identifier><identifier>DOI: 10.1103/PHYSREVD.83.054029</identifier><language>eng</language><publisher>United States</publisher><subject>BOSONS ; COMPUTERIZED SIMULATION ; CORRECTIONS ; DIMENSIONLESS NUMBERS ; ELECTROMAGNETIC FORM FACTORS ; ELEMENTARY PARTICLES ; FACTORIZATION ; FERMIONS ; FORM FACTORS ; FUNCTIONS ; GLUONS ; HADRONS ; LINEAR MOMENTUM ; MASS ; MESONS ; MOMENTUM TRANSFER ; PARTICLE PROPERTIES ; PARTICLES ; PHYSICS OF ELEMENTARY PARTICLES AND FIELDS ; PIONS ; PSEUDOSCALAR MESONS ; QUARKS ; RENORMALIZATION ; SIMULATION ; SINGULARITY ; TRANSVERSE MOMENTUM ; WAVE FUNCTIONS ; WILSON LOOP</subject><ispartof>Physical review. D, Particles and fields, 2011-03, Vol.83 (5)</ispartof><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,780,784,885,27922,27923</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/21537434$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Li Hsiangnan</creatorcontrib><creatorcontrib>Department of Physics, National Cheng-Kung University, Tainan, Taiwan 701</creatorcontrib><creatorcontrib>Department of Physics, National Tsing-Hua University, Hsinchu, Taiwan 300</creatorcontrib><creatorcontrib>Shen Yuelong</creatorcontrib><creatorcontrib>College of Information Science and Engineering, Ocean University of China, Qingdao, Shandong 266100</creatorcontrib><creatorcontrib>Wang Yuming</creatorcontrib><creatorcontrib>Institute of High Energy Physics and Theoretical Physics Center for Science Facilities, Post Office Box 918</creatorcontrib><creatorcontrib>Zou Hao</creatorcontrib><title>Next-to-leading-order correction to pion form factor in k{sub T} factorization</title><title>Physical review. D, Particles and fields</title><description>We calculate the next-to-leading-order (NLO) correction to the pion electromagnetic form factor at leading twist in the k{sub T} factorization theorem. Partons off-shell by k{sub T}{sup 2} are considered in both quark diagrams and effective diagrams for the transverse-momentum-dependent pion wave function. The light-cone singularities in the transverse-momentum-dependent pion wave function are regularized by rotating the Wilson lines away from the light cone. The soft divergences from gluon exchanges among initial- and fal-state partons cancel exactly. We derive the infrared-finite k{sub T}-dependent NLO hard kernel for the pion electromagnetic form factor by taking the difference of the above two sets of diagrams. Varying the renormalization and factorization scales, we find that the NLO correction is smaller, when both the scales are set to the invariant masses of internal particles: it becomes lower than 40% of the leading-order contribution for momentum transfer squared Q{sup 2}>7 GeV{sup 2}. It is observed that the NLO leading-twist correction does not play an essential role in explaining the experimental data, but the leading-order higher-twist contribution does.</description><subject>BOSONS</subject><subject>COMPUTERIZED SIMULATION</subject><subject>CORRECTIONS</subject><subject>DIMENSIONLESS NUMBERS</subject><subject>ELECTROMAGNETIC FORM FACTORS</subject><subject>ELEMENTARY PARTICLES</subject><subject>FACTORIZATION</subject><subject>FERMIONS</subject><subject>FORM FACTORS</subject><subject>FUNCTIONS</subject><subject>GLUONS</subject><subject>HADRONS</subject><subject>LINEAR MOMENTUM</subject><subject>MASS</subject><subject>MESONS</subject><subject>MOMENTUM TRANSFER</subject><subject>PARTICLE PROPERTIES</subject><subject>PARTICLES</subject><subject>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</subject><subject>PIONS</subject><subject>PSEUDOSCALAR MESONS</subject><subject>QUARKS</subject><subject>RENORMALIZATION</subject><subject>SIMULATION</subject><subject>SINGULARITY</subject><subject>TRANSVERSE MOMENTUM</subject><subject>WAVE FUNCTIONS</subject><subject>WILSON LOOP</subject><issn>0556-2821</issn><issn>1089-4918</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNotjkFLAzEYRIMouFb_gKeA59QkX7LZHKXWVihVtAqeSpLNarRuJIkgiv_dLXYuD4ZheAidMjpmjML57fzp_m76eDluYEyloFzvoYrRRhOhWbOPKiplTXjD2SE6yvmVDuE1VGi59F-FlEg23rShfyYxtT5hF1PyroTY4xLxx5ZdTO-4M67EhEOP337yp8Wr310Vvs12fYwOOrPJ_mTHEXq4mq4mc7K4mV1PLhYkMgaFcKYGNwdOi7a2yoqacVNrSoWRnZXaKWkbYyi01rVO11wprRhQ02kDYD2M0Nn_b8wlrLMLxbsXF_t-kF5zJkEJEPAHIWdRrA</recordid><startdate>20110331</startdate><enddate>20110331</enddate><creator>Li Hsiangnan</creator><creator>Department of Physics, National Cheng-Kung University, Tainan, Taiwan 701</creator><creator>Department of Physics, National Tsing-Hua University, Hsinchu, Taiwan 300</creator><creator>Shen Yuelong</creator><creator>College of Information Science and Engineering, Ocean University of China, Qingdao, Shandong 266100</creator><creator>Wang Yuming</creator><creator>Institute of High Energy Physics and Theoretical Physics Center for Science Facilities, Post Office Box 918</creator><creator>Zou Hao</creator><scope>OTOTI</scope></search><sort><creationdate>20110331</creationdate><title>Next-to-leading-order correction to pion form factor in k{sub T} factorization</title><author>Li Hsiangnan ; Department of Physics, National Cheng-Kung University, Tainan, Taiwan 701 ; Department of Physics, National Tsing-Hua University, Hsinchu, Taiwan 300 ; Shen Yuelong ; College of Information Science and Engineering, Ocean University of China, Qingdao, Shandong 266100 ; Wang Yuming ; Institute of High Energy Physics and Theoretical Physics Center for Science Facilities, Post Office Box 918 ; Zou Hao</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-o113t-217089c3c94d6b7b4612a69004a5fb59c75b8aa03dbcdc9627797130af9a33be3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>BOSONS</topic><topic>COMPUTERIZED SIMULATION</topic><topic>CORRECTIONS</topic><topic>DIMENSIONLESS NUMBERS</topic><topic>ELECTROMAGNETIC FORM FACTORS</topic><topic>ELEMENTARY PARTICLES</topic><topic>FACTORIZATION</topic><topic>FERMIONS</topic><topic>FORM FACTORS</topic><topic>FUNCTIONS</topic><topic>GLUONS</topic><topic>HADRONS</topic><topic>LINEAR MOMENTUM</topic><topic>MASS</topic><topic>MESONS</topic><topic>MOMENTUM TRANSFER</topic><topic>PARTICLE PROPERTIES</topic><topic>PARTICLES</topic><topic>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</topic><topic>PIONS</topic><topic>PSEUDOSCALAR MESONS</topic><topic>QUARKS</topic><topic>RENORMALIZATION</topic><topic>SIMULATION</topic><topic>SINGULARITY</topic><topic>TRANSVERSE MOMENTUM</topic><topic>WAVE FUNCTIONS</topic><topic>WILSON LOOP</topic><toplevel>online_resources</toplevel><creatorcontrib>Li Hsiangnan</creatorcontrib><creatorcontrib>Department of Physics, National Cheng-Kung University, Tainan, Taiwan 701</creatorcontrib><creatorcontrib>Department of Physics, National Tsing-Hua University, Hsinchu, Taiwan 300</creatorcontrib><creatorcontrib>Shen Yuelong</creatorcontrib><creatorcontrib>College of Information Science and Engineering, Ocean University of China, Qingdao, Shandong 266100</creatorcontrib><creatorcontrib>Wang Yuming</creatorcontrib><creatorcontrib>Institute of High Energy Physics and Theoretical Physics Center for Science Facilities, Post Office Box 918</creatorcontrib><creatorcontrib>Zou Hao</creatorcontrib><collection>OSTI.GOV</collection><jtitle>Physical review. D, Particles and fields</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Li Hsiangnan</au><au>Department of Physics, National Cheng-Kung University, Tainan, Taiwan 701</au><au>Department of Physics, National Tsing-Hua University, Hsinchu, Taiwan 300</au><au>Shen Yuelong</au><au>College of Information Science and Engineering, Ocean University of China, Qingdao, Shandong 266100</au><au>Wang Yuming</au><au>Institute of High Energy Physics and Theoretical Physics Center for Science Facilities, Post Office Box 918</au><au>Zou Hao</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Next-to-leading-order correction to pion form factor in k{sub T} factorization</atitle><jtitle>Physical review. D, Particles and fields</jtitle><date>2011-03-31</date><risdate>2011</risdate><volume>83</volume><issue>5</issue><issn>0556-2821</issn><eissn>1089-4918</eissn><abstract>We calculate the next-to-leading-order (NLO) correction to the pion electromagnetic form factor at leading twist in the k{sub T} factorization theorem. Partons off-shell by k{sub T}{sup 2} are considered in both quark diagrams and effective diagrams for the transverse-momentum-dependent pion wave function. The light-cone singularities in the transverse-momentum-dependent pion wave function are regularized by rotating the Wilson lines away from the light cone. The soft divergences from gluon exchanges among initial- and fal-state partons cancel exactly. We derive the infrared-finite k{sub T}-dependent NLO hard kernel for the pion electromagnetic form factor by taking the difference of the above two sets of diagrams. Varying the renormalization and factorization scales, we find that the NLO correction is smaller, when both the scales are set to the invariant masses of internal particles: it becomes lower than 40% of the leading-order contribution for momentum transfer squared Q{sup 2}>7 GeV{sup 2}. It is observed that the NLO leading-twist correction does not play an essential role in explaining the experimental data, but the leading-order higher-twist contribution does.</abstract><cop>United States</cop><doi>10.1103/PHYSREVD.83.054029</doi></addata></record> |
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subjects | BOSONS COMPUTERIZED SIMULATION CORRECTIONS DIMENSIONLESS NUMBERS ELECTROMAGNETIC FORM FACTORS ELEMENTARY PARTICLES FACTORIZATION FERMIONS FORM FACTORS FUNCTIONS GLUONS HADRONS LINEAR MOMENTUM MASS MESONS MOMENTUM TRANSFER PARTICLE PROPERTIES PARTICLES PHYSICS OF ELEMENTARY PARTICLES AND FIELDS PIONS PSEUDOSCALAR MESONS QUARKS RENORMALIZATION SIMULATION SINGULARITY TRANSVERSE MOMENTUM WAVE FUNCTIONS WILSON LOOP |
title | Next-to-leading-order correction to pion form factor in k{sub T} factorization |
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