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)
Hauptverfasser: 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
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container_issue 5
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container_title Physical review. D, Particles and fields
container_volume 83
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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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}&gt;7 GeV{sup 2}. 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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}&gt;7 GeV{sup 2}. 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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}&gt;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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source American Physical Society Journals
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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