Onset of scaling violation in pion and kaon elastic electromagnetic form factors
Using a symmetry-preserving truncation of the quantum field equations describing hadron properties, parameter-free predictions are delivered for pion and kaon elastic electromagnetic form factors, FP=π,K, thereby unifying them with kindred results for nucleon elastic electromagnetic form factors. Re...
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| Published in | Physics letters. B Vol. 855; p. 138823 |
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| Main Authors | , , |
| Format | Journal Article |
| Language | English |
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Elsevier B.V
01.08.2024
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| Abstract | Using a symmetry-preserving truncation of the quantum field equations describing hadron properties, parameter-free predictions are delivered for pion and kaon elastic electromagnetic form factors, FP=π,K, thereby unifying them with kindred results for nucleon elastic electromagnetic form factors. Regarding positive-charge states, the analysis stresses that the presence of scaling violations in QCD entails that Q2FP(Q2) should exhibit a single maximum on Q2>0. Locating such a maximum is both necessary and sufficient to establish the existence of scaling violations. The study predicts that, for charged π, K mesons, the Q2FP(Q2) maximum lies in the neighbourhood Q2≃5 GeV2. Foreseeable experiments will test these predictions and, providing their Q2 reach meets expectations, potentially also provide details on the momentum dependence of meson form factor scaling violation. |
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| AbstractList | Using a symmetry-preserving truncation of the quantum field equations describing hadron properties, parameter-free predictions are delivered for pion and kaon elastic electromagnetic form factors, FP=π,K, thereby unifying them with kindred results for nucleon elastic electromagnetic form factors. Regarding positive-charge states, the analysis stresses that the presence of scaling violations in QCD entails that Q2FP(Q2) should exhibit a single maximum on Q2>0. Locating such a maximum is both necessary and sufficient to establish the existence of scaling violations. The study predicts that, for charged π, K mesons, the Q2FP(Q2) maximum lies in the neighbourhood Q2≃5 GeV2. Foreseeable experiments will test these predictions and, providing their Q2 reach meets expectations, potentially also provide details on the momentum dependence of meson form factor scaling violation. |
| ArticleNumber | 138823 |
| Author | Roberts, Craig D. Binosi, Daniele Yao, Zhao-Qian |
| Author_xml | – sequence: 1 givenname: Zhao-Qian orcidid: 0000-0002-9621-6994 surname: Yao fullname: Yao, Zhao-Qian email: zyao@ectstar.eu organization: European Centre for Theoretical Studies in Nuclear Physics and Related Areas, Villa Tambosi, Strada delle Tabarelle 286, I-38123 Villazzano (TN), Italy – sequence: 2 givenname: Daniele orcidid: 0000-0003-1742-4689 surname: Binosi fullname: Binosi, Daniele email: binosi@ectstar.eu organization: European Centre for Theoretical Studies in Nuclear Physics and Related Areas, Villa Tambosi, Strada delle Tabarelle 286, I-38123 Villazzano (TN), Italy – sequence: 3 givenname: Craig D. orcidid: 0000-0002-2937-1361 surname: Roberts fullname: Roberts, Craig D. email: cdroberts@nju.edu.cn organization: School of Physics, Nanjing University, Nanjing, Jiangsu 210093, China |
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| Keywords | Elastic electromagnetic form factors Emergence of mass Continuum Schwinger function methods Nambu-Goldstone bosons Scaling violations Hard exclusive processes |
| Language | English |
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| References | Cui, Gao, Binosi, Chang, Roberts, Schmidt (br0730) 2022; 39 Binosi, Chang, Ding, Gao, Papavassiliou, Roberts (br0680) 2019; 790 Horn, Roberts (br0020) 2016; 43 Maris, Roberts (br0140) 1997; 56 Fischer, Huber (br0710) 2020; 102 Ding, Roberts, Schmidt (br0080) 2023; 6 Qin, Roberts, Schmidt (br0150) 2014; 733 Wang, Liang, Draper, Liu, Yang (br0300) 2021; 104 Maris, Tandy (br0610) 2006; 161 Chen, Lu, Binosi, Roberts, Rodríguez-Quintero, Segovia (br0670) 2019; 99 Lepage, Brodsky (br0240) 1979; 87 Koponen, Zimermmane-Santos, Davies, Lepage, Lytle (br0280) 2017; 96 Cui, Binosi, Roberts, Schmidt (br0740) 2022; 46 Efremov, Radyushkin (br0250) 1980; 94 Chang, Liu, Roberts, Shi, Sun, Zong (br0590) 2009; 79 Munczek (br0450) 1995; 52 Aguilar (br0180) 2019; 55 Davies, Koponen, Lepage, Lytle, Zimermmane-Santos (br0290) 2018; LATTICE2018 Chambers (br0270) 2017; 96 Ferreira, Papavassiliou (br0100) 2023; 6 Binosi, Pilloni, Tripolt (br0750) 2023; 839 Eichmann, Sanchis-Alepuz, Williams, Alkofer, Fischer (br0030) 2016; 91 Lepage, Brodsky (br0260) 1980; 22 Gao, Chang, Liu, Roberts, Tandy (br0480) 2017; 96 Cui, Binosi, Roberts, Schmidt (br0550) 2021; 822 Ahmed, Chen, Huang (br0430) 2023; 108 Huber, Fischer, Sanchis-Alepuz (br0700) 2020; 80 Arrington (br0190) 2021; 48 Yao, Binosi, Cui, Roberts (br0520) Roberts (br0350) 1996; 605 Schlessinger, Schwartz (br0640) 1966; 16 Schlessinger (br0650) 1968; 167 Horn (br0530) 2008; 78 Raya, Bashir, Binosi, Roberts, Rodríguez-Quintero (br0120) 2024 Hua (br0330) 2022; 129 Huber (br0540) 2008; 78 Xing, Ding, Cui, Pimikov, Roberts, Schmidt (br0780) 2024; 849 Yao, Binosi, Cui, Roberts (br0720) 2021; 818 Salmè (br0130) 2022; 2340 Fischer (br0040) 2019; 105 Ent, Rossi (br0160) 2015; 25 Binosi, Chang, Papavassiliou, Roberts (br0580) 2015; 742 Carman, Gothe, Mokeev, Roberts (br0090) 2023; 6 Deur, Brodsky, Roberts (br0110) 2024; 134 Qin, Roberts (br0050) 2020; 37 Bender, Roberts, von Smekal (br0460) 1996; 380 T. Horn, G.M. Huber, D. Gaskell, et al., Study of the L–T Separated Pion Electroproduction Cross Section at 11 GeV and Measurement of the Charged Pion Form Factor to High Binosi (br0070) 2022; 63 Roberts, Richards, Horn, Chang (br0060) 2021; 120 Maris, Roberts (br0360) 1998; 58 Nakanishi (br0490) 1969; 43 Bashir, Raya, Sánchez-Madrigal, Roberts (br0560) 2009; 46 Bhagwat, Pichowsky, Tandy (br0630) 2003; 67 Lan, Fu, Mondal, Zhao, Vary (br0390) 2022; 825 Maris, Tandy (br0440) 2000; 62 approved Jefferson Lab experiment “E12-19-006”, 2019. Ahmady, Mondal, Sandapen (br0370) 2018; 98 Binosi, Tripolt (br0690) 2020; 801 Chen, Ding, Chang, Roberts (br0770) 2018; 98 Abdul Khalek (br0200) 2022; 1026 Alexandrou, Bacchio, Cloet, Constantinou, Delmar, Hadjiyiannakou, Koutsou, Lauer, Vaquero (br0310) 2022; 105 Chang, Cloet, Roberts, Schmidt, Tandy (br0470) 2013; 111 Workman (br0010) 2022; 2022 Choi, Ji (br0380) 2020; 102 Chai, Cheng, Hua (br0790) 2023; 83 Anderle (br0220) 2021; 16 Li, Maris, Vary (br0420) 2023; 836 Cui, Binosi, Roberts, Schmidt, Triantafyllopoulos (br0760) 2023; 839 Tripolt, Haritan, Wambach, Moiseyev (br0660) 2017; 774 Er, Azizi (br0410) 2022; 82 Krassnigg (br0620) 2008; CONFINEMENT 8 Wang, Chen (br0230) 2022; 63 Chen, Guo, Roberts, Wang (br0210) 2020; 61 Qin, Chang, Liu, Roberts, Wilson (br0570) 2011; 84 Gao, Hanlon, Karthik, Mukherjee, Petreczky, Scior, Syritsyn, Zhao (br0340) 2022; 106 Ydrefors, de Paula, Nogueira, Frederico, Salmé (br0400) 2021; 820 Cui, Zhang, Binosi, de Soto, Mezrag, Papavassiliou, Roberts, Rodríguez-Quintero, Segovia, Zafeiropoulos (br0600) 2020; 44 Quintans (br0170) 2022; 63 Horn, Huber, Markowitz (br0510) 2009 Ding, Gao, Hanlon, Mukherjee, Petreczky, Shi, Syritsyn, Zhao (br0320) 2024; LATTICE2023 Nakanishi (10.1016/j.physletb.2024.138823_br0490) 1969; 43 Raya (10.1016/j.physletb.2024.138823_br0120) Choi (10.1016/j.physletb.2024.138823_br0380) 2020; 102 Roberts (10.1016/j.physletb.2024.138823_br0060) 2021; 120 Efremov (10.1016/j.physletb.2024.138823_br0250) 1980; 94 Cui (10.1016/j.physletb.2024.138823_br0760) 2023; 839 Lan (10.1016/j.physletb.2024.138823_br0390) 2022; 825 Huber (10.1016/j.physletb.2024.138823_br0540) 2008; 78 Eichmann (10.1016/j.physletb.2024.138823_br0030) 2016; 91 Fischer (10.1016/j.physletb.2024.138823_br0040) 2019; 105 Arrington (10.1016/j.physletb.2024.138823_br0190) 2021; 48 Chambers (10.1016/j.physletb.2024.138823_br0270) 2017; 96 Lepage (10.1016/j.physletb.2024.138823_br0240) 1979; 87 Chai (10.1016/j.physletb.2024.138823_br0790) 2023; 83 Binosi (10.1016/j.physletb.2024.138823_br0680) 2019; 790 Hua (10.1016/j.physletb.2024.138823_br0330) 2022; 129 Ahmady (10.1016/j.physletb.2024.138823_br0370) 2018; 98 Fischer (10.1016/j.physletb.2024.138823_br0710) 2020; 102 Qin (10.1016/j.physletb.2024.138823_br0050) 2020; 37 Munczek (10.1016/j.physletb.2024.138823_br0450) 1995; 52 Cui (10.1016/j.physletb.2024.138823_br0600) 2020; 44 Chang (10.1016/j.physletb.2024.138823_br0590) 2009; 79 Maris (10.1016/j.physletb.2024.138823_br0440) 2000; 62 Davies (10.1016/j.physletb.2024.138823_br0290) 2018; LATTICE2018 Chang (10.1016/j.physletb.2024.138823_br0470) 2013; 111 Alexandrou (10.1016/j.physletb.2024.138823_br0310) 2022; 105 Binosi (10.1016/j.physletb.2024.138823_br0750) 2023; 839 Maris (10.1016/j.physletb.2024.138823_br0610) 2006; 161 Salmè (10.1016/j.physletb.2024.138823_br0130) 2022; 2340 Qin (10.1016/j.physletb.2024.138823_br0570) 2011; 84 Maris (10.1016/j.physletb.2024.138823_br0360) 1998; 58 Binosi (10.1016/j.physletb.2024.138823_br0580) 2015; 742 Qin (10.1016/j.physletb.2024.138823_br0150) 2014; 733 Abdul Khalek (10.1016/j.physletb.2024.138823_br0200) 2022; 1026 10.1016/j.physletb.2024.138823_br0500 Cui (10.1016/j.physletb.2024.138823_br0550) 2021; 822 Anderle (10.1016/j.physletb.2024.138823_br0220) 2021; 16 Roberts (10.1016/j.physletb.2024.138823_br0350) 1996; 605 Tripolt (10.1016/j.physletb.2024.138823_br0660) 2017; 774 Wang (10.1016/j.physletb.2024.138823_br0230) 2022; 63 Koponen (10.1016/j.physletb.2024.138823_br0280) 2017; 96 Deur (10.1016/j.physletb.2024.138823_br0110) 2024; 134 Bashir (10.1016/j.physletb.2024.138823_br0560) 2009; 46 Chen (10.1016/j.physletb.2024.138823_br0670) 2019; 99 Workman (10.1016/j.physletb.2024.138823_br0010) 2022; 2022 Binosi (10.1016/j.physletb.2024.138823_br0070) 2022; 63 Chen (10.1016/j.physletb.2024.138823_br0770) 2018; 98 Chen (10.1016/j.physletb.2024.138823_br0210) 2020; 61 Horn (10.1016/j.physletb.2024.138823_br0020) 2016; 43 Ahmed (10.1016/j.physletb.2024.138823_br0430) 2023; 108 Yao (10.1016/j.physletb.2024.138823_br0720) 2021; 818 Ydrefors (10.1016/j.physletb.2024.138823_br0400) 2021; 820 Ent (10.1016/j.physletb.2024.138823_br0160) 2015; 25 Yao (10.1016/j.physletb.2024.138823_br0520) Carman (10.1016/j.physletb.2024.138823_br0090) 2023; 6 Bhagwat (10.1016/j.physletb.2024.138823_br0630) 2003; 67 Cui (10.1016/j.physletb.2024.138823_br0730) 2022; 39 Ding (10.1016/j.physletb.2024.138823_br0320) 2024; LATTICE2023 Ferreira (10.1016/j.physletb.2024.138823_br0100) 2023; 6 Aguilar (10.1016/j.physletb.2024.138823_br0180) 2019; 55 Horn (10.1016/j.physletb.2024.138823_br0530) 2008; 78 Huber (10.1016/j.physletb.2024.138823_br0700) 2020; 80 Schlessinger (10.1016/j.physletb.2024.138823_br0640) 1966; 16 Li (10.1016/j.physletb.2024.138823_br0420) 2023; 836 Bender (10.1016/j.physletb.2024.138823_br0460) 1996; 380 Schlessinger (10.1016/j.physletb.2024.138823_br0650) 1968; 167 Cui (10.1016/j.physletb.2024.138823_br0740) 2022; 46 Xing (10.1016/j.physletb.2024.138823_br0780) 2024; 849 Ding (10.1016/j.physletb.2024.138823_br0080) 2023; 6 Gao (10.1016/j.physletb.2024.138823_br0480) 2017; 96 Maris (10.1016/j.physletb.2024.138823_br0140) 1997; 56 Krassnigg (10.1016/j.physletb.2024.138823_br0620) 2008; CONFINEMENT 8 Er (10.1016/j.physletb.2024.138823_br0410) 2022; 82 Lepage (10.1016/j.physletb.2024.138823_br0260) 1980; 22 Binosi (10.1016/j.physletb.2024.138823_br0690) 2020; 801 Quintans (10.1016/j.physletb.2024.138823_br0170) 2022; 63 Wang (10.1016/j.physletb.2024.138823_br0300) 2021; 104 Gao (10.1016/j.physletb.2024.138823_br0340) 2022; 106 Horn (10.1016/j.physletb.2024.138823_br0510) 2009 |
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| Title | Onset of scaling violation in pion and kaon elastic electromagnetic form factors |
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