Proton spin structure and generalized polarizabilities in the strong quantum chromodynamics regime

D. Ruth; R. Zielinski; C. Gu; M. Allada (Cummings); T. Badman; M. Huang; J. Liu; P. Zhu; K. Allada; J. Zhang; A. Camsonne; J. P. Chen; K. Slifer; K. Aniol; J. Annand; J. Arrington; T. Averett; H. Baghdasaryan; V. Bellini; W. Boeglin; J. Brock; C. Carlin; C. Chen; E. Cisbani; D. Crabb; A. Daniel; D. Day; R. Duve; L. El Fassi; M. Friedman; E. Fuchey; H. Gao; R. Gilman; S. Glamazdin; P. Gueye; M. Hafez; Y. Han; O. Hansen; M. Hashemi Shabestari; O. Hen; D. Higinbotham; T. Horn; S. Iqbal; E. Jensen; H. Kang; C. D. Keith; A. Kelleher; D. Keller; H. Khanal; I. Korover; G. Kumbartzki; W. Li; J. Lichtenstadt; R. Lindgren; E. Long; S. Malace; P. Markowitz; J. Maxwell; D. M. Meekins; Z. E. Meziani; C. McLean; R. Michaels; M. Mihovilovič; N. Muangma; C. Munoz Camacho; J. Musson; K. Myers; Y. Oh; M. Pannunzio Carmignotto; C. Perdrisat; S. Phillips; E. Piasetzky; J. Pierce; V. Punjabi; Y. Qiang; P. E. Reimer; Y. Roblin; G. Ron; O. Rondon; G. Russo; K. Saenboonruang; B. Sawatzky; A. Shahinyan; R. Shneor; S. Širca; J. Sjoegren; P. Solvignon-Slifer; N. Sparveris; V. Sulkosky; F. Wesselmann; W. Yan; H. Yang; H. Yao; Z. Ye; M. Yurov; Y. Zhang; Y. X. Zhao; X. Zheng

doi:10.1038/s41567-022-01781-y

Proton spin structure and generalized polarizabilities in the strong quantum chromodynamics regime

D. Ruth
, R. Zielinski
, C. Gu
, M. Allada (Cummings)
, T. Badman
, M. Huang
, J. Liu
, P. Zhu
, K. Allada
, J. Zhang
, A. Camsonne
, J. P. Chen
, K. Slifer
, K. Aniol
, J. Annand
, J. Arrington
, T. Averett
, H. Baghdasaryan
, V. Bellini
, W. Boeglin

J. Brock, C. Carlin, C. Chen, E. Cisbani, D. Crabb, A. Daniel, D. Day, R. Duve, L. El Fassi, M. Friedman, E. Fuchey, H. Gao, R. Gilman, S. Glamazdin, P. Gueye, M. Hafez, Y. Han, O. Hansen, M. Hashemi Shabestari, O. Hen, D. Higinbotham, T. Horn, S. Iqbal, E. Jensen, H. Kang, C. D. Keith, A. Kelleher, D. Keller, H. Khanal, I. Korover, G. Kumbartzki, W. Li, J. Lichtenstadt, R. Lindgren, E. Long, S. Malace, P. Markowitz, J. Maxwell, D. M. Meekins, Z. E. Meziani, C. McLean, R. Michaels, M. Mihovilovič, N. Muangma, C. Munoz Camacho, J. Musson, K. Myers, Y. Oh, M. Pannunzio Carmignotto, C. Perdrisat, S. Phillips, E. Piasetzky, J. Pierce, V. Punjabi, Y. Qiang, P. E. Reimer, Y. Roblin, G. Ron, O. Rondon, G. Russo, K. Saenboonruang, B. Sawatzky, A. Shahinyan, R. Shneor, S. Širca, J. Sjoegren, P. Solvignon-Slifer, N. Sparveris, V. Sulkosky, F. Wesselmann, W. Yan, H. Yang, H. Yao, Z. Ye, M. Yurov, Y. Zhang, Y. X. Zhao, X. Zheng

Physics

University of New Hampshire
University of Virginia
College of William and Mary
Duke University
University of Science and Technology of China
Massachusetts Institute of Technology
Thomas Jefferson National Accelerator Facility
California State University Los Angeles
University of Glasgow
Argonne National Laboratory
Lawrence Berkeley National Laboratory
University of Catania
Florida International University
Hampton University
National Institute for Nuclear Physics
Rutgers - The State University of New Jersey, New Brunswick
Mississippi State University
Hebrew University of Jerusalem
Temple University
NASU - Kharkov Institute of Physics and Technology
Old Dominion University
Cairo University
Catholic University of America
Christopher Newport University
Seoul National University
Tel Aviv University
University of Regina
University of South Carolina
University of Ljubljana
Jožef Stefan Institute
Institut de Physique Nucléaire
Oak Ridge National Laboratory
Norfolk State University
A. Alikhanian Yerevan Institute of Physics
Xavier University of Louisiana
Chinese Academy of Sciences

Research output: Contribution to journal › Article › peer-review

10 Scopus citations

Abstract

The strong interaction is not well understood at low energies or for interactions with low momentum transfer. Chiral perturbation theory gives testable predictions for the nucleonic generalized polarizabilities, which are fundamental quantities describing the nucleon’s response to an external field. We report a measurement of the proton’s generalized spin polarizabilities extracted with a polarized electron beam and a polarized solid ammonia target in the region where chiral perturbation theory is expected to be valid. The investigated structure function g₂ characterizes the internal spin structure of the proton. From its moments, we extract the longitudinal–transverse spin polarizability δ_LT and twist-3 matrix element and polarizability d₂¯. Our results provide discriminating power between existing chiral perturbation theory calculations and will help provide a better understanding of this strong quantum chromodynamics regime.

Original language	English
Pages (from-to)	1441-1446
Number of pages	6
Journal	Nature Physics
Volume	18
Issue number	12
DOIs	https://doi.org/10.1038/s41567-022-01781-y
State	Published - Dec 2022

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Ruth, D., Zielinski, R., Gu, C., Allada (Cummings), M., Badman, T., Huang, M., Liu, J., Zhu, P., Allada, K., Zhang, J., Camsonne, A., Chen, J. P., Slifer, K., Aniol, K., Annand, J., Arrington, J., Averett, T., Baghdasaryan, H., Bellini, V., ... Zheng, X. (2022). Proton spin structure and generalized polarizabilities in the strong quantum chromodynamics regime. Nature Physics, 18(12), 1441-1446. https://doi.org/10.1038/s41567-022-01781-y

@article{c4e44e77759b456fa24e2eac69efcfd0,

title = "Proton spin structure and generalized polarizabilities in the strong quantum chromodynamics regime",

abstract = "The strong interaction is not well understood at low energies or for interactions with low momentum transfer. Chiral perturbation theory gives testable predictions for the nucleonic generalized polarizabilities, which are fundamental quantities describing the nucleon{\textquoteright}s response to an external field. We report a measurement of the proton{\textquoteright}s generalized spin polarizabilities extracted with a polarized electron beam and a polarized solid ammonia target in the region where chiral perturbation theory is expected to be valid. The investigated structure function g2 characterizes the internal spin structure of the proton. From its moments, we extract the longitudinal{\textendash}transverse spin polarizability δLT and twist-3 matrix element and polarizability d2¯. Our results provide discriminating power between existing chiral perturbation theory calculations and will help provide a better understanding of this strong quantum chromodynamics regime.",

author = "D. Ruth and R. Zielinski and C. Gu and \{Allada (Cummings)\}, M. and T. Badman and M. Huang and J. Liu and P. Zhu and K. Allada and J. Zhang and A. Camsonne and Chen, \{J. P.\} and K. Slifer and K. Aniol and J. Annand and J. Arrington and T. Averett and H. Baghdasaryan and V. Bellini and W. Boeglin and J. Brock and C. Carlin and C. Chen and E. Cisbani and D. Crabb and A. Daniel and D. Day and R. Duve and Fassi, \{L. El\} and M. Friedman and E. Fuchey and H. Gao and R. Gilman and S. Glamazdin and P. Gueye and M. Hafez and Y. Han and O. Hansen and Shabestari, \{M. Hashemi\} and O. Hen and D. Higinbotham and T. Horn and S. Iqbal and E. Jensen and H. Kang and Keith, \{C. D.\} and A. Kelleher and D. Keller and H. Khanal and I. Korover and G. Kumbartzki and W. Li and J. Lichtenstadt and R. Lindgren and E. Long and S. Malace and P. Markowitz and J. Maxwell and Meekins, \{D. M.\} and Meziani, \{Z. E.\} and C. McLean and R. Michaels and M. Mihovilovi{\v c} and N. Muangma and Camacho, \{C. Munoz\} and J. Musson and K. Myers and Y. Oh and Carmignotto, \{M. Pannunzio\} and C. Perdrisat and S. Phillips and E. Piasetzky and J. Pierce and V. Punjabi and Y. Qiang and Reimer, \{P. E.\} and Y. Roblin and G. Ron and O. Rondon and G. Russo and K. Saenboonruang and B. Sawatzky and A. Shahinyan and R. Shneor and S. {\v S}irca and J. Sjoegren and P. Solvignon-Slifer and N. Sparveris and V. Sulkosky and F. Wesselmann and W. Yan and H. Yang and H. Yao and Z. Ye and M. Yurov and Y. Zhang and Zhao, \{Y. X.\} and X. Zheng",

note = "Publisher Copyright: {\textcopyright} 2022, The Author(s), under exclusive licence to Springer Nature Limited.",

year = "2022",

month = dec,

doi = "10.1038/s41567-022-01781-y",

language = "English",

volume = "18",

pages = "1441--1446",

journal = "Nature Physics",

issn = "1745-2473",

publisher = "Nature Research",

number = "12",

}

Ruth, D, Zielinski, R, Gu, C, Allada (Cummings), M, Badman, T, Huang, M, Liu, J, Zhu, P, Allada, K, Zhang, J, Camsonne, A, Chen, JP, Slifer, K, Aniol, K, Annand, J, Arrington, J, Averett, T, Baghdasaryan, H, Bellini, V, Boeglin, W, Brock, J, Carlin, C, Chen, C, Cisbani, E, Crabb, D, Daniel, A, Day, D, Duve, R, Fassi, LE, Friedman, M, Fuchey, E, Gao, H, Gilman, R, Glamazdin, S, Gueye, P, Hafez, M, Han, Y, Hansen, O, Shabestari, MH, Hen, O, Higinbotham, D, Horn, T, Iqbal, S, Jensen, E, Kang, H, Keith, CD, Kelleher, A, Keller, D, Khanal, H, Korover, I, Kumbartzki, G, Li, W, Lichtenstadt, J, Lindgren, R, Long, E, Malace, S, Markowitz, P, Maxwell, J, Meekins, DM, Meziani, ZE, McLean, C, Michaels, R, Mihovilovič, M, Muangma, N, Camacho, CM, Musson, J, Myers, K, Oh, Y, Carmignotto, MP, Perdrisat, C, Phillips, S, Piasetzky, E, Pierce, J, Punjabi, V, Qiang, Y, Reimer, PE, Roblin, Y, Ron, G, Rondon, O, Russo, G, Saenboonruang, K, Sawatzky, B, Shahinyan, A, Shneor, R, Širca, S, Sjoegren, J, Solvignon-Slifer, P, Sparveris, N, Sulkosky, V, Wesselmann, F, Yan, W, Yang, H, Yao, H, Ye, Z, Yurov, M, Zhang, Y, Zhao, YX & Zheng, X 2022, 'Proton spin structure and generalized polarizabilities in the strong quantum chromodynamics regime', Nature Physics, vol. 18, no. 12, pp. 1441-1446. https://doi.org/10.1038/s41567-022-01781-y

TY - JOUR

T1 - Proton spin structure and generalized polarizabilities in the strong quantum chromodynamics regime

AU - Ruth, D.

AU - Zielinski, R.

AU - Gu, C.

AU - Allada (Cummings), M.

AU - Badman, T.

AU - Huang, M.

AU - Liu, J.

AU - Zhu, P.

AU - Allada, K.

AU - Zhang, J.

AU - Camsonne, A.

AU - Chen, J. P.

AU - Slifer, K.

AU - Aniol, K.

AU - Annand, J.

AU - Arrington, J.

AU - Averett, T.

AU - Baghdasaryan, H.

AU - Bellini, V.

AU - Boeglin, W.

AU - Brock, J.

AU - Carlin, C.

AU - Chen, C.

AU - Cisbani, E.

AU - Crabb, D.

AU - Daniel, A.

AU - Day, D.

AU - Duve, R.

AU - Fassi, L. El

AU - Friedman, M.

AU - Fuchey, E.

AU - Gao, H.

AU - Gilman, R.

AU - Glamazdin, S.

AU - Gueye, P.

AU - Hafez, M.

AU - Han, Y.

AU - Hansen, O.

AU - Shabestari, M. Hashemi

AU - Hen, O.

AU - Higinbotham, D.

AU - Horn, T.

AU - Iqbal, S.

AU - Jensen, E.

AU - Kang, H.

AU - Keith, C. D.

AU - Kelleher, A.

AU - Keller, D.

AU - Khanal, H.

AU - Korover, I.

AU - Kumbartzki, G.

AU - Li, W.

AU - Lichtenstadt, J.

AU - Lindgren, R.

AU - Long, E.

AU - Malace, S.

AU - Markowitz, P.

AU - Maxwell, J.

AU - Meekins, D. M.

AU - Meziani, Z. E.

AU - McLean, C.

AU - Michaels, R.

AU - Mihovilovič, M.

AU - Muangma, N.

AU - Camacho, C. Munoz

AU - Musson, J.

AU - Myers, K.

AU - Oh, Y.

AU - Carmignotto, M. Pannunzio

AU - Perdrisat, C.

AU - Phillips, S.

AU - Piasetzky, E.

AU - Pierce, J.

AU - Punjabi, V.

AU - Qiang, Y.

AU - Reimer, P. E.

AU - Roblin, Y.

AU - Ron, G.

AU - Rondon, O.

AU - Russo, G.

AU - Saenboonruang, K.

AU - Sawatzky, B.

AU - Shahinyan, A.

AU - Shneor, R.

AU - Širca, S.

AU - Sjoegren, J.

AU - Solvignon-Slifer, P.

AU - Sparveris, N.

AU - Sulkosky, V.

AU - Wesselmann, F.

AU - Yan, W.

AU - Yang, H.

AU - Yao, H.

AU - Ye, Z.

AU - Yurov, M.

AU - Zhang, Y.

AU - Zhao, Y. X.

AU - Zheng, X.

PY - 2022/12

Y1 - 2022/12

N2 - The strong interaction is not well understood at low energies or for interactions with low momentum transfer. Chiral perturbation theory gives testable predictions for the nucleonic generalized polarizabilities, which are fundamental quantities describing the nucleon’s response to an external field. We report a measurement of the proton’s generalized spin polarizabilities extracted with a polarized electron beam and a polarized solid ammonia target in the region where chiral perturbation theory is expected to be valid. The investigated structure function g2 characterizes the internal spin structure of the proton. From its moments, we extract the longitudinal–transverse spin polarizability δLT and twist-3 matrix element and polarizability d2¯. Our results provide discriminating power between existing chiral perturbation theory calculations and will help provide a better understanding of this strong quantum chromodynamics regime.

AB - The strong interaction is not well understood at low energies or for interactions with low momentum transfer. Chiral perturbation theory gives testable predictions for the nucleonic generalized polarizabilities, which are fundamental quantities describing the nucleon’s response to an external field. We report a measurement of the proton’s generalized spin polarizabilities extracted with a polarized electron beam and a polarized solid ammonia target in the region where chiral perturbation theory is expected to be valid. The investigated structure function g2 characterizes the internal spin structure of the proton. From its moments, we extract the longitudinal–transverse spin polarizability δLT and twist-3 matrix element and polarizability d2¯. Our results provide discriminating power between existing chiral perturbation theory calculations and will help provide a better understanding of this strong quantum chromodynamics regime.

UR - https://www.scopus.com/pages/publications/85139950284

U2 - 10.1038/s41567-022-01781-y

DO - 10.1038/s41567-022-01781-y

M3 - Article

AN - SCOPUS:85139950284

SN - 1745-2473

VL - 18

SP - 1441

EP - 1446

JO - Nature Physics

JF - Nature Physics

IS - 12

ER -

Proton spin structure and generalized polarizabilities in the strong quantum chromodynamics regime

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