Multipole structure of the nucleon tensor form factors
Pith reviewed 2026-06-30 13:23 UTC · model grok-4.3
The pith
Rotational 1/N_c corrections in the chiral quark-soliton model supply the missing flavor components of nucleon tensor multipole form factors.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Within the chiral quark-soliton model based on the 1/N_c expansion, the rotational 1/N_c corrections provide the leading nonvanishing contributions to the flavor components of the tensor multipole form factors that are absent at leading order, thereby completing the flavor decomposition at the present order. The model yields the numerical values g_T^{u+d}=0.81, κ_T^{u-d}=1.97, and E_T^{u+d}(0)=5.98; the isoscalar quantities are dominated by valence quarks while the isovector anomalous tensor magnetic moment receives a sizable Dirac-sea contribution. The corresponding form factors fall monotonically with increasing -t.
What carries the argument
Rotational 1/N_c corrections within the chiral quark-soliton model, which generate the previously vanishing flavor components of the tensor multipole form factors.
If this is right
- The isoscalar tensor charge and quadrupole moment are governed primarily by valence quarks.
- The isovector anomalous tensor magnetic moment receives a sizable contribution from the Dirac sea.
- All examined tensor form factors decrease monotonically with increasing momentum transfer.
- The isovector anomalous tensor magnetic form factor exhibits a pronounced falloff at small |t| due to the Dirac sea.
Where Pith is reading between the lines
- These results suggest that any model of nucleon tensor structure omitting 1/N_c rotational effects will miss essential flavor asymmetries.
- The separation of valence and sea contributions could be tested by comparing with flavor-tagged lattice simulations at similar pion masses.
- The momentum dependence implies that low-Q^2 experiments are especially sensitive to sea-quark effects in the tensor dipole channel.
Load-bearing premise
The chiral quark-soliton model with parameters fixed to reproduce known physics accurately represents the nucleon's tensor multipole structure once rotational corrections are included.
What would settle it
A lattice QCD calculation or experimental extraction that finds the isoscalar tensor charge g_T^{u+d} substantially different from 0.81 would contradict the reported values.
Figures
read the original abstract
We investigate the multipole structure of the nucleon tensor form factors within the chiral quark-soliton model based on the $1/N_c$ expansion. Extending the previous leading-order analysis~\cite{Ghim:2025gqo}, we include the rotational $1/N_c$ corrections. These corrections provide the leading nonvanishing contributions to the flavor components that are absent at leading order, thereby completing the flavor decomposition of the tensor multipole form factors at the present order. We numerically evaluate the isoscalar tensor charge, the isovector anomalous tensor magnetic moment, and the isoscalar tensor quadrupole moment, obtaining $g_T^{u+d}=0.81$, $\kappa_T^{u-d}=1.97$, and $E_T^{u+d}(0)=5.98$, respectively. The isoscalar tensor charge and quadrupole moment are mainly governed by the valence-quark contribution, whereas the isovector anomalous tensor magnetic moment receives a sizable Dirac-sea contribution. We also examine the momentum-transfer dependence of the corresponding form factors. They decrease monotonically with increasing $-t$. In particular, the isovector anomalous tensor magnetic form factor shows a pronounced falloff in the small-$|t|$ region, reflecting the importance of the Dirac sea in the tensor dipole structure.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript extends a prior leading-order analysis of nucleon tensor form factors in the chiral quark-soliton model by incorporating rotational 1/N_c corrections. It claims these corrections supply the leading nonvanishing contributions to flavor components absent at leading order, thereby completing the flavor decomposition of the tensor multipole form factors at the working order. Numerical evaluations within the model yield g_T^{u+d}=0.81, κ_T^{u-d}=1.97, and E_T^{u+d}(0)=5.98; the isoscalar quantities are valence-dominated while the isovector anomalous magnetic moment receives a sizable Dirac-sea contribution. The momentum dependence of the form factors is also examined and shown to decrease monotonically with -t.
Significance. Within the framework of the chiral quark-soliton model, the work supplies a consistent completion of the flavor decomposition at O(1/N_c) and isolates the relative importance of valence versus sea contributions to different multipoles. The concrete numerical outputs and their Q^2 dependence furnish model-specific predictions that can be compared against other effective approaches or lattice results. The model dependence inherently limits broader QCD implications, but the internal consistency of the 1/N_c treatment is a clear strength of the calculation.
minor comments (2)
- The abstract and numerical results section report specific values (g_T^{u+d}=0.81, κ_T^{u-d}=1.97, E_T^{u+d}(0)=5.98) without error bars, variation over the soliton parameters (constituent mass, size), or explicit quantification of the size of the rotational corrections relative to the leading-order results of the cited prior work. Including a brief sensitivity table or discussion would improve the robustness of the presented numbers.
- A short table or paragraph directly comparing the new O(1/N_c) results to the leading-order values from Ref. [Ghim:2025gqo] would clarify the impact of the rotational corrections on each multipole.
Simulated Author's Rebuttal
We thank the referee for the positive assessment of our work and the recommendation of minor revision. No specific major comments were provided in the report.
Circularity Check
No significant circularity; model-internal evaluation
full rationale
The paper explicitly frames all results as numerical evaluations inside the chiral quark-soliton model with 1/N_c expansion, extending a prior leading-order calculation by the same authors. The central claim—that rotational corrections supply the first non-vanishing contributions to certain flavor components—is a direct consequence of the model's 1/N_c counting rules applied at the next order, not a reduction of outputs to inputs by construction. Numerical values (g_T^{u+d}=0.81 etc.) are presented as model outputs, not as independent predictions or first-principles results. No self-citation is load-bearing for an external uniqueness theorem, no ansatz is smuggled, and no fitted parameter is relabeled as a prediction. The derivation chain remains self-contained within the stated effective model.
Axiom & Free-Parameter Ledger
free parameters (1)
- soliton parameters (constituent mass, size)
axioms (2)
- domain assumption The 1/N_c expansion organizes corrections to leading-order soliton results for tensor form factors.
- domain assumption Chiral symmetry and the Dirac sea are correctly implemented in the model for tensor operators.
Reference graph
Works this paper leans on
-
[1]
N.-Y. Ghim, H.-Y. Won, J.-Y. Kim, and H.-C. Kim, Phys. Rev. D111, 074024 (2025), arXiv:2501.12241 [hep-ph]
-
[2]
S. L. Adler, E. W. Colglazier, Jr., J. B. Healy, I. Kar- liner, J. Lieberman, Y. J. Ng, and H.-S. Tsao, Phys. Rev. D11, 3309 (1975)
1975
-
[3]
R. L. Jaffe and X.-D. Ji, Phys. Rev. Lett.67, 552 (1991)
1991
-
[4]
R. L. Jaffe and X.-D. Ji, Nucl. Phys. B375, 527 (1992)
1992
-
[5]
H.-x. He and X.-D. Ji, Phys. Rev. D52, 2960 (1995), arXiv:hep-ph/9412235
work page internal anchor Pith review Pith/arXiv arXiv 1995
-
[6]
Low Energy Tests of the Weak Interaction
J. Erler and M. J. Ramsey-Musolf, Prog. Part. Nucl. Phys.54, 351 (2005), arXiv:hep-ph/0404291
work page internal anchor Pith review Pith/arXiv arXiv 2005
-
[7]
Electric dipole moments as probes of new physics
M. Pospelov and A. Ritz, Annals Phys.318, 119 (2005), arXiv:hep-ph/0504231
work page internal anchor Pith review Pith/arXiv arXiv 2005
-
[8]
Tests of the standard electroweak model in beta decay
N. Severijns, M. Beck, and O. Naviliat-Cuncic, Rev. Mod. Phys.78, 991 (2006), arXiv:nucl-ex/0605029
work page internal anchor Pith review Pith/arXiv arXiv 2006
-
[9]
Beta Decays and Non-Standard Interactions in the LHC Era
V. Cirigliano, S. Gardner, and B. Holstein, Prog. Part. Nucl. Phys.71, 93 (2013), arXiv:1303.6953 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2013
-
[10]
Beyond-Standard-Model Tensor Interaction and Hadron Phenomenology
A. Courtoy, S. Baeßler, M. Gonz´ alez-Alonso, and S. Liuti, Phys. Rev. Lett.115, 162001 (2015), arXiv:1503.06814 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2015
-
[11]
Bhattacharya, V
T. Bhattacharya, V. Cirigliano, S. D. Cohen, R. Gupta, A. Joseph, H.-W. Lin, and B. Yoon (Precision Neu- tron Decay Matrix Elements (PNDME) Collaboration), Phys. Rev. D92, 094511 (2015)
2015
-
[12]
New physics searches in nuclear and neutron $\beta$ decay
M. Gonz´ alez-Alonso, O. Naviliat-Cuncic, and N. Sev- erijns, Prog. Part. Nucl. Phys.104, 165 (2019), arXiv:1803.08732 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2019
-
[13]
C. Antelet al., Eur. Phys. J. C83, 1122 (2023), arXiv:2305.01715 [hep-ph]
-
[14]
Constraints on Dark Matter from Colliders
J. Goodman, M. Ibe, A. Rajaraman, W. Shepherd, T. M. P. Tait, and H.-B. Yu, Phys. Rev. D82, 116010 9 (2010), arXiv:1008.1783 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2010
-
[15]
From quarks to nucleons in dark matter direct detection
F. Bishara, J. Brod, B. Grinstein, and J. Zupan, JHEP 11, 059, arXiv:1707.06998 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv
- [16]
- [17]
-
[18]
A. Glick-Magid, Phys. Rev. D110, L051701 (2024), arXiv:2312.08339 [hep-ph]
- [19]
-
[20]
J. P. Ralston and D. E. Soper, Nucl. Phys. B152, 109 (1979)
1979
-
[21]
Kodaira, S
J. Kodaira, S. Matsuda, K. Sasaki, and T. Uematsu, Nucl. Phys. B159, 99 (1979)
1979
-
[22]
Artru and M
X. Artru and M. Mekhfi, Z. Phys. C45, 669 (1990)
1990
-
[23]
A. P. Bukhvostov, E. A. Kuraev, and L. N. Lipatov, Sov. Phys. JETP60, 22 (1984)
1984
-
[24]
J. L. Cortes, B. Pire, and J. P. Ralston, Z. Phys. C55, 409 (1992)
1992
-
[25]
Transverse-Spin and Transverse-Momentum Effects in High-Energy Processes
V. Barone, F. Bradamante, and A. Martin, Prog. Part. Nucl. Phys.65, 267 (2010), arXiv:1011.0909 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2010
-
[26]
C. A. Aidala, S. D. Bass, D. Hasch, and G. K. Mallot, Rev. Mod. Phys.85, 655 (2013), arXiv:1209.2803 [hep- ph]
work page internal anchor Pith review Pith/arXiv arXiv 2013
-
[27]
Diehl, Prog
S. Diehl, Prog. Part. Nucl. Phys.133, 104069 (2023)
2023
-
[28]
L. W. Whitlow, E. M. Riordan, S. Dasu, S. Rock, and A. Bodek, Phys. Lett. B282, 475 (1992)
1992
-
[29]
PERTURBATIVE QCD AND NUCLEON STRUCTURE FUNCTIONS.
J. Kodaira, Prog. Theor. Phys. Suppl.120, 37 (1995), arXiv:hep-ph/9501381
work page internal anchor Pith review Pith/arXiv arXiv 1995
-
[30]
A. V. Efremov, K. Goeke, and P. Schweitzer, Eur. Phys. J. C35, 207 (2004), arXiv:hep-ph/0403124
work page internal anchor Pith review Pith/arXiv arXiv 2004
-
[31]
Baroneet al.(PAX), (2005), arXiv:hep-ex/0505054
V. Baroneet al.(PAX), (2005), arXiv:hep-ex/0505054
-
[32]
M. Anselmino, V. Barone, A. Drago, and N. N. Nikolaev, Phys. Lett. B594, 97 (2004), arXiv:hep- ph/0403114
-
[33]
Drell-Yan processes, transversity and light-cone wavefunctions
B. Pasquini, M. Pincetti, and S. Boffi, Phys. Rev. D76, 034020 (2007), arXiv:hep-ph/0612094
work page internal anchor Pith review Pith/arXiv arXiv 2007
-
[34]
A. Airapetianet al.(HERMES), Phys. Rev. Lett.94, 012002 (2005), arXiv:hep-ex/0408013
work page internal anchor Pith review Pith/arXiv arXiv 2005
-
[35]
V. Y. Alexakhinet al.(COMPASS), Phys. Rev. Lett. 94, 202002 (2005), arXiv:hep-ex/0503002
work page internal anchor Pith review Pith/arXiv arXiv 2005
-
[36]
Transversity and Collins functions from SIDIS and e+e- data
M. Anselmino, M. Boglione, U. D’Alesio, A. Kotzinian, F. Murgia, A. Prokudin, and C. Turk, Phys. Rev. D75, 054032 (2007), arXiv:hep-ph/0701006
work page internal anchor Pith review Pith/arXiv arXiv 2007
-
[37]
Update on transversity and Collins functions from SIDIS and e+ e- data
M. Anselmino, M. Boglione, U. D’Alesio, A. Kotzinian, F. Murgia, A. Prokudin, and S. Melis, Nucl. Phys. B Proc. Suppl.191, 98 (2009), arXiv:0812.4366 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2009
-
[38]
Simultaneous extraction of transversity and Collins functions from new SIDIS and e+e- data
M. Anselmino, M. Boglione, U. D’Alesio, S. Melis, F. Murgia, and A. Prokudin, Phys. Rev. D87, 094019 (2013), arXiv:1303.3822 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2013
-
[39]
Z.-B. Kang, A. Prokudin, P. Sun, and F. Yuan, Phys. Rev. D91, 071501 (2015), arXiv:1410.4877 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2015
- [40]
-
[41]
R. Seidlet al.(Belle), Phys. Rev. D78, 032011 (2008), [Erratum: Phys.Rev.D 86, 039905 (2012)], arXiv:0805.2975 [hep-ex]
work page internal anchor Pith review Pith/arXiv arXiv 2008
-
[42]
Realistic estimate of valence transversity distributions from inclusive dihadron production
M. Radici, A. Courtoy, A. Bacchetta, and M. Guagnelli, JHEP05, 123, arXiv:1503.03495 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv
-
[43]
Z. Ye, N. Sato, K. Allada, T. Liu, J.-P. Chen, H. Gao, Z.-B. Kang, A. Prokudin, P. Sun, and F. Yuan, Phys. Lett. B767, 91 (2017), arXiv:1609.02449 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2017
-
[44]
H.-W. Lin, W. Melnitchouk, A. Prokudin, N. Sato, and H. Shows, Phys. Rev. Lett.120, 152502 (2018), arXiv:1710.09858 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[45]
C. Cocuzza, A. Metz, D. Pitonyak, A. Prokudin, N. Sato, and R. Seidl (JAM), Phys. Rev. Lett.132, 091901 (2024), arXiv:2306.12998 [hep-ph]
-
[46]
C. Cocuzza, A. Metz, D. Pitonyak, A. Prokudin, N. Sato, and R. Seidl (Jefferson Lab Angular Mo- mentum (JAM)), Phys. Rev. D109, 034024 (2024), arXiv:2308.14857 [hep-ph]
-
[47]
Accessing nucleon transversity with one-point energy correlators
M.-S. Gao, Z.-B. Kang, W. Li, and D. Y. Shao, (2025), arXiv:2509.15809 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2025
-
[48]
S. Aoki, M. Doui, T. Hatsuda, and Y. Kuramashi, Phys. Rev. D56, 433 (1997), arXiv:hep-lat/9608115
work page internal anchor Pith review Pith/arXiv arXiv 1997
-
[49]
Transverse spin structure of the nucleon from lattice QCD simulations
M. G¨ ockeler, P. H¨ agler, R. Horsley, Y. Nakamura, D. Pleiter, P. E. L. Rakow, A. Sch¨ afer, G. Schierholz, H. St¨ uben, and J. M. Zanotti (QCDSF, UKQCD), Phys. Rev. Lett.98, 222001 (2007), arXiv:hep-lat/0612032
work page internal anchor Pith review Pith/arXiv arXiv 2007
-
[50]
C. Alexandrouet al., Phys. Rev. D95, 114514 (2017), [Erratum: Phys.Rev.D 96, 099906 (2017)], arXiv:1703.08788 [hep-lat]
work page internal anchor Pith review Pith/arXiv arXiv 2017
-
[51]
Flavor diagonal tensor charges of the nucleon from 2+1+1 flavor lattice QCD
R. Gupta, B. Yoon, T. Bhattacharya, V. Cirigliano, Y.-C. Jang, and H.-W. Lin, Phys. Rev. D98, 091501 (2018), arXiv:1808.07597 [hep-lat]
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[52]
Nucleon charges with dynamical overlap fermions
N. Yamanaka, S. Hashimoto, T. Kaneko, and H. Ohki (JLQCD), Phys. Rev. D98, 054516 (2018), arXiv:1805.10507 [hep-lat]
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[53]
C. Alexandrou, S. Bacchio, M. Constantinou, J. Finken- rath, K. Hadjiyiannakou, K. Jansen, G. Koutsou, and A. Vaquero Aviles-Casco, Phys. Rev. D102, 054517 (2020), arXiv:1909.00485 [hep-lat]
-
[54]
C. Alexandrou, M. Constantinou, K. Hadjiyiannakou, K. Jansen, and F. Manigrasso, Phys. Rev. D104, 054503 (2021), arXiv:2106.16065 [hep-lat]
- [55]
-
[56]
Alexandrou, S
C. Alexandrou, S. Bacchio, M. Constantinou, P. Di- mopoulos, J. Finkenrath, R. Frezzotti, K. Had- jiyiannakou, K. Jansen, B. Kostrzewa, G. Koutsou, G. Spanoudes, and C. Urbach, Phys. Rev. D107, 054504 (2023)
2023
-
[57]
M. Rodekamp, M. Engelhardt, J. R. Green, S. Krieg, S. Liuti, S. Meinel, J. W. Negele, A. Pochinsky, and S. Syritsyn, Phys. Rev. D109, 074508 (2024), arXiv:2401.05360 [hep-lat]
-
[58]
J.-H. Wang, Z.-C. Hu, X. Ji, X. Jiang, Y. Su, P. Sun, and Y.-B. Yang, (2025), arXiv:2511.02326 [hep-lat]
- [59]
- [60]
- [61]
- [62]
-
[63]
A. V. Belitsky and A. V. Radyushkin, Phys. Rept.418, 1 (2005), arXiv:hep-ph/0504030
work page internal anchor Pith review Pith/arXiv arXiv 2005
-
[64]
Generalized parton distributions and the structure of the nucleon
S. Boffi and B. Pasquini, Riv. Nuovo Cim.30, 387 (2007), arXiv:0711.2625 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2007
-
[65]
GPD phenomenology and DVCS fitting - Entering the high-precision era
K. Kumericki, S. Liuti, and H. Moutarde, Eur. Phys. J. A52, 157 (2016), arXiv:1602.02763 [hep-ph]. 10
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[66]
d’Hose, S
N. d’Hose, S. Niccolai, and A. Rostomyan, Eur. Phys. J. A52, 151 (2016)
2016
-
[67]
Transverse Deformation of Parton Distributions and Transversity Decomposition of Angular Momentum
M. Burkardt, Phys. Rev. D72, 094020 (2005), arXiv:hep-ph/0505189
work page internal anchor Pith review Pith/arXiv arXiv 2005
-
[68]
Spin densities in the transverse plane and generalized transversity distributions
M. Diehl and P. H¨ agler, Eur. Phys. J. C44, 87 (2005), arXiv:hep-ph/0504175
work page internal anchor Pith review Pith/arXiv arXiv 2005
-
[69]
Chiral-odd generalized parton distributions in constituent quark models
B. Pasquini, M. Pincetti, and S. Boffi, Phys. Rev. D72, 094029 (2005), arXiv:hep-ph/0510376
work page internal anchor Pith review Pith/arXiv arXiv 2005
-
[70]
C. Lorce, B. Pasquini, and M. Vanderhaeghen, JHEP 05, 041, arXiv:1102.4704 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv
- [71]
- [72]
-
[73]
Chiral-odd generalized parton distributions for the low-lying octet baryons
N. Kaur and H. Dahiya, Phys. Rev. D112, 074024 (2025), arXiv:2506.02464 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2025
-
[74]
X. Luan and Z. Lu, Phys. Rev. D110, 034021 (2024), arXiv:2404.13962 [hep-ph]
-
[75]
T. M. Aliev, K. Azizi, and M. Savci, Phys. Rev. D84, 076005 (2011), arXiv:1108.2019 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2011
-
[76]
H.-C. Kim, M. V. Polyakov, and K. Goeke, Phys. Rev. D53, 4715 (1996), arXiv:hep-ph/9509283
work page internal anchor Pith review Pith/arXiv arXiv 1996
-
[77]
H.-C. Kim, M. V. Polyakov, and K. Goeke, Phys. Lett. B387, 577 (1996), arXiv:hep-ph/9604442
work page internal anchor Pith review Pith/arXiv arXiv 1996
-
[78]
M. Wakamatsu, Phys. Rev. D79, 014033 (2009), arXiv:0811.4196 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2009
-
[79]
Tensor charges of light baryons in the Infinite Momentum Frame
C. Lorce, Phys. Rev. D79, 074027 (2009), arXiv:0708.4168 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2009
-
[80]
T. Ledwig, A. Silva, and H.-C. Kim, Phys. Rev. D82, 054014 (2010), arXiv:1007.1355 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2010
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.