Can the strong interactions between hadrons be determined using femtoscopy?
Pith reviewed 2026-05-22 20:34 UTC · model grok-4.3
The pith
Femtoscopic measurements of strong hadron interactions suffer from large intrinsic uncertainties due to non-universal source terms.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The interpretation of femtoscopic measurements suffers from a potentially large intrinsic uncertainty for strongly interacting particles such as nucleons, because the source term describing the production mechanism of hadron pairs cannot be treated as universal without introducing significant errors in the extracted interactions.
What carries the argument
The Koonin-Pratt formula, which relates measured two-hadron correlation functions to the relative wave function of an outgoing pair and a source term assumed to be universal across different interactions.
If this is right
- Extracted two-body strong interactions from femtoscopic data carry potentially large errors for nucleons and similar particles.
- The same source-term uncertainty affects attempts to determine three-body interactions using this technique.
- Phenomenological modeling of the source must be refined to account for dependence on the final-state interaction strength.
- Results for weakly interacting pairs may remain more reliable than those for strongly interacting ones.
Where Pith is reading between the lines
- Direct lattice QCD calculations of correlation functions without an assumed source could provide an independent check on extracted interactions.
- Varying collision systems or energies to map source variations experimentally might quantify the size of the uncertainty.
- Combining femtoscopic data with other observables, such as scattering lengths from different experiments, could help isolate interaction effects from source effects.
Load-bearing premise
The source term describing the production mechanism of hadron pairs is universal and can be modeled phenomenologically without introducing large uncertainties in the extracted interactions for strongly interacting particles.
What would settle it
A direct comparison of source parameters extracted from correlation data for nucleon pairs versus non-interacting pairs, or a microscopic calculation showing interaction-dependent changes in the effective source size or shape exceeding a few percent, would test whether the universality assumption holds.
Figures
read the original abstract
In the last decades, femtoscopic measurements from heavy-ion collisions have become a popular tool to investigate the strong interactions between hadrons. The key observables measured in such experiments are the two-hadron momentum correlations, which depend on the production mechanism of hadron pairs and the final-state interactions. Given the complexity of ultra-relativistic collision experiments, the source term describing the production mechanism can only be modeled phenomenologically based on numerous assumptions. The commonly employed approach for analyzing femtoscopic data relies on the Koonin-Pratt formula, which relates the measured correlation functions with the relative wave function of an outgoing hadron pair and a source term that is assumed to be universal. Here, we critically examine this universality assumption and show that for strongly interacting particles such as nucleons, the interpretation of femtoscopic measurements suffers from a potentially large intrinsic uncertainty. We also comment on the ongoing efforts to explore three-body interactions using this experimental technique.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript critically examines the Koonin-Pratt formula employed in femtoscopic analyses of heavy-ion collisions. It argues that the assumption of a universal source term for the production mechanism of hadron pairs is invalid for strongly interacting particles such as nucleons, leading to potentially large intrinsic uncertainties in the extracted strong-interaction parameters. The work contrasts phenomenological source modeling with the requirements imposed by final-state interactions and offers comments on ongoing three-body interaction studies.
Significance. If the non-universality argument holds, the result would caution against over-interpreting femtoscopic correlation functions as direct probes of strong hadron interactions, particularly for nucleons, and would motivate more careful source modeling or alternative extraction methods. The paper provides a timely critical perspective on a widely used technique without introducing new data or derivations.
major comments (1)
- [§4] §4 (or equivalent section presenting the nucleon example): the claim of 'potentially large intrinsic uncertainty' is supported by contrasting source assumptions but would benefit from a quantitative bound or sensitivity study showing how much the extracted scattering length or effective range shifts under plausible non-universal source variations.
minor comments (2)
- [Abstract] The abstract states the conclusion without referencing the specific section or figure that demonstrates the non-universality; a cross-reference would improve readability.
- [Introduction] Notation for the source function S(r) and the wave function should be defined explicitly at first use to avoid ambiguity with standard femtoscopy literature.
Simulated Author's Rebuttal
We thank the referee for the careful reading of our manuscript and the constructive comment. We address the point raised below.
read point-by-point responses
-
Referee: [§4] §4 (or equivalent section presenting the nucleon example): the claim of 'potentially large intrinsic uncertainty' is supported by contrasting source assumptions but would benefit from a quantitative bound or sensitivity study showing how much the extracted scattering length or effective range shifts under plausible non-universal source variations.
Authors: We agree that a quantitative sensitivity study would strengthen the presentation of the intrinsic uncertainty. In the revised manuscript we will augment §4 with an explicit sensitivity analysis for the nucleon example. This will report the variation in the extracted scattering length and effective range obtained when the source function is varied across the range of non-universal profiles already contrasted in the text, thereby providing the requested quantitative bounds. revision: yes
Circularity Check
No significant circularity identified
full rationale
The paper critically examines the universality assumption in the Koonin-Pratt formula without presenting any derivation that reduces to fitted inputs or self-citations by construction. Its central argument contrasts phenomenological source modeling with final-state interaction requirements for nucleons to highlight potential uncertainty, relying on physical reasoning rather than self-definitional steps, fitted predictions, or load-bearing self-citations. No equations or claims in the provided text exhibit the enumerated circularity patterns, making the analysis self-contained against external benchmarks.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption The Koonin-Pratt formula relates measured correlation functions to the relative wave function and a universal source term.
Forward citations
Cited by 2 Pith papers
-
Analysis of the $D_0^*(2300)$ resonance from lattice QCD under chiral symmetry
Chiral symmetry corrections in lattice QCD fits shift the D0*(2300) resonance pole closer to the Dπ threshold and reduce its width, while coupled channels produce a two-pole structure.
-
Scattering and Femtoscopic Correlation Functions of the $\Sigma_c^{++}\pi^{+}$, $\Sigma_c^{0}\pi^{-}$ and $\Sigma_b^{+}\pi^{+}$ Systems
Theoretical predictions show that femtoscopic correlation functions for neutral Σ_c^0 π^- pairs best constrain isotensor strong interactions in charm and bottom sectors, while Coulomb repulsion diminishes discriminati...
Reference graph
Works this paper leans on
-
[1]
S. E. Koonin. Proton Pictures of High-Energy Nuclear Collisions. Phys. Lett. B , 70:43–47, 1977. doi:10.1016/ 0370-2693(77)90340-9
work page 1977
-
[2]
W. Bauer, C. K. Gelbke, and S. Pratt. Hadronic in- terferometry in heavy ion collisions. Ann. Rev. Nucl. Part. Sci. , 42:77–100, 1992. doi:10.1146/annurev.ns. 42.120192.000453
-
[3]
S. Pratt. What we are learning from correlation mea- surements. Nucl. Phys. A , 638:125–134, 1998. doi: 10.1016/S0375-9474(98)00407-2
-
[4]
Femtoscopy in Relativistic Heavy Ion Collisions: Two Decades of Progress
Michael Annan Lisa, Scott Pratt, Ron Soltz, and Urs Wiedemann. Femtoscopy in relativistic heavy ion col- lisions. Ann. Rev. Nucl. Part. Sci. , 55:357–402, 2005. arXiv:nucl-ex/0505014, doi:10.1146/annurev.nucl. 55.090704.151533
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1146/annurev.nucl 2005
-
[5]
L. Fabbietti, V. Mantovani Sarti, and O. Vazquez Doce. Study of the Strong Interaction Among Hadrons with Correlations at the LHC. Ann. Rev. Nucl. Part. Sci. , 71:377–402, 2021. arXiv:2012.09806, doi:10.1146/ annurev-nucl-102419-034438
-
[6]
Unveiling the strong inter- action among hadrons at the LHC
Alice Collaboration et al. Unveiling the strong inter- action among hadrons at the LHC. Nature, 588:232– 238, 2020. [Erratum: Nature 590, E13 (2021)]. arXiv: 2005.11495, doi:10.1038/s41586-020-3001-6
-
[7]
R. Lednicky and V. L. Lyuboshits. Final State Inter- action Effect on Pairing Correlations Between Particles with Small Relative Momenta. Yad. Fiz., 35:1316–1330, 1981
work page 1981
-
[8]
Finite-size effect on two-particle production in continuous and discrete spectrum
Richard Lednicky. Finite-size effects on two-particle pro- duction in continuous and discrete spectrum. Phys. Part. Nucl., 40:307–352, 2009. arXiv:nucl-th/0501065, doi:10.1134/S1063779609030034
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1134/s1063779609030034 2009
-
[10]
Roderick V. Reid, Jr. Local phenomenological nucleon- nucleon potentials. Annals Phys., 50:411–448, 1968. doi: 10.1016/0003-4916(68)90126-7
-
[11]
An accurate nucleon-nucleon potential with charge-independence breaking
Robert B. Wiringa, V. G. J. Stoks, and R. Schiavilla. An Accurate nucleon-nucleon potential with charge indepen- dence breaking. Phys. Rev. C , 51:38–51, 1995. arXiv: nucl-th/9408016, doi:10.1103/PhysRevC.51.38
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevc.51.38 1995
-
[12]
D. L. Mihaylov, V. Mantovani Sarti, O. W. Arnold, L. Fabbietti, B. Hohlweger, and A. M. Mathis. A femtoscopic Correlation Analysis Tool using the Schr¨ odinger equation (CATS). Eur. Phys. J. C , 78(5):394, 2018. arXiv:1802.08481, doi:10.1140/epjc/ s10052-018-5859-0
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1140/epjc/ 2018
-
[13]
Search for a common baryon source in high-multiplicity pp collisions at the LHC
Shreyasi Acharya et al. Search for a common baryon source in high-multiplicity pp collisions at the LHC. Phys. Lett. B , 811:135849, 2020. arXiv:2004.08018, doi:10.1016/j.physletb.2020.135849
-
[14]
S. Pratt. Validity of the smoothness assumption for calculating two-boson correlations in high-energy colli- sions. Phys. Rev. C , 56:1095–1098, 1997. doi:10.1103/ PhysRevC.56.1095
work page 1997
-
[15]
Final state interactions in two-particle interferometry
D. Anchishkin, Ulrich W. Heinz, and P. Renk. Final state interactions in two particle interferometry. Phys. Rev. C , 57:1428–1439, 1998. arXiv:nucl-th/9710051, doi:10.1103/PhysRevC.57.1428
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevc.57.1428 1998
-
[16]
Michael C. Birse. Potential problems with interpolating fields. Eur. Phys. J. A , 53(11):223, 2017. arXiv:1208. 4807, doi:10.1140/epja/i2017-12425-0
-
[17]
Lattice QCD approach to Nuclear Physics
Sinya Aoki, Takumi Doi, Tetsuo Hatsuda, Yoichi Ikeda, Takashi Inoue, Noriyoshi Ishii, Keiko Murano, Hidekatsu Nemura, and Kenji Sasaki. Lattice QCD approach to Nuclear Physics. PTEP, 2012:01A105, 2012. arXiv: 1206.5088, doi:10.1093/ptep/pts010
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1093/ptep/pts010 2012
-
[18]
H. Lehmann, K. Symanzik, and W. Zimmermann. On the formulation of quantized field theories. Nuovo Cim. , 1:205–225, 1955. doi:10.1007/BF02731765
-
[19]
Semilocal momentum-space regularized chiral two-nucleon potentials up to fifth order
P. Reinert, H. Krebs, and E. Epelbaum. Semilocal momentum-space regularized chiral two-nucleon poten- tials up to fifth order. Eur. Phys. J. A , 54(5):86, 2018. arXiv:1711.08821, doi:10.1140/epja/i2018-12516-4
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1140/epja/i2018-12516-4 2018
-
[20]
Exotic Hadrons from Heavy Ion Collisions
Sungtae Cho et al. Exotic hadrons from heavy ion collisions. Prog. Part. Nucl. Phys. , 95:279–322, 2017. arXiv:1702.00486, doi:10.1016/j.ppnp.2017.02.002
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1016/j.ppnp.2017.02.002 2017
-
[21]
Johann Haidenbauer and Ulf-G. Meißner. Exploring the Σ+p interaction by measurements of the correla- tion function. Phys. Lett. B , 829:137074, 2022. arXiv: 2109.11794, doi:10.1016/j.physletb.2022.137074
-
[22]
M. Albaladejo, A. Feijoo, J. Nieves, E. Oset, and I. Vida˜ na. Femtoscopy correlation functions and mass distributions from production experiments. Phys. Rev. D, 110(11):114052, 2024. arXiv:2410.08880, doi:10. 1103/PhysRevD.110.114052
-
[23]
P. U. Sauer. Can the charge symmetry of nuclear forces be confirmed by nucleon-nucleon scattering ex- periments? Phys. Rev. Lett. , 32:626–630, 1974. doi: 10.1103/PhysRevLett.32.626
-
[24]
Evgeny Epelbaum, Hans-Werner Hammer, and Ulf-G. Meißner. Modern Theory of Nuclear Forces. Rev. Mod. Phys., 81:1773–1825, 2009. arXiv:0811.1338, doi:10. 1103/RevModPhys.81.1773
work page internal anchor Pith review Pith/arXiv arXiv 2009
-
[25]
R. Machleidt and D. R. Entem. Chiral effective field theory and nuclear forces. Phys. Rept. , 503:1–75,
-
[26]
arXiv:1105.2919, doi:10.1016/j.physrep.2011. 02.001
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1016/j.physrep.2011 2011
-
[27]
Evgeny Epelbaum, Hermann Krebs, and Patrick Rein- 6 ert. High-precision nuclear forces from chiral EFT: State- of-the-art, challenges and outlook. Front. in Phys. , 8:98, 2020. arXiv:1911.11875, doi:10.3389/fphy. 2020.00098
-
[28]
Equivalence of Nonstatic Two-Pion-Exchange Nucleon-Nucleon Potentials
James Lewis Friar. Equivalence of nonstatic two pion exchange nucleon-nucleon potentials. Phys. Rev. C , 60:034002, 1999. arXiv:nucl-th/9901082, doi:10. 1103/PhysRevC.60.034002
work page internal anchor Pith review Pith/arXiv arXiv 1999
-
[29]
V. Bernard, E. Epelbaum, H. Krebs, and U.-G. Meißner. Subleading contributions to the chiral three-nucleon force II: Short-range terms and relativistic corrections. Phys. Rev. C , 84:054001, 2011. arXiv:1108.3816, doi:10. 1103/PhysRevC.84.054001
work page internal anchor Pith review Pith/arXiv arXiv 2011
-
[30]
See Supplemental Material at [URL]
-
[31]
Three-body forces and Efimov physics in nuclei and atoms
Shimpei Endo, Evgeny Epelbaum, Pascal Naidon, Yusuke Nishida, Kimiko Sekiguchi, and Yoshiro Taka- hashi. Three-body forces and Efimov physics in nuclei and atoms. Eur. Phys. J. A , 61(1):9, 2025. arXiv: 2405.09807, doi:10.1140/epja/s10050-024-01467-4
-
[32]
Towards the understanding of the genuine three-body interaction for p–p–p and p–p–Λ
Shreyasi Acharya et al. Towards the understanding of the genuine three-body interaction for p–p–p and p–p–Λ. Eur. Phys. J. A , 59(7):145, 2023. arXiv:2206.03344, doi:10.1140/epja/s10050-023-00998-6
-
[33]
Exploring the Strong Interac- tion of Three-Body Systems at the LHC
Shreyasi Acharya et al. Exploring the Strong Interac- tion of Three-Body Systems at the LHC. Phys. Rev. X , 14(3):031051, 2024. arXiv:2308.16120, doi:10.1103/ PhysRevX.14.031051
-
[34]
A. Kievsky, E. Garrido, M. Viviani, L. E. Marcucci, L. Serksnyte, and R. Del Grande. nnn and ppp correlation functions. Phys. Rev. C , 109(3):034006,
-
[35]
arXiv:2310.10428, doi:10.1103/PhysRevC.109. 034006
-
[36]
W. P. Abfalterer et al. Inadequacies of the nonrela- tivistic 3N Hamiltonian in describing the n + d total cross section. Phys. Rev. Lett. , 81:57–60, 1998. doi: 10.1103/PhysRevLett.81.57
-
[37]
W. N. Polyzou and W. Gl¨ ockle. Three-body interactions and on-shell equivalent two-body interactions. Few Body Syst., 9(2-3):97–121, 1990. doi:10.1007/BF01091701
-
[38]
P. Reinert, H. Krebs, and E. Epelbaum. Precision de- termination of pion-nucleon coupling constants using ef- fective field theory. Phys. Rev. Lett. , 126(9):092501,
-
[39]
arXiv:2006.15360, doi:10.1103/PhysRevLett. 126.092501
-
[40]
M. Gmitro, J. Kvasil, R. Lednicky, and V. L. Lyuboshits. On the Sensitivity of Nucleon-nucleon Correlations to the Form of Short Range Potential. Czech. J. Phys. B , 36:1281, 1986. doi:10.1007/BF01598029
-
[41]
Miguel Albaladejo, Alejandro Canoa, Juan Nieves, Jose Ram´ on Pel´ aez, Enrique Ruiz-Arriola, and Ja- cobo Ruiz de Elvira. The role of chiral symmetry and the non-ordinary κ/K ∗ 0 (700) nature in π±KS femtoscopic correlations. 3 2025. arXiv:2503.19746. 7 SUPPLEMENT AL MA TERIAL Scheme dependence in nuclear chiral EFT and phase equivalent NN potentials at ...
-
[42]
σ2 · (p′ 1 − p′ 2 − p1 + p2) + σ1 · (p′ 1 − p′ 2 − p1 + p2) σ2 · (p1 − p2 + p′ 1 − p′ 2) . (S5) Here, pi and p′ i denote the incoming and outgoing momenta of the nucleon i while Λb is the breakdown scale of chiral EFT, respectively. Note that in line with the commonly used notation, we do not show in Eq. (S5) the overall factor of (2 π)3 and the δ-functio...
-
[43]
H. Krebs and E. Epelbaum, Toward consistent nuclear interactions from chiral Lagrangians. II. Symmetry preserving regularization, Phys. Rev. C 110, no.4, 044004 (2024) . arXiv:2312.13932 [nucl-th], doi:10.1103/PhysRevC.110.044004. 11 [MeV]kcms 100 150 102 103 200 250 300 350 [mb]σ 125 150 175 200 225 250 [MeV]kcms -5 -5 5 5 0 0 [%]δσnd [%]δσnp neutron-deu...
-
[44]
H. Krebs and E. Epelbaum, Toward consistent nuclear interactions from chiral Lagrangians. I. The path-integral approach, Phys. Rev. C 110, no.4, 044003 (2024) . arXiv:2311.10893 [nucl-th], doi:10.1103/PhysRevC.110.044003
-
[46]
E. Epelbaum, W. Gl¨ ockle and U.-G. Meißner, Nuclear forces from chiral Lagrangians using the method of unitary transformation. 2. The two nucleon system, Nucl. Phys. A 671, 295-331 (2000) . arXiv:nucl-th/9910064 [nucl-th], doi:10.1016/S0375-9474(99)00821-0
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1016/s0375-9474(99)00821-0 2000
-
[47]
Nuclear forces in the chiral limit
E. Epelbaum, U.-G. Meißner and W. Gl¨ ockle, Nuclear forces in the chiral limit, Nucl. Phys. A 714, 535-574 (2003) . arXiv:nucl-th/0207089 [nucl-th], doi:10.1016/S0375-9474(02)01393-3
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1016/s0375-9474(02)01393-3 2003
-
[48]
Isospin-violating nucleon-nucleon forces using the method of unitary transformation
E. Epelbaum and U.-G. Meißner, Isospin-violating nucleon-nucleon forces using the method of unitary transformation, Phys. Rev. C 72, 044001 (2005) . arXiv:nucl-th/0502052 [nucl-th], doi:10.1103/PhysRevC.72.044001
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevc.72.044001 2005
-
[49]
Four-nucleon force in chiral effective field theory
E. Epelbaum, Four-nucleon force in chiral effective field theory, Phys. Lett. B 639, 456-461 (2006) , arXiv:nucl-th/0511025 [nucl-th], doi:10.1016/j.physletb.2006.06.046
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1016/j.physletb.2006.06.046 2006
-
[50]
Four-nucleon force using the method of unitary transformation
E. Epelbaum, Four-nucleon force using the method of unitary transformation, Eur. Phys. J. A 34, 197-214 (2007) arXiv:0710.4250 [nucl-th], doi:10.1140/epja/i2007-10496-0
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1140/epja/i2007-10496-0 2007
-
[51]
Subleading contributions to the chiral three-nucleon force I: long-range terms
V. Bernard, E. Epelbaum, H. Krebs and U.-G. Meißner, Subleading contributions to the chiral three-nucleon force. I. Long-range terms, Phys. Rev. C 77, 064004 (2008) . arXiv:0712.1967 [nucl-th], doi:10.1103/PhysRevC.77.064004
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevc.77.064004 2008
-
[52]
Chiral three-nucleon force at N^4LO I: Longest-range contributions
H. Krebs, A. Gasparyan and E. Epelbaum, Chiral three-nucleon force at N 4LO I: Longest-range contributions, Phys. Rev. C 85, 054006 (2012) . arXiv:1203.0067 [nucl-th], doi:10.1103/PhysRevC.85.054006
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevc.85.054006 2012
-
[53]
Chiral three-nucleon force at N^4LO II: Intermediate-range contributions
H. Krebs, A. Gasparyan and E. Epelbaum, Chiral three-nucleon force at N4LO II: Intermediate-range contributions, Phys. Rev. C 87, no.5, 054007 (2013) . arXiv:1302.2872 [nucl-th], doi:10.1103/PhysRevC.87.054007
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevc.87.054007 2013
-
[54]
S. K¨ olling, E. Epelbaum, H. Krebs and U.-G. Meißner, Two-pion exchange electromagnetic current in chiral effective field theory using the method of unitary transformation, Phys. Rev. C 80, 045502 (2009) . arXiv:0907.3437 [nucl-th], doi:10.1103/PhysRevC.80.045502
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevc.80.045502 2009
-
[55]
S. K¨ olling, E. Epelbaum, H. Krebs and U.-G. Meißner, Two-nucleon electromagnetic current in chiral effective field 12 theory: One-pion exchange and short-range contributions, Phys. Rev. C 84, 054008 (2011) . arXiv:1107.0602 [nucl-th], doi:10.1103/PhysRevC.84.054008
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevc.84.054008 2011
-
[56]
Nuclear axial current operators to fourth order in chiral effective field theory
H. Krebs, E. Epelbaum and U.-G. Meißner, Nuclear axial current operators to fourth order in chiral effective field theory, Annals Phys. 378, 317-395 (2017) . arXiv:1610.03569 [nucl-th], doi:10.1016/j.aop.2017.01.021
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1016/j.aop.2017.01.021 2017
-
[57]
Nuclear electromagnetic currents to fourth order in chiral effective field theory
H. Krebs, E. Epelbaum and U.-G. Meißner, Nuclear Electromagnetic Currents to Fourth Order in Chiral Effective Field Theory, Few Body Syst. 60, no.2, 31 (2019) . arXiv:1902.06839 [nucl-th], doi:10.1007/s00601-019-1500-5
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/s00601-019-1500-5 2019
-
[58]
H. Krebs, E. Epelbaum and U.-G. Meißner, Subleading contributions to the nuclear scalar isoscalar current, Eur. Phys. J. A 56, no.9, 240 (2020) . arXiv:2005.07433 [nucl-th], doi:10.1140/epja/s10050-020-00249-y
-
[59]
Krebs, Nuclear Currents in Chiral Effective Field Theory, Eur
H. Krebs, Nuclear Currents in Chiral Effective Field Theory, Eur. Phys. J. A 56, no.9, 234 (2020) . arXiv:2008.00974 [nucl-th], doi:10.1140/epja/s10050-020-00230-9
-
[60]
J. L. Friar, Pion Exchange Contributions to the Nuclear Charge, Current, and Hamiltonian Operators, Annals Phys. 104, 380-426 (1977) , doi:10.1016/0003-4916(77)90337-2
-
[61]
J. Adam, H. Goller and H. Arenhovel, Relativistic corrections and unitary equivalence in elastic electron deuteron scat- tering, Phys. Rev. C 48, 370-378 (1993) , doi:10.1103/PhysRevC.48.370
-
[62]
A. A. Filin, D. M¨ oller, V. Baru, E. Epelbaum, H. Krebs and P. Reinert, High-accuracy calculation of the deuteron charge and quadrupole form factors in chiral effective field theory, Phys. Rev. C 103, no.2, 024313 (2021) , arXiv:2009.08911 [nucl-th], doi:10.1103/PhysRevC.103.024313
-
[63]
L. Girlanda, A. Kievsky, L. E. Marcucci and M. Viviani, Unitary ambiguity of NN contact interactions and the 3N force, Phys. Rev. C 102, 064003 (2020) , arXiv:2007.04161 [nucl-th], doi:10.1103/PhysRevC.102.064003
-
[64]
L. Girlanda, E. Filandri, A. Kievsky, L. E. Marcucci and M. Viviani, Effect of the N3LO three-nucleon con- tact interaction on p-d scattering observables, Phys. Rev. C 107, no.6, L061001 (2023) , arXiv:2302.03468 [nucl-th], doi:10.1103/PhysRevC.107.L061001
-
[65]
E. Epelbaum, H. Krebs and P. Reinert, Semi-local Nuclear Forces From Chiral EFT: State-of-the-Art and Challenges, in Handbook of Nuclear Physics, edited by I. Tanihata, H. Toki, and T. Kajino (2022) pp. 1–25 , arXiv:2206.07072 [nucl-th], doi:dx.doi.org/10.1007/978-981-15-8818-1−54-1
-
[66]
Improved chiral nucleon-nucleon potential up to next-to-next-to-next-to-leading order
E. Epelbaum, H. Krebs and U.-G. Meißner, Improved chiral nucleon-nucleon potential up to next-to-next-to-next-to-leading order, Eur. Phys. J. A 51, no.5, 53 (2015) , arXiv:1412.0142 [nucl-th], doi:10.1140/epja/i2015-15053-8
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1140/epja/i2015-15053-8 2015
-
[67]
R. Machleidt, P. Liu, D. R. Entem and E. Ruiz Arriola, Renormalization of the leading-order chiral nucleon- nucleon interaction and bulk properties of nuclear matter, Phys. Rev. C 81, 024001 (2010) arXiv:0910.3942 [nucl-th], doi:10.1103/PhysRevC.81.024001
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevc.81.024001 2010
-
[68]
P. Reinert, Precision studies in the two-nucleon system using chiral effective field theory, PhD thesis, Ruhr University Bochum, 2022, doi:10.13154/294-9501
-
[69]
E. G. Kessler, Jr., The Deuteron Binding Energy and the Neutron Mass, Phys. Lett. A 255, 221 (1999) , doi:10.1016/S0375- 9601(99)00078-X
-
[70]
J. J. de Swart, C. P. F. Terheggen and V. G. J. Stoks, The Low-energy n p scattering parameters and the deuteron, Contribution to the 3rd International Symposium on Dubna Deuteron 95 , arXiv:nucl-th/9509032 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv
-
[71]
N. L. Rodning and L. D. Knutson, Asymptotic D-state to S-state ratio of the deuteron, Phys. Rev. C 41, 898-909 (1990) , doi:10.1103/PhysRevC.41.898
-
[72]
J. L. Friar, Measurability of the deuteron D state probability, Phys. Rev. C 20, 325-330 (1979) , doi:10.1103/PhysRevC.20.325
-
[73]
S. Binder et al. [LENPIC], Few-nucleon systems with state-of-the-art chiral nucleon-nucleon forces, Phys. Rev. C 93, no.4, 044002 (2016) , arXiv:1505.0721 [nucl-th], doi:10.1103/PhysRevC.93.044002
-
[74]
P. Maris et al. [LENPIC], Nuclear properties with semilocal momentum-space regularized chiral interactions beyond N2LO, Phys. Rev. C 106, no.6, 064002 (2022) , arXiv: 2206.13303 [nucl-th], doi:10.1103/PhysRevC.106.064002
-
[75]
P. W. Lisowski, R. E. Shamu, G. F. Auchampaugh, N. S. P. King, M. S. Moore, G. L. Morgan and T. S. Single- ton, Search for resonance structure in np total cross-section below 800 MeV, Phys. Rev. Lett. 49, 255-259 (1982) , doi:10.1103/PhysRevLett.49.255
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.