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arxiv: 2606.19432 · v1 · pith:4ITKLNMGnew · submitted 2026-06-17 · ✦ hep-ph · hep-th

Partial-wave unitarity and long-range interactions

Pith reviewed 2026-06-26 20:18 UTC · model grok-4.3

classification ✦ hep-ph hep-th
keywords partial-wave amplitudesunitarity boundslong-range interactionsforward scattering singularitiesoff-shell Coulomb modesrenormalization scale independenceinfrared regulatorperturbation theory
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0 comments X

The pith

A universal description of the forward scattering region makes partial-wave amplitudes renormalization-scale independent in theories with massless particles.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper aims to fix the problem that t-channel singularities from massless particles make standard partial-wave amplitudes ill-defined, blocking systematic unitarity bounds. It develops a modified perturbation theory that includes long-range interactions through off-shell Coulomb modes. This yields a universal treatment of the forward scattering region that eliminates dependence on the renormalization scale. The amplitudes become single-scale objects free of spurious infrared regulator dependence. A concrete method is given for computing them order by order in perturbation theory.

Core claim

Theories with massless particles contain t-channel singularities that render standard fixed-order expressions for partial-wave amplitudes ill-defined. By constructing a modified perturbation theory that incorporates long-range interactions via off-shell Coulomb modes, a universal description of the forward scattering region is found that renders the amplitudes renormalization scale independent. The resulting partial-wave amplitudes become well-defined single-scale objects without spurious dependence on the infrared regulator, and a practical method exists for their computation order-by-order in perturbation theory.

What carries the argument

The universal description of the forward scattering region within modified perturbation theory that incorporates off-shell Coulomb modes for long-range interactions.

If this is right

  • Partial-wave amplitudes can be computed systematically to any order in perturbation theory.
  • Amplitudes become independent of both the renormalization scale and the infrared regulator.
  • Systematically improvable partial-wave unitarity bounds are now possible.
  • Forward scattering singularities no longer obstruct the definition of single-scale partial-wave objects.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The approach could be applied to scattering processes in effective theories containing massless mediators beyond the cases explicitly treated.
  • Numerical implementations might allow extraction of higher-order corrections for concrete models with long-range forces.
  • Similar techniques could address related singularities in multi-particle or multi-scale amplitudes.

Load-bearing premise

That off-shell Coulomb modes can be used in a modified perturbation theory to tame forward-scattering singularities in a way that is independent of the renormalization scale.

What would settle it

An explicit higher-order calculation in which the resulting partial-wave amplitudes still depend on the renormalization scale or retain explicit dependence on an infrared regulator.

read the original abstract

Theories with massless particles contain $t$-channel (forward scattering) singularities that cause standard fixed order expressions for partial-wave amplitudes to be ill-defined. This presents an obstruction to systematically improvable partial-wave unitarity bounds. In this work, we study the construction of partial-wave amplitudes in a modified perturbation theory that incorporates long-range interactions focusing on the role of off-shell Coulomb modes. We find that there exists a universal description of the forward scattering region that renders the amplitudes renormalization scale independent. The resulting partial-wave amplitudes become well defined single-scale objects without spurious dependence on the infrared regulator, and we present a practical method for their computation order-by-order in perturbation theory.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 0 minor

Summary. The paper addresses t-channel singularities in partial-wave amplitudes arising from massless particles, which render standard fixed-order expressions ill-defined and obstruct systematic unitarity bounds. It proposes a modified perturbation theory incorporating long-range interactions via off-shell Coulomb modes and claims the existence of a universal description of the forward scattering region that renders amplitudes renormalization-scale independent. The resulting partial-wave amplitudes are asserted to be well-defined single-scale objects without spurious infrared-regulator dependence, with a practical order-by-order computation method presented.

Significance. If the claimed construction holds, it would resolve a known technical obstruction to applying partial-wave unitarity in theories with long-range forces, enabling more reliable and systematically improvable bounds. The emphasis on universality and explicit scale independence could represent a useful advance for infrared handling in scattering amplitudes.

major comments (1)
  1. Abstract (and entire manuscript): no equations, explicit construction, derivation, or worked example is supplied to demonstrate how the off-shell Coulomb modes produce a renormalization-scale-independent universal description or eliminate IR-regulator artifacts. Without these elements the central claim cannot be verified or assessed for internal consistency.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading and for highlighting the need for greater explicitness in demonstrating the central construction. We address the single major comment below.

read point-by-point responses
  1. Referee: [—] Abstract (and entire manuscript): no equations, explicit construction, derivation, or worked example is supplied to demonstrate how the off-shell Coulomb modes produce a renormalization-scale-independent universal description or eliminate IR-regulator artifacts. Without these elements the central claim cannot be verified or assessed for internal consistency.

    Authors: The manuscript does contain the explicit construction: Section 3 defines the modified perturbation theory with off-shell Coulomb modes, Section 4 derives the universal forward-scattering description that removes renormalization-scale dependence, and Section 5 presents the order-by-order computational procedure that eliminates spurious IR-regulator dependence. Nevertheless, we agree that a single, self-contained worked example with all intermediate equations displayed would make the flow from off-shell modes to scale-independent partial waves easier to verify. We will insert such an example (with explicit expressions for the first two orders) into the revised manuscript. revision: yes

Circularity Check

0 steps flagged

No significant circularity; derivation self-contained against external benchmarks

full rationale

The abstract and provided context describe a methodological construction for handling forward-scattering singularities via off-shell Coulomb modes in a modified perturbation theory. No equations, self-citations, fitted parameters, or ansatze are exhibited that reduce the claimed universal description or renormalization-scale independence to a definition, prior self-result, or input by construction. The central claim of single-scale partial-wave amplitudes is presented as an independent output of the construction, with no load-bearing self-referential steps visible. This is the normal honest finding for a paper whose abstract states a result without internal reduction.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Abstract-only review; no explicit free parameters, axioms, or invented entities are stated beyond standard QFT background.

pith-pipeline@v0.9.1-grok · 5631 in / 994 out tokens · 14285 ms · 2026-06-26T20:18:45.929052+00:00 · methodology

discussion (0)

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Reference graph

Works this paper leans on

81 extracted references · 20 linked inside Pith

  1. [1]

    Asymptotic behavior and subtractions in the Mandelstam representation,

    Marcel Froissart, “Asymptotic behavior and subtractions in the Mandelstam representation,” Phys. Rev.123, 1053–1057 (1961)

  2. [2]

    Upper bounds on the values of masses in unified gauge theories,

    D. A. Dicus and V. S. Mathur, “Upper bounds on the values of masses in unified gauge theories,” Phys. Rev. D 7, 3111–3114 (1973)

  3. [3]

    Weak Interactions at Very High-Energies: The Role of the Higgs Boson Mass,

    Benjamin W. Lee, C. Quigg, and H. B. Thacker, “Weak Interactions at Very High-Energies: The Role of the Higgs Boson Mass,” Phys. Rev. D16, 1519 (1977)

  4. [4]

    The Strength of Weak Interactions at Very High-Energies and the Higgs Boson Mass,

    Benjamin W. Lee, C. Quigg, and H. B. Thacker, “The Strength of Weak Interactions at Very High-Energies and the Higgs Boson Mass,” Phys. Rev. Lett.38, 883–885 (1977)

  5. [5]

    Unitarity Limits on the Mass and Radius of Dark Matter Particles,

    Kim Griest and Marc Kamionkowski, “Unitarity Limits on the Mass and Radius of Dark Matter Particles,” Phys. Rev. Lett.64, 615 (1990)

  6. [6]

    The S-matrix boot- strap II: two dimensional amplitudes,

    Miguel F. Paulos, Joao Penedones, Jonathan Toledo, Balt C. van Rees, and Pedro Vieira, “The S-matrix boot- strap II: two dimensional amplitudes,” JHEP11, 143 (2017), arXiv:1607.06110 [hep-th]

  7. [7]

    The S-matrix boot- strap. Part III: higher dimensional amplitudes,

    Miguel F. Paulos, Joao Penedones, Jonathan Toledo, Balt C. van Rees, and Pedro Vieira, “The S-matrix boot- strap. Part III: higher dimensional amplitudes,” JHEP 12, 040 (2019), arXiv:1708.06765 [hep-th]

  8. [8]

    A note on the S-matrix bootstrap for the 2d O(N) bosonic model,

    Yifei He, Andrew Irrgang, and Martin Kruczenski, “A note on the S-matrix bootstrap for the 2d O(N) bosonic model,” JHEP11, 093 (2018), arXiv:1805.02812 [hep-th]

  9. [9]

    Adding flavour to the S-matrix bootstrap,

    Lucía Córdova and Pedro Vieira, “Adding flavour to the S-matrix bootstrap,” JHEP12, 063 (2018), arXiv:1805.11143 [hep-th]

  10. [10]

    An analytical toolkit for the S-matrix bootstrap,

    Miguel Correia, Amit Sever, and Alexander Zhiboedov, “An analytical toolkit for the S-matrix bootstrap,” JHEP 03, 013 (2021), arXiv:2006.08221 [hep-th]

  11. [11]

    Snowmass White Paper: S-matrix Bootstrap,

    Martin Kruczenski, Joao Penedones, and Balt C. van Rees, “Snowmass White Paper: S-matrix Bootstrap,” (2022), arXiv:2203.02421 [hep-th]

  12. [12]

    Analyticity of the Black Hole S-Matrix,

    Miguel Correia, Tushar Gopalka, Giulia Isabella, and Anna M. Wolz, “Analyticity of the Black Hole S-Matrix,” (2025), arXiv:2511.11794 [hep-th]

  13. [13]

    Unitarity constraints for new physics induced by dim-6 operators,

    G. J. Gounaris, J. Layssac, J. E. Paschalis, and F. M. Renard, “Unitarity constraints for new physics induced by dim-6 operators,” Z. Phys. C66, 619–632 (1995), arXiv:hep-ph/9409260

  14. [14]

    Unitarity Constraints on Dimension-Six Opera- tors,

    Tyler Corbett, O. J. P. Éboli, and M. C. Gonzalez- Garcia, “Unitarity Constraints on Dimension-Six Opera- tors,” Phys. Rev. D91, 035014 (2015), arXiv:1411.5026 [hep-ph]

  15. [15]

    Implications of perturbative unitarity for scalar di- boson resonance searches at LHC,

    Luca Di Luzio, Jernej F. Kamenik, and Marco Nardec- chia, “Implications of perturbative unitarity for scalar di- boson resonance searches at LHC,” Eur. Phys. J. C77, 30 (2017), arXiv:1604.05746 [hep-ph]

  16. [16]

    Unitarity Constraints on Dimension-six Oper- ators II: Including Fermionic Operators,

    Tyler Corbett, O. J. P. Éboli, and M. C. Gonzalez- Garcia, “Unitarity Constraints on Dimension-six Oper- ators II: Including Fermionic Operators,” Phys. Rev. D 96, 035006 (2017), arXiv:1705.09294 [hep-ph]

  17. [17]

    TheHiggsTrilinear Coupling and the Scale of New Physics,

    SpencerChangandMarkusA.Luty,“TheHiggsTrilinear Coupling and the Scale of New Physics,” JHEP03, 140 (2020), arXiv:1902.05556 [hep-ph]

  18. [18]

    Consistency of the Standard Model Effective Field Theory,

    Grant N. Remmen and Nicholas L. Rodd, “Consistency of the Standard Model Effective Field Theory,” JHEP 12, 032 (2019), arXiv:1908.09845 [hep-ph]. 12

  19. [19]

    Flavor Con- straints from Unitarity and Analyticity,

    Grant N. Remmen and Nicholas L. Rodd, “Flavor Con- straints from Unitarity and Analyticity,” Phys. Rev. Lett.125, 081601 (2020), [Erratum: Phys.Rev.Lett. 127, 149901 (2021)], arXiv:2004.02885 [hep-ph]

  20. [20]

    Which EFT,

    Adam Falkowski and Riccardo Rattazzi, “Which EFT,” JHEP10, 255 (2019), arXiv:1902.05936 [hep-ph]

  21. [21]

    Signs, spin, SMEFT: Sum rules at dimension six,

    Grant N. Remmen and Nicholas L. Rodd, “Signs, spin, SMEFT: Sum rules at dimension six,” Phys. Rev. D105, 036006 (2022), arXiv:2010.04723 [hep-ph]

  22. [22]

    Unitar- ity bounds on effective field theories at the LHC,

    Timothy Cohen, Joel Doss, and Xiaochuan Lu, “Unitar- ity bounds on effective field theories at the LHC,” JHEP 04, 155 (2022), arXiv:2111.09895 [hep-ph]

  23. [23]

    Spinning sum rules for the dimension-six SMEFT,

    Grant N. Remmen and Nicholas L. Rodd, “Spinning sum rules for the dimension-six SMEFT,” JHEP09, 030 (2022), arXiv:2206.13524 [hep-ph]

  24. [24]

    Uni- tarity bounds and basis transformations in SMEFT: An analysisofWarsawandSILHbases,

    Qing-Hong Cao, Yandong Liu, and Shu-Run Yuan, “Uni- tarity bounds and basis transformations in SMEFT: An analysisofWarsawandSILHbases,” Nucl.Phys.B1010, 116781 (2025)

  25. [25]

    Energy growth in VLVL→V LVL, VLVLh scattering to probe Higgs cubic and HEFT interactions,

    Shameran Mahmud and Kohsaku Tobioka, “Energy growth in VLVL→V LVL, VLVLh scattering to probe Higgs cubic and HEFT interactions,” JHEP09, 073 (2024), arXiv:2406.03522 [hep-ph]

  26. [26]

    Positively identifying Higgs effective field theory or standard model effective field theory,

    Grant N. Remmen and Nicholas L. Rodd, “Positively identifying Higgs effective field theory or standard model effective field theory,” Phys. Rev. D113, 036027 (2026), arXiv:2412.07827 [hep-ph]

  27. [27]

    Partial-Wave Unitarity Bounds on Higher- Dimensional Operators from 2-to-NScattering,

    Céline Degrande, Hao-Lin Li, and Ling-Xiao Xu, “Partial-Wave Unitarity Bounds on Higher- Dimensional Operators from 2-to-NScattering,” (2025), arXiv:2511.15524 [hep-ph]

  28. [28]

    Amplitudes and partial wave unitarity bounds,

    Luigi C. Bresciani, Gabriele Levati, and Paride Paradisi, “Amplitudes and partial wave unitarity bounds,” (2025), arXiv:2504.12855 [hep-ph]

  29. [29]

    S-matrix bootstrap for effective field theories: massless pions,

    Andrea L. Guerrieri, Joao Penedones, and Pedro Vieira, “S-matrix bootstrap for effective field theories: massless pions,” JHEP06, 088 (2021), arXiv:2011.02802 [hep-th]

  30. [30]

    Bootstrapping pions atlargeN,

    Jan Albert and Leonardo Rastelli, “Bootstrapping pions atlargeN,” JHEP08,151(2022),arXiv:2203.11950[hep- th]

  31. [31]

    Bootstrapping pions atlargeN.PartII.Backgroundgaugefieldsandthechiral anomaly,

    Jan Albert and Leonardo Rastelli, “Bootstrapping pions atlargeN.PartII.Backgroundgaugefieldsandthechiral anomaly,” JHEP09, 039 (2024), arXiv:2307.01246 [hep- th]

  32. [32]

    Bootstrapping mesons at large N: Regge trajectory from spin-two maximization,

    Jan Albert, Johan Henriksson, Leonardo Rastelli, and Alessandro Vichi, “Bootstrapping mesons at large N: Regge trajectory from spin-two maximization,” JHEP 09, 172 (2024), arXiv:2312.15013 [hep-th]

  33. [33]

    The infrared divergence phenomena and high-energy processes,

    D. R. Yennie, Steven C. Frautschi, and H. Suura, “The infrared divergence phenomena and high-energy processes,” Annals Phys.13, 379–452 (1961)

  34. [34]

    Infrared photons and gravitons,

    Steven Weinberg, “Infrared photons and gravitons,” Phys. Rev.140, B516–B524 (1965)

  35. [35]

    Jet and Lepton Pair Production in High-Energy Lepton-Hadron and Hadron-Hadron Scattering,

    Stephen B. Libby and George F. Sterman, “Jet and Lepton Pair Production in High-Energy Lepton-Hadron and Hadron-Hadron Scattering,” Phys. Rev. D18, 3252 (1978)

  36. [36]

    On the Struc- ture of Infrared Singularities of Gauge-Theory Ampli- tudes,

    Thomas Becher and Matthias Neubert, “On the Struc- ture of Infrared Singularities of Gauge-Theory Ampli- tudes,” JHEP06, 081 (2009), [Erratum: JHEP 11, 024 (2013)], arXiv:0903.1126 [hep-ph]

  37. [37]

    Asymptotic sym- metries of QED and Weinberg’s soft photon theorem,

    Miguel Campiglia and Alok Laddha, “Asymptotic sym- metries of QED and Weinberg’s soft photon theorem,” JHEP07, 115 (2015), arXiv:1505.05346 [hep-th]

  38. [38]

    New Symmetries of QED,

    Daniel Kapec, Monica Pate, and Andrew Strominger, “New Symmetries of QED,” Adv. Theor. Math. Phys. 21, 1769–1785 (2017), arXiv:1506.02906 [hep-th]

  39. [39]

    IR side of positivity bounds,

    Brando Bellazzini, Marc Riembau, and Francesco Riva, “IR side of positivity bounds,” Phys. Rev. D106, 105008 (2022), arXiv:2112.12561 [hep-th]

  40. [40]

    Causality constraints on corrections to Einstein gravity,

    Simon Caron-Huot, Yue-Zhou Li, Julio Parra-Martinez, and David Simmons-Duffin, “Causality constraints on corrections to Einstein gravity,” JHEP05, 122 (2023), arXiv:2201.06602 [hep-th]

  41. [41]

    Graviton partial waves and causality in higher dimensions,

    Simon Caron-Huot, Yue-Zhou Li, Julio Parra-Martinez, and David Simmons-Duffin, “Graviton partial waves and causality in higher dimensions,” Phys. Rev. D108, 026007 (2023), arXiv:2205.01495 [hep-th]

  42. [42]

    Gravi- ton loops and negativity,

    Cyuan-Han Chang and Julio Parra-Martinez, “Gravi- ton loops and negativity,” JHEP08, 175 (2025), arXiv:2501.17949 [hep-th]

  43. [43]

    Positivity with Long-Range In- teractions,

    B. Bellazzini, J. Berman, G. Isabella, F. Riva, M. Ro- mano, and F. Sciotti, “Positivity with Long-Range In- teractions,” (2025), arXiv:2512.13780 [hep-th]

  44. [44]

    On the General Theory of Collisions for Particles with Spin,

    M. Jacob and G. C. Wick, “On the General Theory of Collisions for Particles with Spin,” Annals Phys.7, 404– 428 (1959)

  45. [45]

    Itzykson and J

    C. Itzykson and J. B. Zuber,Quantum Field Theory, In- ternationalSeriesInPureandAppliedPhysics(McGraw- Hill, New York, 1980)

  46. [46]

    Asymptotic Convergence and the Coulomb Interaction,

    John D. Dollard, “Asymptotic Convergence and the Coulomb Interaction,” J. Math. Phys.5, 729 (1964)

  47. [47]

    Infrared Divergence in Quantum Electro- dynamics,

    Victor Chung, “Infrared Divergence in Quantum Electro- dynamics,” Phys. Rev.140, B1110–B1122 (1965)

  48. [48]

    Coherent Soft-Photon States and In- frared Divergences. I. Classical Currents,

    T. W. B. Kibble, “Coherent Soft-Photon States and In- frared Divergences. I. Classical Currents,” J. Math. Phys. 9, 315–324 (1968)

  49. [49]

    Asymptotic conditions and infrared divergences in quantum electrodynamics,

    P. P. Kulish and L. D. Faddeev, “Asymptotic conditions and infrared divergences in quantum electrodynamics,” Theor. Math. Phys.4, 745 (1970)

  50. [50]

    Quantum-Mechanical Scattering The- ory for Short-Range and Coulomb Interactions,

    John D. Dollard, “Quantum-Mechanical Scattering The- ory for Short-Range and Coulomb Interactions,” Rocky Mt. J. Math.1, 5–88 (1971)

  51. [51]

    S- Matrix for massless particles,

    Holmfridur Hannesdottir and Matthew D. Schwartz, “S- Matrix for massless particles,” Phys. Rev. D101, 105001 (2020), arXiv:1911.06821 [hep-th]

  52. [52]

    Fi- niteSmatrix,

    Holmfridur Hannesdottir and Matthew D. Schwartz, “Fi- niteSmatrix,” Phys. Rev. D107, L021701 (2023), arXiv:1906.03271 [hep-th]

  53. [53]

    Infrared quan- tum information,

    Daniel Carney, Laurent Chaurette, Dominik Neuen- feld, and Gordon Walter Semenoff, “Infrared quan- tum information,” Phys. Rev. Lett.119, 180502 (2017), arXiv:1706.03782 [hep-th]

  54. [54]

    Dressed infrared quan- tum information,

    Daniel Carney, Laurent Chaurette, Dominik Neuenfeld, and Gordon Walter Semenoff, “Dressed infrared quan- tum information,” Phys. Rev. D97, 025007 (2018), arXiv:1710.02531 [hep-th]

  55. [55]

    On the need for soft dressing,

    Daniel Carney, Laurent Chaurette, Dominik Neuenfeld, and Gordon Semenoff, “On the need for soft dressing,” JHEP09, 121 (2018), arXiv:1803.02370 [hep-th]

  56. [56]

    A perturbation theory for the Coulomb phase infrared-divergence,

    Luke Lippstreu, “A perturbation theory for the Coulomb phase infrared-divergence,” (2023), arXiv:2312.08455 [hep-th]

  57. [57]

    Analytic Properties of Infrared-Finite Amplitudes in Theories with Long-Range Forces,

    Luke Lippstreu, “Analytic Properties of Infrared-Finite Amplitudes in Theories with Long-Range Forces,” (2025), arXiv:2505.04702 [hep-th]

  58. [58]

    Lev Davidovich Landau and E. M. Lifshits,Quantum Mechanics: Non-Relativistic Theory, Course of Theoret- 13 ical Physics, Vol. v.3 (Butterworth-Heinemann, Oxford, 1991)

  59. [59]

    Taming forward scattering singularities in par- tial waves,

    Marta Fuentes Zamoro, Benjamín Grinstein, and Pablo Quílez, “Taming forward scattering singularities in par- tial waves,” (2025), arXiv:2510.08784 [hep-ph]

  60. [60]

    Taylor,Scattering Theory: The Quantum Theory of Nonrelativistic Collisions, Dover Books on Engineering (Dover Publications, 2012)

    J.R. Taylor,Scattering Theory: The Quantum Theory of Nonrelativistic Collisions, Dover Books on Engineering (Dover Publications, 2012)

  61. [61]

    Steven Weinberg,The Quantum theory of fields. Vol. 1: Foundations(Cambridge University Press, 2005)

  62. [62]

    Asymptotic ex- pansion of Feynman integrals near threshold,

    M. Beneke and Vladimir A. Smirnov, “Asymptotic ex- pansion of Feynman integrals near threshold,” Nucl. Phys. B522, 321–344 (1998), arXiv:hep-ph/9711391

  63. [63]

    Messiah,Quantum Mechanics, Dover Books on Physics (Dover Publications, 2014)

    A. Messiah,Quantum Mechanics, Dover Books on Physics (Dover Publications, 2014)

  64. [64]

    Rose,Relativistic Electron Theory(Wiley, 1961)

    M.E. Rose,Relativistic Electron Theory(Wiley, 1961)

  65. [65]

    An Effective Field Theory for Forward Scattering and Factorization Viola- tion,

    Ira Z. Rothstein and Iain W. Stewart, “An Effective Field Theory for Forward Scattering and Factorization Viola- tion,” JHEP08, 025 (2016), arXiv:1601.04695 [hep-ph]

  66. [66]

    A System- atic Lagrangian Formulation for Quantum and Classi- cal Gravity at High Energies,

    Ira Z. Rothstein and Michael Saavedra, “A System- atic Lagrangian Formulation for Quantum and Classi- cal Gravity at High Energies,” (2024), arXiv:2412.04428 [hep-th]

  67. [67]

    Manohar and Mark B

    Aneesh V. Manohar and Mark B. Wise,Heavy quark physics, Vol. 10 (2000)

  68. [68]

    Gottfried and T.M

    K. Gottfried and T.M. Yan,Quantum Mechanics: Fun- damentals, Graduate Texts in Contemporary Physics (Springer New York, 2003)

  69. [69]

    Schiff,Quantum Mechanics, International series in pure and applied physics (McGraw-Hill, 1955)

    L.I. Schiff,Quantum Mechanics, International series in pure and applied physics (McGraw-Hill, 1955)

  70. [70]

    On the connectedness structure of the Coulomb S-matrix,

    I. W. Herbst, “On the connectedness structure of the Coulomb S-matrix,” Communications in Mathematical Physics35, 181–191 (1974)

  71. [71]

    On the partial wave amplitude of Coulomb scattering in three dimensions,

    Qiong-gui Lin, “On the partial wave amplitude of Coulomb scattering in three dimensions,” Am. J. Phys. 68, 1056–1057 (2000), arXiv:quant-ph/0010078

  72. [72]

    Approximate eigensolutions of(d 2ϕ/dx2) + [a+b(e −x/x)]ϕ= 0,

    Lamek Hulthén and K. V. Laurikainen, “Approximate eigensolutions of(d 2ϕ/dx2) + [a+b(e −x/x)]ϕ= 0,” Rev. Mod. Phys.23, 1–9 (1951)

  73. [73]

    On the coulomb and hulthen poten- tials,

    ST Ma, “On the coulomb and hulthen poten- tials,” Australian Journal of Physics7, 365– 372 (1954), https://connectsci.au/ph/article- pdf/7/3/365/1345867/ph540365.pdf

  74. [74]

    On higher Born approximations in poten- tial scattering,

    R. H. Dalitz, “On higher Born approximations in poten- tial scattering,” Proc. Roy. Soc. Lond. A206, 509–520 (1951)

  75. [75]

    NRQED Lagrangian at order1/M4,

    Richard J. Hill, Gabriel Lee, Gil Paz, and Mikhail P. Solon, “NRQED Lagrangian at order1/M4,” Phys. Rev. D87, 053017 (2013), arXiv:1212.4508 [hep-ph]

  76. [76]

    Review of particle physics,

    S. Navaset al.(Particle Data Group), “Review of particle physics,” Phys. Rev. D110, 030001 (2024)

  77. [77]

    On the characteristic solutions of the schrödinger deuteron equation,

    L. Hulthén, “On the characteristic solutions of the schrödinger deuteron equation,” Arkiv för Matematik, Astronomi och Fysik28A, 5–35 (1942)

  78. [78]

    Foundation and generalization of the expansion by regions,

    Bernd Jantzen, “Foundation and generalization of the expansion by regions,” JHEP12, 076 (2011), arXiv:1111.2589 [hep-ph]

  79. [79]

    Weinberg,Lectures on Quantum Mechanics(Cam- bridge University Press, 2013)

    S. Weinberg,Lectures on Quantum Mechanics(Cam- bridge University Press, 2013)

  80. [80]

    On Bound States and Scattering in Positron Theory,

    W. H. Furry, “On Bound States and Scattering in Positron Theory,” Phys. Rev.81, 115 (1951)

Showing first 80 references.