anomalous magnetic moment



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In perturbative quantum field theory, the magnetic moment of particles as predicted by classical field theory may receive corrections due to quantum effects. Such corrections are also called quantum anomalies, and hence one speaks of the anomalous magnetic moments, traditionally denoted by “g2g-2”.

The archetypical example is the anomalous magnetic moment of the electron in quantum electrodynamics, which is famous as the pQFT-prediction that matches experiment to an accuracy of about 10 1210^{-12} (e.g.Scharf 95, (3.10.20)).

Similarly there is the anomalous magenetic moment g μ2g_\mu - 2 of the muon and the other leptons.


In fact, the anomalous magnetic moment of the muon g μ2g_\mu - 2 has become notorious for apparently showing a noticeable discrepancy between theoretic prediction from the standard model of particle physics and its value as determined in experiment. The discrepancy is now found to have statistical significance around 3.5σ (DHMZ 17) or 4σ (Jegerlehner 18a). Recent measurements may even show a possible deviation around 2.5 σ for the electron’s anomalous magnetic moment (see Falkowski 18). Details depend on understanding of non-perturbative effects (Jegerlehner 18b, section 2).

In particular, there seems to be inconsistencies in the theoretical understanding of the relevant lattice QCD-computations:

graphics from Lehner-Meyer 20, Fig 14

If these experimental “anomalies” (in the sense of phenomenology) in the anomalous magnetic moment g μ2g_\mu - 2 (and possibly even in g e2g_e -2) are real (the established rule of thumb is that deviations are established once their statistical significance reaches 5σ, see here), they point to “new physics” beyond the standard model of particle physics.

In fact Lyons 13b argued that the detection-threshold of the statistical significance of anomalies here should be just 4σ, which would mean that they should already count as being detected:

table taken from Lyons 13b, p. 4

Together with the flavour anomalies, these anomalies relate to the flavour problem in the standard model of particle physics:

graphics from Crivellin-Hoferichter 20

(here “RR” refers to flavour anomalies in various channels, “aa” refers to anomalies in the the anomalous magnetic moments of the electron and the muon, “LFUV” is shoft for “Lepton Flavor Universality Violation”, and the numbers are the statistical significances of the effects seen)

Possible explanations for the anomomalies in the anomalous magnetic moments is the existence of leptoquarks (Bauer-Neubert 15, CCDM 16, Falkowski 17, Müller 18), which at the same time are a candidate for explaining the flavour anomalies (see also Chiang-Okada 17).


QED contributions

(…) for the electron see e.g. Scharf 95, section 3.10 (…)

Quantum gravity contributions

The further corrections of 1-loop perturbative quantum gravity to the anomalous magnetic moment of the electron and the muon have been computed in (Berends-Gastman 75) and found to be finite without need for renormalization. These Feynman diagrams contribute:

Axion contributions

Possible contributions to and xconstraints on g lep2g_{lep}-2 from hypothetical axions are discussed in ACGM 08, MMPP 16, BNT 17



Basic discussion:

  • Othmar Steinmann, What is the Magnetic Moment of the Electron?, Commun.Math.Phys. 237 (2003) 181-201 (arXiv:hep-ph/0211187)

  • Kirill Melnikov, Arkady Vainshtein, Theory of the Muon Anomalous Magnetic Moment, Springer Tracts in Modern Physics 216, 2006

  • Friedrich Jegerlehner, The Anomalous Magnetic Moment of the Muon, Springer Tracts in Modern Physics 226, Springer-Verlag Berlin Heidelberg, 2008

Discussion of detection-threshold for the statistical significance of anomalies:

See also

Comprehensive discussion for the muon:

  • T. Aoyama et al., The anomalous magnetic moment of the muon in the Standard Model (arXiv:2006.04822)

Experiment and deviation

Discussion of precision experiment and possible deviation from theory:

Relation to flavour anomalies

Possible explanation of the anomaly in the anomalous magnetic moments in terms of leptoquarks:

  • Martin Bauer, Matthias Neubert, One Leptoquark to Rule Them All: A Minimal Explanation for R D (*)R_{D^{(\ast)}}, R KR_K and (g2) μ(g-2)_\mu, Phys. Rev. Lett. 116, 141802 (2016) (arXiv:1511.01900)

  • Estefania Coluccio Leskow, Andreas Crivellin, Giancarlo D’Ambrosio, Dario Müller, (g2) μ(g-2)_\mu, Lepton Flavour Violation and Z Decays with Leptoquarks: Correlations and Future Prospects, Phys. Rev. D 95, 055018 (2017) (arXiv:1612.06858)

  • Anirban Biswas, Avirup Shaw, Reconciling dark matter, R K (*)R_{K^{(\ast)}} anomalies and (g2) μ(g-2)_\mu in an L μL τL_\mu-L_\tau scenario (arXiv:1903.08745)

  • Adam Falkowski, Leptoquarks strike back, November 2017

  • Cheng-Wei Chiang, Hiroshi Okada, A simple model for explaining muon-related anomalies and dark matter (arXiv:1711.07365)

  • Dario Müller, Leptoquarks in Flavour Physics, EPJ Web of Conferences 179, 01015 (2018) (arXiv:1801.03380)

  • Junichiro Kawamura, Stuart Raby, Andreas Trautner, Complete Vector-like Fourth Family and new U(1)U(1)' for Muon Anomalies (arXiv:1906.11297)

Further possible joint explanation of the anomalies observed in the muon anomalous magnetic moment and the flavour anomalies:

  • Geneviève Bélanger, Cédric Delaunay, Susanne Westhoff, A Dark Matter Relic From Muon Anomalies, Phys. Rev. D 92, 055021 (2015) (arXiv:1507.06660)

  • Cheng-Wei Chiang, Hiroshi Okada, A simple model for explaining muon-related anomalies and dark matter (arXiv:1711.07365)

  • Junichiro Kawamura, Stuart Raby, Andreas Trautner, Complete Vector-like Fourth Family and new U(1)U(1)' for Muon Anomalies (arXiv:1906.11297)

  • Lorenzo Calibbi, M.L. López-Ibáñez, Aurora Melis, Oscar Vives, Muon and electron g2g-2 and lepton masses in flavor models (arXiv:2003.06633)

  • A. S. de Jesus, S. Kovalenko, F. S. Queiroz, K. Sinha, C. Siqueira, Vector-Like Leptons and Inert Scalar Triplet: Lepton Flavor Violation, g2g-2 and Collider Searches (arXiv:2004.01200)

  • Shaikh Saad, Combined explanations of (g2) μ(g-2)_\mu, R D *R_{D^\ast}, R K *R_{K^\ast} anomalies in a two-loop radiative neutrino mass model (arXiv:2005.04352)

  • Da Huang, António P. Morais, Rui Santos, Anomalies in BB Decays and Muon g2g-2 from Dark Loops (arXiv:2007.05082)

  • K.S. Babu, P.S. Bhupal Dev, Sudip Jana, Anil Thapa, Unified Framework for BB-Anomalies, Muon g2g-2, and Neutrino Masses (arXiv:2009.01771)

  • Sang Quang Dinh, Hieu Minh Tran, Muon g2g-2 and semileptonic BB decays in BDW model with gauge kinetic mixing (arXiv:2011.07182)

Realization in F-theory of GUT-models with Z'-bosons and/or [leptoquarks]] addressing the flavour anomalies and the (g-2) anomalies:

  • Miguel Crispim Romao, Stephen F. King, George K. Leontaris, Non-universal ZZ' from Fluxed GUTs, Physics Letters B Volume 782, 10 July 2018, Pages 353-361 (arXiv:1710.02349)

  • A. Karozas, G. K. Leontaris, I. Tavellaris, N. D. Vlachos, On the LHC signatures of SU(5)×U(1)SU(5) \times U(1)' F-theory motivated models (arXiv:2007.05936)

QED contributions

The computation of the anomalous magnetic dipole moment of the electron in QED is spelled out (via causal perturbation theory) in

QCD contribution


Discussion of QCD contributions via lattice QCD:

  • Christoph Lehner, Aaron S. Meyer, Consistency of hadronic vacuum polarization between lattice QCD and the R-ratio (arXiv:2003.04177)

Via holographic QCD

Application of holographic QCD to anomalous magnetic moment of the muon:

  • Luigi Cappiello, What does Holographic QCD predict for anomalous (g2) μ(g-2)_\mu?, 2015 (pdf)

  • Josef Leutgeb, Anton Rebhan, Axial vector transition form factors in holographic QCD and their contribution to the anomalous magnetic moment of the muon (arXiv:1912.01596)

Gravity contributions

Corrections at 1-loop from quantum gravity are discussed in

  • F. A. Berends, R. Gastmans, Quantum gravity and the electron and muon anomalous magnetic moment, Phys. Lett. B55 Issue 3 Feb 1975 311-312 (doi:10.1016/0370-2693(75)90608-5)

This discussion is adapted to supergravity in

  • F. del Aguila, A. Culatti, R. Munoz-Tapia, M. Perez-Victoria, Supergravity corrections to (g2) l(g-2)_l in differential renormalization, Nuclear Physics B 504 (1997) 532-550 (arXiv:hep-ph/9702342)

Axion contributions

Contribution of hypothetical axions to the anomalous magnetic moment of the electron and muon in QED:

  • Yannis Semertzidis, Magnetic and Electric Dipole Moments in Storage Rings, chapter 6 of Markus Kuster, Georg Raffelt, Berta Beltrán (eds.), Axions: Theory, cosmology, and Experimental Searches, Lect. Notes Phys. 741 (Springer, Berlin Heidelberg 2008) (doi:10.1007/978-3-540-73518-2_2)

  • Roberta Armillis, Claudio Coriano, Marco Guzzi, Simone Morelli, Axions and Anomaly-Mediated Interactions: The Green-Schwarz and Wess-Zumino Vertices at Higher Orders and g-2 of the muon, JHEP 0810:034,2008 (arXiv:0808.1882)

  • W.J. Marciano, A. Masiero, P. Paradisi, M. Passera, Contributions of axion-like particles to lepton dipole moments, Phys. Rev. D 94, 115033 (2016) (arXiv:1607.01022)

  • Martin Bauer, Matthias Neubert, Andrea Thamm, Collider Probes of Axion-Like Particles, J. High Energ. Phys. (2017) 2017: 44. (arXiv:1708.00443, doi:10.1007/JHEP12(2017)044)

The basic relevant Feynman diagrams are worked out here:

Last revised on November 17, 2020 at 03:56:38. See the history of this page for a list of all contributions to it.