scholarly journals Estimate of the Sixth-Order Contribution to the Anomalous Magnetic Moment of the Electron

1968 ◽  
Vol 168 (5) ◽  
pp. 1562-1567 ◽  
Author(s):  
Ronald G. Parsons
Keyword(s):  
Magnetic Moment ◽  
Anomalous Magnetic Moment ◽  
Sixth Order ◽  
Order Contribution

A sixth order contribution to the electron anomalous magnetic moment

1975 ◽  
Vol 57 (5) ◽  
pp. 460-462 ◽  
Author(s):  
R. Barbieri ◽  
M. Caffo ◽  
E. Remiddi
Keyword(s):  
Magnetic Moment ◽  
Anomalous Magnetic Moment ◽  
Sixth Order ◽  
Order Contribution

scholarly journals On sixth-order corrections to the anomalous magnetic moment of the electron

1970 ◽  
Vol 33 (8) ◽  
pp. 605-606 ◽  
Author(s):  
A. De Rújula ◽  
B. Lautrup ◽  
A. Peterman
Keyword(s):  
Magnetic Moment ◽  
Anomalous Magnetic Moment ◽  
Sixth Order

scholarly journals Hadronic Leading Order Contribution to the Muon g-2

2018 ◽  
Vol 179 ◽  
pp. 01016
Author(s):  
Daisuke Nomura
Keyword(s):  
Experimental Data ◽  
Standard Model ◽  
Magnetic Moment ◽  
Anomalous Magnetic Moment ◽  
Leading Order ◽  
Muon Anomalous Magnetic Moment ◽  
Order Contribution ◽  
Quark Contribution ◽  
The Standard Model ◽  
Vacuum Polarisation

We calculate the Standard Model (SM) prediction for the muon anomalous magnetic moment. By using the latest experimental data for e+e- → hadrons as input to dispersive integrals, we obtain the values of the leading order (LO) and the next-to-leading-order (NLO) hadronic vacuum polarisation contributions as ahad, LO VPμ = (693:27 ± 2:46) × 10-10 and ahad, NLO VP μ = (_9.82 ± 0:04) × 1010-10, respectively. When combined with other contributions to the SM prediction, we obtain aμ(SM) = (11659182:05 ± 3.56) × 10-10; which is deviated from the experimental value by Δaμ(exp) _ aμ(SM) = (27.05 ± 7.26) × 10-10. This means that there is a 3.7 σ discrepancy between the experimental value and the SM prediction. We also discuss another closely related quantity, the running QED coupling at the Z-pole, α(M2 Z). By using the same e+e- → hadrons data as input, our result for the 5-flavour quark contribution to the running QED coupling at the Z pole is Δ(5)had(M2 Z) = (276.11 ± 1.11) × 10-4, from which we obtain Δ(M2 Z) = 128.946 ± 0.015.

The anomalous magnetic moment of the electron in QED: Some more sixth order contributions in the dispersive approach

1978 ◽  
Vol 144 (2-3) ◽  
pp. 329-348 ◽  
Author(s):  
R. Barbieri ◽  
M. Caffo ◽  
E. Remiddi ◽  
S. Turrini ◽  
D. Oury
Keyword(s):  
Magnetic Moment ◽  
Anomalous Magnetic Moment ◽  
Sixth Order ◽  
Dispersive Approach

More corrections to the sixth-order anomalous magnetic moment of the muon

1980 ◽  
Vol 6 (1) ◽  
pp. 3-6 ◽  
Author(s):  
Morten L. Laursen ◽  
Mark A. Samuel ◽  
Ashok K. Ray
Keyword(s):  
Magnetic Moment ◽  
Anomalous Magnetic Moment ◽  
Sixth Order
Sign in / Sign up

Export Citation Format

Share Document