“…(1) as well as the (numerically insignificant) term 3m 2 µ /(5M 2 W ) arising from the tree-level W propagator. The precise measurement of the muon lifetime and the equivalently precise calculation of ∆ QED [36,37] thus provide the accurate value G µ = (1.16637 ± 0.00001 × 10 −5 ) GeV −2 .…”
Section: Prediction For M W -Basic Entriesmentioning
We present the currently most accurate evaluation of the W boson mass, M W , in the Minimal Supersymmetric Standard Model (MSSM). The full complex phase dependence at the one-loop level, all available MSSM two-loop corrections as well as the full Standard Model result have been included. We analyse the impact of the different sectors of the MSSM at the one-loop level with a particular emphasis on the effect of the complex phases. We discuss the prediction for M W based on all known higher-order contributions in representative MSSM scenarios. Furthermore we obtain an estimate of the remaining theoretical uncertainty from unknown higher-order corrections. * email: Sven.Heinemeyer@cern.ch †
“…(1) as well as the (numerically insignificant) term 3m 2 µ /(5M 2 W ) arising from the tree-level W propagator. The precise measurement of the muon lifetime and the equivalently precise calculation of ∆ QED [36,37] thus provide the accurate value G µ = (1.16637 ± 0.00001 × 10 −5 ) GeV −2 .…”
Section: Prediction For M W -Basic Entriesmentioning
We present the currently most accurate evaluation of the W boson mass, M W , in the Minimal Supersymmetric Standard Model (MSSM). The full complex phase dependence at the one-loop level, all available MSSM two-loop corrections as well as the full Standard Model result have been included. We analyse the impact of the different sectors of the MSSM at the one-loop level with a particular emphasis on the effect of the complex phases. We discuss the prediction for M W based on all known higher-order contributions in representative MSSM scenarios. Furthermore we obtain an estimate of the remaining theoretical uncertainty from unknown higher-order corrections. * email: Sven.Heinemeyer@cern.ch †
“…(2.8) by performing a large momentum expansion of the imaginary part of propagator-type diagrams. The second order corrections to ∆q have been presented recently [10,15] for m e = 0. The result, ignoring the effects of tau loops, is…”
Section: The Muon Lifetime and The Fermi Coupling Constantmentioning
confidence: 99%
“…The total decay rate may be calculated directly as the imaginary part of muon self-energy diagrams and was done in Ref. [10]. In charge retention order terms in the numerators that are odd in the electron mass lead to a helicity flip along the internal electron line that causes the purely left-handed V−A vertices to annihilate.…”
Section: The Muon Lifetime and The Fermi Coupling Constantmentioning
The determination of the Fermi coupling constant, G F , is examined in the light of recently calculated 2-loop QED corrections and planned experiments to measure the muon lifetime to a level below 1 ppm. The methods used in the calculation of the QED corrections are described in detail. Sources of the dominant theoretical and experimental uncertainties are identified. Finally the incorporation of G F into analyses using the full electroweak Standard Model is discussed.
“…The O(α 2 ) corrections to µ decay have been completed recently [40]. The remaining uncertainty in G F is from the experimental input.…”
Section: Ew Model and Constraints On New Physicsmentioning
confidence: 99%
“…Martin, Outhwaite, Ryskin [32] 0.02741 ± 0.00019 includes new BES data Burkhardt & Pietrzyk [33] 0.02763 ± 0.00036 PQCD for √ s > 12 GeV de Troconiz & Yndurain [34] 0.02754 ± 0.00010 PQCD for s > 2 GeV 2 Jegerlehner [35] 0.02766 ± 0.00013 converted from MOM scheme (b) The Fermi constant, G F = 1.16637(1) × 10 −5 GeV −2 , determined from the muon lifetime formula [39,40], …”
Section: Renormalization and Radiative Correctionsmentioning
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