1977
DOI: 10.1016/0550-3213(77)90342-x
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Limit on mass differences in the Weinberg model

Abstract: Within the Weinberg model mass differences between members of a multiplet generate further mass differences between the neutral and charged vector bosons. The experimental situation on the Weinberg model leads to an upper limit of about 800 GeV on mass differences within a multiplet. No limit on the average mass can be deduced.

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Cited by 736 publications
(468 citation statements)
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References 5 publications
(3 reference statements)
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“…The former receives large fermionic contributions from the shift in the fine structure constant due to light fermions, ∆α ∝ log(m f /M Z ), a pure SM contribution. The latter involves the leading universal corrections induced by the mass splitting between fields in an isospin doublet [43],…”
Section: Complete One-loop Results In the Complex Mssmmentioning
confidence: 99%
“…The former receives large fermionic contributions from the shift in the fine structure constant due to light fermions, ∆α ∝ log(m f /M Z ), a pure SM contribution. The latter involves the leading universal corrections induced by the mass splitting between fields in an isospin doublet [43],…”
Section: Complete One-loop Results In the Complex Mssmmentioning
confidence: 99%
“…One of the applications of four-loop tadpoles mentioned at the beginning concerns a quantity of primary importance in the area of electroweak physics, namely the ρ parameter introduced by Veltman [15]. Defined as the ratio of the charged and neutral current strengths, it differs from its leading-order value of one, by a shift which can be expressed through the transverse parts of W and Z boson self-energies…”
Section: Introductionmentioning
confidence: 99%
“…A predominant role in this respect has to be assigned to the ρ-parameter [13], with loop contributions ∆ρ through vector-boson self-energies, which constitute the leading process-independent quantum corrections to electroweak precision observables, such as the prediction for ∆r, the M W -M Z interdependence, and the effective leptonic weak mixing angle, sin 2 θ eff . Radiative corrections to the electroweak precision observables within the MSSM have been extensively discussed (for a review see, e.g.…”
mentioning
confidence: 99%