Add to ORKGWe use the SU(3) SU(2) U(1) renormalization-group equations to place upper limits on the scale where new physics beyond the standard model must emerge. Our bounds rely solely on the structure of the renormalization-group equations and on the magnitudes of heavy-quark masses. For example, if Σm2q>~(450 GeV)2, new physics must be found below 105 GeV
In the context of the radiative electroweak symmetry breaking scenario we investigate the implicatio...
We have searched for conceptually simple extensions of the standard model, and describe here a candi...
We use effective field theory to show that small increases in the up and down quark masses would mov...
An unavoidable condition for consistency of the standard model is that all quarks must be lighter th...
An unavoidable condition for consistency of the standard model is that all quarks must be lighter th...
The radiative mass structure of some Grand Unified Models is discussed. They contain fermions with S...
Discusses the viewpoint that the standard SU(3)*SU(2)*U(1) model is only a low-energy manifestation ...
The gauge symmetry of the Standard Model is SU(3)c×SU(2)L×U(1)Y for unknown reasons. One aspect that...
The origin of mass must lie in physics beyond the Standard Model. Dynamical electroweak symmetry bre...
In this talk we describe examples of renormalizable strongly interacting field theories where chiral...
If N=2 supersymmetry breaks to N=1 supersymmetry at an intermediate scale $m_2$ and then, later on, ...
3 pags., 1 tab.Since new Z bosons (Z) are predicted by many approaches to particle physics beyond th...
A short-distance heavy quark mass depends on two parameters, the renormalization scale mu controllin...
Motivated by recent experimental indications of large {nu}{sub {mu}} - {nu}{tau} mixing, we explore ...
Abstract Precision measurements of high energy top quarks at the LHC constitute a powerful probe of ...
In the context of the radiative electroweak symmetry breaking scenario we investigate the implicatio...
We have searched for conceptually simple extensions of the standard model, and describe here a candi...
We use effective field theory to show that small increases in the up and down quark masses would mov...
An unavoidable condition for consistency of the standard model is that all quarks must be lighter th...
An unavoidable condition for consistency of the standard model is that all quarks must be lighter th...
The radiative mass structure of some Grand Unified Models is discussed. They contain fermions with S...
Discusses the viewpoint that the standard SU(3)*SU(2)*U(1) model is only a low-energy manifestation ...
The gauge symmetry of the Standard Model is SU(3)c×SU(2)L×U(1)Y for unknown reasons. One aspect that...
The origin of mass must lie in physics beyond the Standard Model. Dynamical electroweak symmetry bre...
In this talk we describe examples of renormalizable strongly interacting field theories where chiral...
If N=2 supersymmetry breaks to N=1 supersymmetry at an intermediate scale $m_2$ and then, later on, ...
3 pags., 1 tab.Since new Z bosons (Z) are predicted by many approaches to particle physics beyond th...
A short-distance heavy quark mass depends on two parameters, the renormalization scale mu controllin...
Motivated by recent experimental indications of large {nu}{sub {mu}} - {nu}{tau} mixing, we explore ...
Abstract Precision measurements of high energy top quarks at the LHC constitute a powerful probe of ...
In the context of the radiative electroweak symmetry breaking scenario we investigate the implicatio...
We have searched for conceptually simple extensions of the standard model, and describe here a candi...
We use effective field theory to show that small increases in the up and down quark masses would mov...