Epstein Secrets

lid varies with 41. We find that 14„r also changes at a level comparable to its sensitivity to Mg or Ali as the gauge pa- rameter deviates from the Landau gauge (egc = 0). It is there- fore important to consider this ambiguity for model building purposes. Nevertheless, the absolute change in lid is far

erved values, MH 125 GeV and Mt :4 173 GeV, the coupling runs neg- ative at h 107° — 1012 GeV; this is the well-known vacuum stability problem of the Standard Model [26]. Successful HI requires an O(2e) deviation from central values toward either larger Higgs boson mass or smaller top quark mass. Gauge depende

ia varies with $4e. We find that V;,,( also changes at a level comparable to its sensitivity to Ahr or Me as the gauge pa- rameter deviates from the Landau gauge (‘ = 0). It is there- fore important to consider this ambiguity for model building purposes. Nevertheless, the absolute change in Vim is far t

bserved values, 125 GeV and Mt xr. 173 GeV, the coupling runs neg- ative at h ot 101° —1012 GeV; this is the well-known vacuum stability problem of the Standard Model [26). Successful HI requires an O(2o) deviation from central values toward either larger Higgs boson mass or smaller top quark mass. Gauge depende

losely surround the negative charge, and so at a distance the physical effects of the initial negative charge are reduced. This meant, according to Landau, that the closer you get to an elec- tron, the larger its actual charge will appear. If we measure the electron charge to be some specific value at

ne wanted to talk about the details in public. 2P_GrealetaleryEverTold_AC.indd 254 12/16116 3:06 PIA EFTA00286176 Spanking the Vacuum 255 That the Standard Model didn't fix in advance many of the details of the Higgs sector didn't dissuade many theorists from proposing models that "predicted" the Higgs mass