Epstein Secrets

arth and Space Exploration Arizona State University. Tempe. AZ 85827-1404 2Research School of Astronomy and Astrophysics, Mt. Stromlo Observatory. Australian National University, Canberra, Australia 2611 (Dated: March 19, 2014) We consider the status of Higgs Inflation in light of the recently announced detection of B-modes

t be high. lint x 2 x 1016 GeV. Higgs Inflation generally predicts a small amplitude of tensor perturbations. and therefore it is natural to ask if Higgs Inflation might accommodate this new measurement. We find the answer is essentially no, unless one considers either extreme fine tuning. or possibly

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 dependence enters the calculation at two places: ex- plicitly in the one-loop correction to the effectiv

Earth and Space Esplomtion Arizona State University. Tempe. AZ 85827-1404 2Reseatrh School of Astronomy and Astrophysics, Mt. Stromlo Observatory, Australian National University. Canberra, Australia 2611 (Dated: March 19, 2014) We consider the status of Higgs Inflation in light of the recently announced detection of B-modes

t be high, Via Az 2 x 101° GeV. Higgs Inflation generally predicts a small amplitude of tensor perturbations. and therefore it is natural to ask if Higgs Inflation might accommodate this new measurement. We find the answer is essentially no. unless one considers either extreme fine tuning. or possibly

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 dependence enters the calculation at two places: ex- plicitly in the one-loop correction to the effectiv

it- ing forty years for, rumors began to fly in the community. Many of these came from the experimenters themselves. I have a part-time position at Australian National University in Canberra, and the International Con- ference on High Energy Physics was going to be in held in Melbourne in July of 2012. Melbourne has a big LHC

s would leave only the photon left over as a massless gauge boson. But there's more. By virtue of the gauge symmetry he introduced, Weinberg's new Higgs particle would also interact with electrons, and when the condensate formed, the effect would be to give electrons a mass as well as the W and Z pa

a revolutionary. But reluctant revolutionary he was, although, due to some shortsighted journal editors, he almost didn't get the chance. In 1960 Higgs had just taken up his post and had been asked to serve on the committee that coordinated the first Scottish Universities Summer School in Physics.