This preview shows page 1. Sign up to view the full content.
Unformatted text preview: 253a/Schwartz Due November 23, 2010 Problem Set 11 The Higgs is a (hypothetical) real scalar particle which couples to the standard model as L higgs =- 1 2 ( square + m h 2 ) + i i i + i ( i- m i + g z Z ) i + 1 2 Z ( square + m Z 2 ) Z + Z Z 2 + (1) i is called a Yukawa Coupling and is different for each fermion species i . In the standard model, i = m i v , where v is the Higgs vacuum-expectation-value, related to the masses of the electroweak gauge bosons: v = 2 m W g w e a k = 246 GeV. Z is the Z-boson with m Z = 91 GeV, Z = m Z 2 v , and g z 0.1. 1. Direct Higgs searches. Before the LHC, CERN ran an e + e- collider called LEP, running first (LEP 1) at s = 92 GeV then (LEP 2) at s 200 GeV, with 1 fb- 1 = 10- 39 cm- 2 integrated luminosity for each run. a) What is the partial width (decay rate) for the Higgs to decay to fermion i ?...
View Full Document