Weak interactions.

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Presentation transcript:

weak interactions

weak decays beta decay of neutron

e n neutrino p direct interaction of four fermions Enrico Fermi, ~1936

Enrico Fermil

1964 ===> gauge theory electroweak

1957 weak bosons W J. Schwinger

( Glashow, Salam, Weinberg ) - 1964 - 1968 gauge theory of the electroweak interactions ( Glashow, Salam, Weinberg )

Glashow Salam Weinberg 1964-1968

weak and electromagnetic interactions partial unification

gauge group SU(2)xU(1)

S U (2) x U (1) weak interaction electromagnetic interaction

SU(2) x U(1) 3 + 1 gauge bosons photon Z W(+) W(-)

SU(2)xU(1) weak interactions electromagnetism neutral current

SU(2)xU(1) neutral current CERN 1972

photon: superposition of SU(2) and U(1) – gauge boson Why photon massless? Why W – boson massive?

by spontaneous symmetry breaking mass generation by spontaneous symmetry breaking ( “ Higgs “ – mechanism)

Minimal electroweak theory Gauge group: SU(2) x U(1)

SU(2) U(1) fermions

symmetry breaking: SU(2) and U(1) are broken, but the electric charge is unbroken

neutral current interaction parity violation

neutral current interaction parity violation observed in atomic physics

weak interactions

weak decays beta decay of neutron

e n neutrino p direct interaction of four fermions Enrico Fermi, ~1936

Minimal electroweak theory Gauge group: SU(2) x U(1)

symmetry breaking: SU(2) and U(1) are broken, but the electric charge is unbroken

M(W) = 80.4 GeV M(Z)= 91.2 GeV CERN, 1984 =>

The masses of the weak bosons are predicted, once the weak angle is measured. The electron mass cannot be predicted ( the coupling constant g is unknown ).

electroweak theory: QCD: mass generation by SSB mass generation problem: mass generation electroweak theory: mass generation by SSB QCD: mass generation by confinement

hypothetical Higgs boson

limit on mass of Higgs boson from LEP: 114 GeV

L3 I ATLAS CMS LHCb Alice LEP - LHC

muon H===> Z Z LHC Higgs particle

W W M(W)~100 MeV - other possibility to generate the masses for the weak bosons: W =>pion=>W pion W W M(W)~100 MeV

W =>technipion=>W - technicolor W =>technipion=>W technipion W W M(W)~100 GeV

composite weak bosons, leptons and quarks other possibility: composite weak bosons, leptons and quarks