Higgs Bosons Phenomenology in the Higgs Triplet Model

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Impact of qq ′ → H ±± H ∓ Current searches are already sensitive to qq ′ → H ±± H ∓ ! • 2l search: sensitive to H ±± H ∓ irrespective of H ± decay • 3l search: sensitive to H ±± H ∓ if H ± → l ± ν → Define inclusive single H ±± cross-section for 2l search: σ H ±±= σ(pp → H ++ H −− ) + 2σ(pp → H ±± H ∓ ) Increases search potential of Tevatron in ee, eµ, µµ channels Akeroyd,Aoki 05
Inclusive single H ±± production at Tevatron Akeroyd,Aoki 05 σ H ±± = σ(pp → H ++ H −− ) + 2σ(pp → H ++ H − ) σ H±± (fb) 350 300 250 200 150 100 50 H ++ H − − only (a) √s =1.96 TeV m H± =m H±± −20 GeV m H± =m H±± m H± =m H±± +20 GeV 0 100 110 120 130 140 150 160 170 180 190 200 m (GeV) H±±
Page 1 and 2: Higgs Bosons Phenomenology in the H
Page 3 and 4: Neutrino Mass and Mixing Strong evi
Page 5 and 6: Neutrino mass hierarchies Three pos
Page 7 and 8: TeV scale models of neutrino mass g
Page 9 and 10: Higgs boson spectrum The HTM has 7
Page 11 and 12: Decays of H ±± : Decay channels f
Page 13 and 14: Limits on hij Presence of H ±± wo
Page 15 and 16: Production of H ±± at Tevatron Fi
Page 17 and 18: Tevatron search (2003) for pp → H
Page 19 and 20: Tevatron search (2007) for pp → H
Page 21: Single H ±± production via qq ′
Page 25 and 26: Summary for qq ′ → H ±± H ∓
Page 27 and 28: Light H ±± at LHC Simulations by
Page 29 and 30: Explicit expressions for hij All hi
Page 31 and 32: Dependence of BR(H ±± → l ± l
Page 33 and 34: BR(H ±± → l ± i l± j ) agains
Page 35 and 36: BR(H ±± → l ± i l± j ) agains
Page 37 and 38: HTM prediction in the plane [BR(H
Page 39 and 40: HTM prediction in the plane [BR(H
Page 41 and 42: HTM prediction for H ± → l ± ν

Higgs Bosons Phenomenology in the Higgs Triplet Model

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