Higgs Bosons Phenomenology in the Higgs Triplet Model

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Inclusive s<strong>in</strong>gle H ±± production at LHC Akeroyd,Aoki 05 σ H±± (fb) 100 10 1 0.1 0.01 H ++ H − − only (a) m = m −80GeV H± H±± m = m H± H±± m = m +80GeV H± H±± √s =14 TeV 200 300 400 500 600 700 800 900 1000 m H±± (GeV)
Summary for qq ′ → H ±± H ∓ • Cross-section can be as large as qq → H ++ H −− • Can enhance H ±± discovery potential <strong>in</strong> 2l,3l channels • (Best?) Production process for H ± of HTM at hadron colliders • Not yet simulated (but see Han et al arXiv:0803.3450)
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 and 22: Single H ±± production via qq ′
Page 23: Inclusive single H ±± production
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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