TY - JOUR
T1 - Modified top quark condensation model with the extra heavy fermion, the 125 GeV pseudo-Goldstone boson, and the additional heavy scalar bosons
AU - Khaidukov, Z. V.
AU - Zubkov, M. A.
N1 - Publisher Copyright:
© 2017 World Scientific Publishing Company.
PY - 2017/8/30
Y1 - 2017/8/30
N2 - We discuss the modified top quark condensation model proposed in Ref. 54. This construction was inspired by the top-seesaw scenario, in which the extra heavy fermion χ that may be paired with the top quark is added. Besides, this model incorporates the ideas of the little Higgs scenario, in which the 125 GeV scalar particle appears as a pseudo-Goldstone boson. This model admits (in addition to the 125 GeV scalar boson H) the heavier scalar excitation H′. We consider the region of parameters, where its mass is MH′ ∼ 1 TeV, the width of H′ is τH′ ∼ 0.3MH′, while the mass of the heavy fermion is mχ ∼ 1 TeV. We find that in this model the value of the cross-section σpp→H′+X→γ+γ+γ+X for √s = 13 TeV is essentially smaller than the present experimental upper bound. Besides, we find that for the chosen values of parameters there should exist the CP-even scalar boson with mass ≈ 2mχ and very small width. In addition, the model predicts the existence of the extra neutral CP-even scalar boson and the charged scalar boson with masses of the order of 1 TeV.
AB - We discuss the modified top quark condensation model proposed in Ref. 54. This construction was inspired by the top-seesaw scenario, in which the extra heavy fermion χ that may be paired with the top quark is added. Besides, this model incorporates the ideas of the little Higgs scenario, in which the 125 GeV scalar particle appears as a pseudo-Goldstone boson. This model admits (in addition to the 125 GeV scalar boson H) the heavier scalar excitation H′. We consider the region of parameters, where its mass is MH′ ∼ 1 TeV, the width of H′ is τH′ ∼ 0.3MH′, while the mass of the heavy fermion is mχ ∼ 1 TeV. We find that in this model the value of the cross-section σpp→H′+X→γ+γ+γ+X for √s = 13 TeV is essentially smaller than the present experimental upper bound. Besides, we find that for the chosen values of parameters there should exist the CP-even scalar boson with mass ≈ 2mχ and very small width. In addition, the model predicts the existence of the extra neutral CP-even scalar boson and the charged scalar boson with masses of the order of 1 TeV.
KW - Composite Higgs bosons
KW - LHC
KW - proton-proton collisions
KW - top-seesaw
UR - http://www.scopus.com/inward/record.url?scp=85028354409&partnerID=8YFLogxK
U2 - 10.1142/S0217751X1750141X
DO - 10.1142/S0217751X1750141X
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AN - SCOPUS:85028354409
SN - 0217-751X
VL - 32
JO - International Journal of Modern Physics A
JF - International Journal of Modern Physics A
IS - 23-24
M1 - 1750141
ER -