Five-lepton and six-lepton signatures from production of neutral triplet scalars in the Higgs Triplet Model
Five-lepton and six-lepton signatures from production of neutral triplet scalars in the Higgs Triplet Model
The neutral triplet scalars (H^0, A^0) in the Higgs Triplet Model (HTM) are difficult to detect at the LHC for the case of mass degeneracy with the singly charged (H^+) and doubly charged (H^++) scalars. A non-zero value of a specific quartic coupling in the scalar potential removes this degeneracy, and positive values of this coupling would give rise to the mass hierarchy m_{A^0,H^0} > m_{H^+} > m_{H^++}. In this scenario the decays H^0-> H^+ W^* and A^0-> H^+ W^*, followed by H^+ -> H^{++} W^*, can proceed with large branching ratios, even for small mass splittings among the triplet scalars. Such a cascade process would lead to production of H^{++}H^{--} accompanied by several virtual W bosons, and would provide a way of observing H^0 and A^0 with a signature which is different from that of the conventional production process for doubly charged scalars, q qbar -> \gamma^*, Z^* -> H^{++}H^{--}. Assuming the decay H^{++} to l^+ l^+, we quantify the magnitude of the five-lepton and six-lepton signals in these channels, which have essentially negligible backgrounds at the LHC.
055026-[13 pages]
Akeroyd, A.G.
e5de827d-7119-41c2-9f1e-5ef123afdf98
Moretti, S.
b57cf0f0-4bc3-4e02-96e3-071255366614
Sugiyama, Hiroaki
1b7a22f2-c44a-4de4-94c2-d84ab41dd678
24 January 2012
Akeroyd, A.G.
e5de827d-7119-41c2-9f1e-5ef123afdf98
Moretti, S.
b57cf0f0-4bc3-4e02-96e3-071255366614
Sugiyama, Hiroaki
1b7a22f2-c44a-4de4-94c2-d84ab41dd678
Akeroyd, A.G., Moretti, S. and Sugiyama, Hiroaki
(2012)
Five-lepton and six-lepton signatures from production of neutral triplet scalars in the Higgs Triplet Model.
Physical Review D, D85 (5), .
(doi:10.1103/PhysRevD.85.055026).
Abstract
The neutral triplet scalars (H^0, A^0) in the Higgs Triplet Model (HTM) are difficult to detect at the LHC for the case of mass degeneracy with the singly charged (H^+) and doubly charged (H^++) scalars. A non-zero value of a specific quartic coupling in the scalar potential removes this degeneracy, and positive values of this coupling would give rise to the mass hierarchy m_{A^0,H^0} > m_{H^+} > m_{H^++}. In this scenario the decays H^0-> H^+ W^* and A^0-> H^+ W^*, followed by H^+ -> H^{++} W^*, can proceed with large branching ratios, even for small mass splittings among the triplet scalars. Such a cascade process would lead to production of H^{++}H^{--} accompanied by several virtual W bosons, and would provide a way of observing H^0 and A^0 with a signature which is different from that of the conventional production process for doubly charged scalars, q qbar -> \gamma^*, Z^* -> H^{++}H^{--}. Assuming the decay H^{++} to l^+ l^+, we quantify the magnitude of the five-lepton and six-lepton signals in these channels, which have essentially negligible backgrounds at the LHC.
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Published date: 24 January 2012
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19 pages, 13 figures
Organisations:
Physics & Astronomy
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Local EPrints ID: 356693
URI: http://eprints.soton.ac.uk/id/eprint/356693
ISSN: 1550-7998
PURE UUID: bd215f8b-7f43-4f29-8abe-92c76027f4ac
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Date deposited: 17 Sep 2013 15:01
Last modified: 15 Mar 2024 03:37
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Author:
Hiroaki Sugiyama
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