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The other Higgses, at resonance, in the Lee-Wick extension of the Standard Model
Within the framework of the Lee Wick Standard Model (LWSM) we investigate Higgs pair production $gg \to h_0 h_0$, $gg \to h_0 \tilde p_0$ and top pair production $gg \to \bar tt$ at the Large Hadron Collider (LHC), where the neutral particles from the Higgs sector ($h_0$, $\tilde h_0$ and $\tilde p_...
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
2011
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Acceso en línea: | https://dx.doi.org/10.1007/JHEP10(2011)145 http://cds.cern.ch/record/1376319 |
_version_ | 1780922964696367104 |
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author | Figy, Terrance Zwicky, Roman |
author_facet | Figy, Terrance Zwicky, Roman |
author_sort | Figy, Terrance |
collection | CERN |
description | Within the framework of the Lee Wick Standard Model (LWSM) we investigate Higgs pair production $gg \to h_0 h_0$, $gg \to h_0 \tilde p_0$ and top pair production $gg \to \bar tt$ at the Large Hadron Collider (LHC), where the neutral particles from the Higgs sector ($h_0$, $\tilde h_0$ and $\tilde p_0$) appear as possible resonant intermediate states. We investigate the signal $gg \to h_0 h_0 \to \bar b b \gamma \gamma$ and we find that the LW Higgs, depending on its mass-range, can be seen not long after the LHC upgrade in 2012. More precisely this happens when the new LW Higgs states are below the top pair threshold. In $gg \to \bar tt$ the LW states, due to the wrong-sign propagator and negative width, lead to a dip-peak structure instead of the usual peak-dip structure which gives a characteristic signal especially for low-lying LW Higgs states. We comment on the LWSM and the forward-backward asymmetry in view of the measurement at the TeVatron. Furthermore, we present a technique which reduces the hyperbolic diagonalization to standard diagonalization methods. We clarify issues of spurious phases in the Yukawa sector. |
id | cern-1376319 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2011 |
record_format | invenio |
spelling | cern-13763192023-03-14T19:47:07Zdoi:10.1007/JHEP10(2011)145http://cds.cern.ch/record/1376319engFigy, TerranceZwicky, RomanThe other Higgses, at resonance, in the Lee-Wick extension of the Standard ModelParticle Physics - PhenomenologyWithin the framework of the Lee Wick Standard Model (LWSM) we investigate Higgs pair production $gg \to h_0 h_0$, $gg \to h_0 \tilde p_0$ and top pair production $gg \to \bar tt$ at the Large Hadron Collider (LHC), where the neutral particles from the Higgs sector ($h_0$, $\tilde h_0$ and $\tilde p_0$) appear as possible resonant intermediate states. We investigate the signal $gg \to h_0 h_0 \to \bar b b \gamma \gamma$ and we find that the LW Higgs, depending on its mass-range, can be seen not long after the LHC upgrade in 2012. More precisely this happens when the new LW Higgs states are below the top pair threshold. In $gg \to \bar tt$ the LW states, due to the wrong-sign propagator and negative width, lead to a dip-peak structure instead of the usual peak-dip structure which gives a characteristic signal especially for low-lying LW Higgs states. We comment on the LWSM and the forward-backward asymmetry in view of the measurement at the TeVatron. Furthermore, we present a technique which reduces the hyperbolic diagonalization to standard diagonalization methods. We clarify issues of spurious phases in the Yukawa sector.Within the framework of the Lee Wick Standard Model (LWSM) we investigate Higgs pair production $gg \to h_0 h_0$, $gg \to h_0 \tilde p_0$ and top pair production $gg \to \bar tt$ at the Large Hadron Collider (LHC), where the neutral particles from the Higgs sector ($h_0$, $\tilde h_0$ and $\tilde p_0$) appear as possible resonant intermediate states. We investigate the signal $gg \to h_0 h_0 \to \bar b b \gamma \gamma$ and we find that the LW Higgs, depending on its mass-range, can be seen not long after the LHC upgrade in 2012. More precisely this happens when the new LW Higgs states are below the top pair threshold. In $gg \to \bar tt$ the LW states, due to the wrong-sign propagator and negative width, lead to a dip-peak structure instead of the usual peak-dip structure which gives a characteristic signal especially for low-lying LW Higgs states. We comment on the LWSM and the forward-backward asymmetry in view of the measurement at the TeVatron. Furthermore, we present a technique which reduces the hyperbolic diagonalization to standard diagonalization methods. We clarify issues of spurious phases in the Yukawa sector.arXiv:1108.3765CERN-PH-TH-2011-184CP-3-2011-25CERN-PH-TH-2011-184CP-3-2011-25oai:cds.cern.ch:13763192011-08-19 |
spellingShingle | Particle Physics - Phenomenology Figy, Terrance Zwicky, Roman The other Higgses, at resonance, in the Lee-Wick extension of the Standard Model |
title | The other Higgses, at resonance, in the Lee-Wick extension of the Standard Model |
title_full | The other Higgses, at resonance, in the Lee-Wick extension of the Standard Model |
title_fullStr | The other Higgses, at resonance, in the Lee-Wick extension of the Standard Model |
title_full_unstemmed | The other Higgses, at resonance, in the Lee-Wick extension of the Standard Model |
title_short | The other Higgses, at resonance, in the Lee-Wick extension of the Standard Model |
title_sort | other higgses, at resonance, in the lee-wick extension of the standard model |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1007/JHEP10(2011)145 http://cds.cern.ch/record/1376319 |
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