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2019:groups:higgs:lightscalars:exotichdecays [2019/06/24 10:45]
jose.miguel.no
2019:groups:higgs:lightscalars:exotichdecays [2019/06/24 17:14]
jose.miguel.no
Line 6: Line 6:
 Please add your initials to sub-projects! Please add your initials to sub-projects!
  
-**Exotic Higgs decays into h -> Z $\phi$**+**Exotic Higgs decays into h -> Z $\phi$** ​(see also discussion in [[2019:​groups:​higgs:​seminvisible|]]). ​
  
 Reference to look for general motivation on exotic Higgs decays, possible models, etc, as well as for information on theoretical work and experimental analylis (as of 2013!): Review/​compendium work on exotic Higgs decays from Curtin, Gori, Shelton, Strassler et al [[https://​arxiv.org/​abs/​1312.4992|1312.4992]]. ​ Reference to look for general motivation on exotic Higgs decays, possible models, etc, as well as for information on theoretical work and experimental analylis (as of 2013!): Review/​compendium work on exotic Higgs decays from Curtin, Gori, Shelton, Strassler et al [[https://​arxiv.org/​abs/​1312.4992|1312.4992]]. ​
  
 +We consider two decay modes of $\phi$: $\phi \to \gamma \gamma$, $\phi \to \mu \mu$ 
  
-$\phi$ -> $\gamma\gamma$. ​Preliminary study from Bauer, Neubert, Thamm [[https://​arxiv.org/​abs/​1708.00443|1708.00443]] ​(see also [[https://​arxiv.org/​pdf/​1704.08207.pdf|1704.08207]]). ​ They put limits on very light ALPs (m_a < 47 MeV) from constraints on h -> Z $\gamma$since for m_a < 47 MeV the two photons from the ALP decay are very collimated and seen as one in the detector. For not-so-light ALPs, they compute just number of signal events for gg -> h -> Z $\phi$, and assume limits for 100 events at LHC (some more discussion in [[2019:​groups:​higgs:​seminvisible|]])+  * $\phi$ -> $\gamma\gamma$. (**SG,AL**)
  
-For $m_\phi > 35$ GeV:+Preliminary study from Bauer, Neubert, Thamm [[https://​arxiv.org/​abs/​1708.00443|1708.00443]] (see also [[https://​arxiv.org/​pdf/​1704.08207.pdf|1704.08207]]).  ​
  
-$h \to Z^* \phi$, $Z^* \to \mu\mu[names: **SG, AL, JN, GM**]+For m_{\phi} < 47 MeV, constraints from $h \to Z \gamma$, since for m_{\phi} < 47 MeV the two photons from the $\phidecay are very collimated and seen as one in the detector.
  
-$h^* \to Z \phi$ [UFO files from effective ggh coupling for kinematics ​and rescale rate with ggF cross section?]+For m_{\phi} > 47 MeV, they compute just number of signal events for $gg \to h \to Z \phi$and assume limits for 100 events at LHC. 
  
-For 47MeV < $m_\phi < 35$ GeV:+$m_\phi < 35$ GeV: $h \to Z \phi$ (on-shell $Z \to \ell\ell$)
  
-$h \to Z \phi$, $Z \to \mu\mu$, $\phi \to \gamma\gamma$ [names**SGALJNGMKT**]+$m_\phi > 35$ GeV: $h \to Z^* \phi$ ($h \to \ell\ell \phi$) 
 + 
 +__TO DO LIST__  
 + 
 +  - ASK FOR FEYNRULES FILE!  
 +  - Validate UFO File {{ :​2019:​groups:​higgs:​alp-pr.tar.gz |ALP UFO file }} (fixed by Peter Richardson) from BauerThamm, Neubert. **[JN, SW]** //NOTE: We need to check for effective ggh coupling in UFO.// (CHECKED: They Have it, so we can generate gluon fusion production of $h$) 
 +  - SM background generation. **[SG,​AL]** 
 +  - Generate signal: study kinematics of different $h$ production modes, as well as $m_{\phi}$ dependence.**[SG,​AL]** 
 +  - Contur study (related to next item). Give **JB** range of parameters to scan for the model.  
 +  - Other constraints. 1) Higgs signal strengths bound on partial BSM width **[JN, SW]** 2) LEP width: Z → $h^*$ $\phi$, $h^*\to bb...$ leads to constraints from Z total width. **[JN, SW]** 3) LEP Exclusive Z decays? 4)... 
 +  
 +  * $\phi$ -> $\mu\mu$ ​Possiblly useful refs ($h\to ZZ^*\to4\mu$[[https://​cds.cern.ch/​record/​2621479/​files/​ATLAS-CONF-2018-018.pdf| ATLAS-CONF-2018-018]],[[https://​cds.cern.ch/​record/​2668684/​files/​HIG-19-001-pas.pdf|CMS]]; ​$h\to aa\to4\mu$[[https://​arxiv.org/​abs/​1812.00380|1812.00380]];​ $h\to aa\to2\tau2\mu$ [[https://​inspirehep.net/​record/​1419565/​files/​HIG-15-011-pas.pdf|HIG-15-011-pas]][[https://​arxiv.org/​pdf/​1505.01609.pdf|1505.01609]]) 
 + 
 +Similar strategy to the one above! ​ In principle above 10 GeV we are safe from SM low mass resonances. Below 10 GeV? Alsohow low can one go in mass by playing with muon isolation. 
 + 
 +$h \to Z \phi$$Z \to \mu\mu$$\phi \to \mu\mu$ recasted from existing analysis of $h \to \phi \phi$, $\phi \to \mu\mu$.
  
-$h \to Z \phi$, $Z \to \mu\mu$, $\phi \to \mu\mu$ recasted from existing analysis of $h \to \phi \phi$, $\phi \to \mu\mu$ [names: **KT**] ​ 
2019/groups/higgs/lightscalars/exotichdecays.txt · Last modified: 2019/06/26 09:20 by antoine.lesauvage