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2019:groups:higgs:lightscalars:exotichdecays [2019/06/24 16:04]
suzanne.gascon
2019:groups:higgs:lightscalars:exotichdecays [2019/06/26 09:20] (current)
antoine.lesauvage
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 We consider two decay modes of $\phi$: $\phi \to \gamma \gamma$, $\phi \to \mu \mu$  We consider two decay modes of $\phi$: $\phi \to \gamma \gamma$, $\phi \to \mu \mu$ 
  
-  * $\phi$ -> $\gamma\gamma$. (**SG**)+  * $\phi$ -> $\gamma\gamma$. (**SG,AL**)
  
 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]]).  ​ 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]]).  ​
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 __TO DO LIST__ ​ __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 Bauer, Thamm, 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 $h$)   - Validate UFO File {{ :​2019:​groups:​higgs:​alp-pr.tar.gz |ALP UFO file }} (fixed by Peter Richardson) from Bauer, Thamm, 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]** +  - SM background generation. ​**Done** ​**[SG,AL]** 
-  - Generate signal: study kinematics of different $h$ production modes, as well as $m_{\phi}$ dependence.**[SG]**+  - 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. ​   - Contur study (related to next item). Give **JB** range of parameters to scan for the model. ​
-  - Other constraints. 1) LEP Z width: Z → $h^*$ $\phi$, $h^*\to bb...$ leads to constraints from Z total width. **[JN, SW]** 2) LEP Exclusive Z decays? ​3)...+  - Other constraints. 1) Higgs signal strengths bound on partial BSM width **[JN, SW]** 2) LEP Z width: Z → $h^*$ $\phi$, $h^*\to bb...$ leads to constraints from Z total width. **[JN, SW]** 3) LEP Exclusive Z decays? ​4)...
    
-  * $\phi$ -> $\mu\mu$+  * $\phi$ -> $\mu\mu$ ​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]];​ $h\to ZZ_d\to 4l$[[http://​arxiv.org/​abs/​1802.03388|1802.03388]])
  
 Similar strategy to the one above! ​ In principle above 10 GeV we are safe from SM low mass resonances. Below 10 GeV? Also, how low can one go in mass by playing with muon isolation. Similar strategy to the one above! ​ In principle above 10 GeV we are safe from SM low mass resonances. Below 10 GeV? Also, how low can one go in mass by playing with muon isolation.
2019/groups/higgs/lightscalars/exotichdecays.1561385085.txt.gz · Last modified: 2019/06/24 16:04 by suzanne.gascon