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2015:groups:higgs:morehiggs:largesplit [2015/06/13 21:14]
jose_miguel.no
2015:groups:higgs:morehiggs:largesplit [2015/06/18 18:09]
jose_miguel.no
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 **Responsible:​** Jose Mi No  ​ **Responsible:​** Jose Mi No  ​
  
-**Members:​** Ken Mimasu, Werner Porod, Jérémy Bernon, Andrey Katz, Dipan Sengupta+**Members:​** Ken Mimasu, Werner Porod, Jérémy Bernon, Andrey Katz, Dipan Sengupta, Sanjoy Biswas
  
  
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 These decays typically dominate the Br of the mother particle when the splitting is large, on one side weakening searches of the mother particle via other Br, on the other providing a new discovery mode for both mother and daughter particles (usually very clean). ​   ​ These decays typically dominate the Br of the mother particle when the splitting is large, on one side weakening searches of the mother particle via other Br, on the other providing a new discovery mode for both mother and daughter particles (usually very clean). ​   ​
  
-**Possible projects/​actions to be done**:+**Project**:
  
-    - Assume light A0 scenario for 2HDM (m_A0 < 100 GeV, e.g. [[http://​arxiv.org/​abs/​1412.3385]]). For TypeII 2HDM, a large splitting m_H0 - m_A0 ~ 200-300 GeV is required. For TypeI 2HDM, sizable m_H0 - m_A0 is not required but perfectly possible. In both cases, g g -> H0 -> Z A0 -> ll bb could probe this scenario for low tan_beta (< 5-10) as a complementary search to bbA0 ([[2015:​groups:​higgs:​morehiggs:​lowmassa]]). ​  ​+  * Assume light A0 scenario for 2HDM (m_A0 < 100 GeV, e.g. [[http://​arxiv.org/​abs/​1412.3385]]). For TypeII 2HDM, a large splitting m_H0 - m_A0 ~ 200-300 GeV is required. For TypeI 2HDM, sizable m_H0 - m_A0 is not required but perfectly possible. In both cases, g g -> H0 -> Z A0 -> ll bb could probe this scenario for low tan_beta (< 5) as a complementary search to bbA0 ([[2015:​groups:​higgs:​morehiggs:​lowmassa]]). 
 +  * Use [[http://​cds.cern.ch/​record/​2014119]] to extract the limits on tan_beta in the (m_A0,m_H0) plane, in the 2HDM alignment limit: 
 +      The plot below shows the excluded regions for Type I (left) and Type II (right): (red -> t_beta = 0.5; blue -> t_beta = 1; orange -> t_beta = 1.5; green -> t_beta = 2) 
 +       
 + ​{{:​2015:​groups:​higgs:​morehiggs:​h0toa0ztriangle.jpeg?​direct&​300|}} {{:​2015:​groups:​higgs:​morehiggs:​h0toa0ztriangle_type2.jpeg?​direct&​300|}}
  
 +Regarding the interplay/​contamination of bbH0 in the gg channel... ​
 +
 +
 +     * LHC14 Prospects and interplay with bbA0
 +
 +     
 +      ​
 **Literature**:​ **Literature**:​
 +
 +
 +**__Light A/H__**:
 +
 +  * [[http://​arxiv.org/​abs/​1412.3385]]:​ A detailed analysis of the 2HDM allowed region for a light A0 (20 GeV < m_A0 < 60 GeV), both in TypeI and TypeII. It also has a discussion of detection prospects in bbA0 and gg->A0 for "​aligment"​ and "​wrong-sign"​ scenarios, showing that in particular for TypeII the "​wrong-sign"​ can be completely explored with bbA0.  ​
 +
 +
 +**__Sizable Splitting in 2HDM and A->​ZH/​H->​ZA__**:​
  
   * [[http://​cds.cern.ch/​record/​2014119]]:​ CMS has recently carried on a search of A0 -> Z H0 / H0 -> Z A0 in ll bb, ll tautau final states. This search constraints values of tan_beta up to 4 for some (m_A0, m_H0) values with a sizable splitting.   * [[http://​cds.cern.ch/​record/​2014119]]:​ CMS has recently carried on a search of A0 -> Z H0 / H0 -> Z A0 in ll bb, ll tautau final states. This search constraints values of tan_beta up to 4 for some (m_A0, m_H0) values with a sizable splitting.
-  * [[http://​arxiv.org/​abs/​1405.5537]]:​ A physical motivation for a large mass splitting m_A0 - m_H0 ~ 200-300 GeV and the search for A0 -> Z H0 at LHC is provided: this large splitting leads to a strong EW phase transition in the early universe, which could be responsible for the generation of the observed matter-antimatter asymmetry via EW baryogenesis. ​We also analyzed ​LHC14 search prospects for A0 -> Z H0 in ll bb and ll W W (W -> l nu).+  * [[http://​arxiv.org/​abs/​1405.5537]]:​ A physical motivation for a large mass splitting m_A0 - m_H0 ~ 200-300 GeV and the search for A0 -> Z H0 at LHC is provided: this large splitting leads to a strong EW phase transition in the early universe, which could be responsible for the generation of the observed matter-antimatter asymmetry via EW baryogenesis. ​It also analyzes ​LHC14 search prospects for A0 -> Z H0 in ll bb and ll W W (W -> l nu).
   * [[http://​arxiv.org/​abs/​1404.1922]]:​ Detailed discussion of LHC14 search prospects for A0 -> Z H0 in both ll bb and ll Z Z, and H0 -> Z A0 in ll bb.   * [[http://​arxiv.org/​abs/​1404.1922]]:​ Detailed discussion of LHC14 search prospects for A0 -> Z H0 in both ll bb and ll Z Z, and H0 -> Z A0 in ll bb.
 +
 +
 +**__Constraints on 2HDM (e.g. Flavour)__**:​
 +  * [[http://​arxiv.org/​abs/​1208.2788]] Bounds on m_H+ from b -> s gamma, both for Type I and Type II. They show that for Type II, the bound is particularly strong (m_H+ > 380 GeV) and tan_beta independent.
    
2015/groups/higgs/morehiggs/largesplit.txt · Last modified: 2015/06/18 18:09 by jose_miguel.no