Dark Matter signals at the LHC from a 3HDM
Dark Matter signals at the LHC from a 3HDM
 
  We analyse new signals of Dark Matter (DM) at the Large Hadron Collider (LHC) in a 3-Higgs Doublet Model (3HDM) where only one doublet acquires a Vacuum Expectation Value (VEV), preserving a parity Z2. The other two doublets are inert and do not develop a VEV, leading to a dark scalar sector controlled by Z2, with the lightest CP-even dark scalar H1 being the DM candidate. This leads to the loop induced decay of the next-to-lightest scalar, H2→ H1ff¯ (f= u, d, c, s, b, e, μ, τ) , mediated by both dark CP-odd and charged scalars. This is a smoking-gun signal of the 3HDM since it is not allowed in the 2HDM with one inert doublet and is expected to be important when H2 and H1 are close in mass. In practice, this signature can be observed in the cascade decay of the SM-like Higgs boson, h→ H1H2→ H1H1ff¯ into two DM particles and di-leptons/di-jets, where h is produced from either gluon-gluon Fusion (ggF) or Vector Boson Fusion (VBF). However, this signal competes with the tree-level channel qq¯ → H1H1Z∗→ H1H1ff¯. We devise some benchmarks, compliant with collider, DM and cosmological data, for which the interplay between these modes is discussed. In particular, we show that the resulting detector signature, [InlineMediaObject not available: see fulltext.], with invariant mass of ff¯ much smaller than mZ, can potentially be extracted already during Run 2 and 3. For example, the H2 → H1γ* and γ* → e+e− case will give a spectacular QED mono-shower signal.
Beyond Standard Model, Dark matter, Hadron-Hadron scattering (experiments), Higgs physics
  
  
  
    
      Cordero, A.
      
        18e7d36c-f706-46d9-869a-42e8faa4c823
      
     
  
    
      Hernandez-Sanchez, J.
      
        1559f21d-dc8f-4616-93b3-44ed3ecd32ff
      
     
  
    
      Keus, V.
      
        f56212de-96d7-4955-8c56-561910f7f167
      
     
  
    
      King, S.F.
      
        f8c616b7-0336-4046-a943-700af83a1538
      
     
  
    
      Moretti, S.
      
        b57cf0f0-4bc3-4e02-96e3-071255366614
      
     
  
    
      Rojas, D.
      
        55118d87-8b05-48de-bcfc-a3d7bb7c13b4
      
     
  
    
      Sokolowska, D.
      
        22a8f2fc-000d-4a70-a0c8-bb0982631654
      
     
  
  
   
  
  
    
    
  
    
    
  
    
      May 2018
    
    
  
  
    
      Cordero, A.
      
        18e7d36c-f706-46d9-869a-42e8faa4c823
      
     
  
    
      Hernandez-Sanchez, J.
      
        1559f21d-dc8f-4616-93b3-44ed3ecd32ff
      
     
  
    
      Keus, V.
      
        f56212de-96d7-4955-8c56-561910f7f167
      
     
  
    
      King, S.F.
      
        f8c616b7-0336-4046-a943-700af83a1538
      
     
  
    
      Moretti, S.
      
        b57cf0f0-4bc3-4e02-96e3-071255366614
      
     
  
    
      Rojas, D.
      
        55118d87-8b05-48de-bcfc-a3d7bb7c13b4
      
     
  
    
      Sokolowska, D.
      
        22a8f2fc-000d-4a70-a0c8-bb0982631654
      
     
  
       
    
 
  
    
      
  
  
  
  
  
  
    Cordero, A., Hernandez-Sanchez, J., Keus, V., King, S.F., Moretti, S., Rojas, D. and Sokolowska, D.
  
  
  
  
   
    (2018)
  
  
    
    Dark Matter signals at the LHC from a 3HDM.
  
  
  
  
    Journal of High Energy Physics, 2018 (5), [30].
  
   (doi:10.1007/JHEP05(2018)030). 
  
  
   
  
  
  
  
  
   
  
    
    
      
        
          Abstract
          We analyse new signals of Dark Matter (DM) at the Large Hadron Collider (LHC) in a 3-Higgs Doublet Model (3HDM) where only one doublet acquires a Vacuum Expectation Value (VEV), preserving a parity Z2. The other two doublets are inert and do not develop a VEV, leading to a dark scalar sector controlled by Z2, with the lightest CP-even dark scalar H1 being the DM candidate. This leads to the loop induced decay of the next-to-lightest scalar, H2→ H1ff¯ (f= u, d, c, s, b, e, μ, τ) , mediated by both dark CP-odd and charged scalars. This is a smoking-gun signal of the 3HDM since it is not allowed in the 2HDM with one inert doublet and is expected to be important when H2 and H1 are close in mass. In practice, this signature can be observed in the cascade decay of the SM-like Higgs boson, h→ H1H2→ H1H1ff¯ into two DM particles and di-leptons/di-jets, where h is produced from either gluon-gluon Fusion (ggF) or Vector Boson Fusion (VBF). However, this signal competes with the tree-level channel qq¯ → H1H1Z∗→ H1H1ff¯. We devise some benchmarks, compliant with collider, DM and cosmological data, for which the interplay between these modes is discussed. In particular, we show that the resulting detector signature, [InlineMediaObject not available: see fulltext.], with invariant mass of ff¯ much smaller than mZ, can potentially be extracted already during Run 2 and 3. For example, the H2 → H1γ* and γ* → e+e− case will give a spectacular QED mono-shower signal.
         
      
      
        
          
            
  
    Text
 JHEP05(2018)030
     - Version of Record
   
  
  
    
  
 
          
            
          
            
           
            
           
        
        
       
    
   
  
  
  More information
  
    
      Accepted/In Press date: 18 April 2018
 
    
      e-pub ahead of print date: 4 May 2018
 
    
      Published date: May 2018
 
    
  
  
    
  
    
  
    
  
    
  
    
  
    
     
        Keywords:
        Beyond Standard Model, Dark matter, Hadron-Hadron scattering (experiments), Higgs physics
      
    
  
    
  
    
  
  
  
    
  
  
        Identifiers
        Local EPrints ID: 421257
        URI: http://eprints.soton.ac.uk/id/eprint/421257
        
          
        
        
        
          ISSN: 1126-6708
        
        
          PURE UUID: cbf83593-a14f-4e08-92d6-6ffd0c8e7d23
        
  
    
        
          
        
    
        
          
        
    
        
          
        
    
        
          
            
          
        
    
        
          
            
              
            
          
        
    
        
          
        
    
        
          
        
    
  
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  Date deposited: 29 May 2018 16:30
  Last modified: 18 Mar 2024 02:57
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      Contributors
      
          
          Author:
          
            
            
              A. Cordero
            
          
        
      
          
          Author:
          
            
            
              J. Hernandez-Sanchez
            
          
        
      
          
          Author:
          
            
            
              V. Keus
            
          
        
      
        
      
        
      
          
          Author:
          
            
            
              D. Rojas
            
          
        
      
          
          Author:
          
            
            
              D. Sokolowska
            
          
        
      
      
      
    
  
   
  
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