Family symmetries in F-theory GUTs
Family symmetries in F-theory GUTs
 
  We discuss F-theory SU(5) GUTs in which some or all of the quark and lepton families are assigned to different curves and family symmetry enforces a leading order rank one structure of the Yukawa matrices. We consider two possibilities for the suppression of baryon and lepton number violation. The first is based on Flipped SU(5) with gauge group SU(5)×U(1)?×SU(4) in which U(1)? plays the role of a generalised matter parity. We present an example which, after imposing a Z2 monodromy, has a family symmetry. Even in the absence of flux, spontaneous breaking of the family symmetry leads to viable quark, charged lepton and neutrino masses and mixing. The second possibility has an R-parity associated with the symmetry of the underlying compactification manifold and the flux. We construct an example of a model with viable masses and mixing angles based on the gauge group SU(5)×SU(5) with a family symmetry after imposing a Z2 monodromy.
  
  
  119-135
  
    
      King, S.F.
      
        f8c616b7-0336-4046-a943-700af83a1538
      
     
  
    
      Leontaris, G.K.
      
        fa51f3b0-efd1-4243-b5b0-1f10bb05fa72
      
     
  
    
      Ross, G.G.
      
        d58064ce-8a29-4bfc-b438-ef29b0a16bcb
      
     
  
  
   
  
  
    
      2010
    
    
  
  
    
      King, S.F.
      
        f8c616b7-0336-4046-a943-700af83a1538
      
     
  
    
      Leontaris, G.K.
      
        fa51f3b0-efd1-4243-b5b0-1f10bb05fa72
      
     
  
    
      Ross, G.G.
      
        d58064ce-8a29-4bfc-b438-ef29b0a16bcb
      
     
  
       
    
 
  
  
    
      
        
          Abstract
          We discuss F-theory SU(5) GUTs in which some or all of the quark and lepton families are assigned to different curves and family symmetry enforces a leading order rank one structure of the Yukawa matrices. We consider two possibilities for the suppression of baryon and lepton number violation. The first is based on Flipped SU(5) with gauge group SU(5)×U(1)?×SU(4) in which U(1)? plays the role of a generalised matter parity. We present an example which, after imposing a Z2 monodromy, has a family symmetry. Even in the absence of flux, spontaneous breaking of the family symmetry leads to viable quark, charged lepton and neutrino masses and mixing. The second possibility has an R-parity associated with the symmetry of the underlying compactification manifold and the flux. We construct an example of a model with viable masses and mixing angles based on the gauge group SU(5)×SU(5) with a family symmetry after imposing a Z2 monodromy.
        
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      Published date: 2010
 
    
  
  
    
  
    
  
    
  
    
  
    
  
    
  
    
  
    
  
  
  
    
  
  
        Identifiers
        Local EPrints ID: 179039
        URI: http://eprints.soton.ac.uk/id/eprint/179039
        
          
        
        
        
          ISSN: 0550-3213
        
        
          PURE UUID: 657ce717-8325-4c13-9487-9a7860297db9
        
  
    
        
          
            
          
        
    
        
          
        
    
        
          
        
    
  
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  Date deposited: 26 Apr 2011 10:33
  Last modified: 14 Mar 2024 02:47
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      Contributors
      
        
      
          
          Author:
          
            
            
              G.K. Leontaris
            
          
        
      
          
          Author:
          
            
            
              G.G. Ross
            
          
        
      
      
      
    
  
   
  
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