Emerging understanding of the ΔI = 1/2 rule from lattice QCD
Emerging understanding of the ΔI = 1/2 rule from lattice QCD
 
  There has been much speculation as to the origin of the ΔI = 1/2 rule (ReA0/ReA2 ~ 22.5). We find that the two dominant contributions to the ΔI = 3/2, K → π π correlation functions have opposite signs, leading to a significant cancelation. This partial cancelation occurs in our computation of ReA2 with physical quark masses and kinematics (where we reproduce the experimental value of A2) and also for heavier pions at threshold. For ReA0, although we do not have results at physical kinematics, we do have results for pions at zero momentum with mπ ~ 420 MeV [ReA0/ReA2 = 9.1 (2.1)] and mπ ~ 330 MeV [ReA0/ReA2 = 12.0 (1.7)]. The contributions which partially cancel in ReA2 are also the largest ones in ReA0, but now they have the same sign and so enhance this amplitude. The emerging explanation of the ΔI = 1/2 rule is a combination of the perturbative running to scales of O (2 GeV), a relative suppression of ReA2 through the cancelation of the two dominant contributions, and the corresponding enhancement of ReA0. QCD and electroweak penguin operators make only very small contributions at such scales.
  
  152001-152006
  
    
      Boyle, P.A.
      
        deafc6c3-3d18-4199-84f5-6f20cd03e311
      
     
  
    
      Christ, N.H.
      
        bca5b070-bac5-4160-b12c-826a608a12b4
      
     
  
    
      Garron, N.
      
        4652f982-8723-41c1-9bf7-46bc5c54c2db
      
     
  
    
      Goode, E.J.
      
        29354b98-c117-4ace-9ca4-1d3ad531485f
      
     
  
    
      Janowski, T.
      
        a2f6e700-6ae9-4a93-93f9-095cbe0ca850
      
     
  
    
      Lehner, C.
      
        f5ed25c1-68c1-4a5f-9e01-73233639caae
      
     
  
    
      Liu, Q.
      
        9c3579c5-8fa0-402b-ad8e-83f4542b1b05
      
     
  
    
      Lytle, A. T.
      
        e6079fc7-7c8f-4481-ab83-45d4e6ae3426
      
     
  
    
      Sachrajda, C.T.
      
        0ed6568b-f52f-4314-8677-4aeeb925d6f7
      
     
  
    
      Soni, A.
      
        7a4196ff-0f6b-429e-af54-d1036e9c433b
      
     
  
    
      Zhang, D.
      
        1c04f0f4-c07c-4671-8fd0-fa07a685fea2
      
     
  
  
   
  
  
    
      9 April 2013
    
    
  
  
    
      Boyle, P.A.
      
        deafc6c3-3d18-4199-84f5-6f20cd03e311
      
     
  
    
      Christ, N.H.
      
        bca5b070-bac5-4160-b12c-826a608a12b4
      
     
  
    
      Garron, N.
      
        4652f982-8723-41c1-9bf7-46bc5c54c2db
      
     
  
    
      Goode, E.J.
      
        29354b98-c117-4ace-9ca4-1d3ad531485f
      
     
  
    
      Janowski, T.
      
        a2f6e700-6ae9-4a93-93f9-095cbe0ca850
      
     
  
    
      Lehner, C.
      
        f5ed25c1-68c1-4a5f-9e01-73233639caae
      
     
  
    
      Liu, Q.
      
        9c3579c5-8fa0-402b-ad8e-83f4542b1b05
      
     
  
    
      Lytle, A. T.
      
        e6079fc7-7c8f-4481-ab83-45d4e6ae3426
      
     
  
    
      Sachrajda, C.T.
      
        0ed6568b-f52f-4314-8677-4aeeb925d6f7
      
     
  
    
      Soni, A.
      
        7a4196ff-0f6b-429e-af54-d1036e9c433b
      
     
  
    
      Zhang, D.
      
        1c04f0f4-c07c-4671-8fd0-fa07a685fea2
      
     
  
       
    
 
  
    
      
  
  
  
  
  
  
    Boyle, P.A., Christ, N.H., Garron, N., Goode, E.J., Janowski, T., Lehner, C., Liu, Q., Lytle, A. T., Sachrajda, C.T., Soni, A. and Zhang, D.
  
  
  
  
   
    (2013)
  
  
    
    Emerging understanding of the ΔI = 1/2 rule from lattice QCD.
  
  
  
  
    Physical Review Letters, 110 (15), .
  
   (doi:10.1103/PhysRevLett.110.152001). 
  
  
  
    (PMID:25167252)
   
  
  
  
  
  
   
  
    
    
      
        
          Abstract
          There has been much speculation as to the origin of the ΔI = 1/2 rule (ReA0/ReA2 ~ 22.5). We find that the two dominant contributions to the ΔI = 3/2, K → π π correlation functions have opposite signs, leading to a significant cancelation. This partial cancelation occurs in our computation of ReA2 with physical quark masses and kinematics (where we reproduce the experimental value of A2) and also for heavier pions at threshold. For ReA0, although we do not have results at physical kinematics, we do have results for pions at zero momentum with mπ ~ 420 MeV [ReA0/ReA2 = 9.1 (2.1)] and mπ ~ 330 MeV [ReA0/ReA2 = 12.0 (1.7)]. The contributions which partially cancel in ReA2 are also the largest ones in ReA0, but now they have the same sign and so enhance this amplitude. The emerging explanation of the ΔI = 1/2 rule is a combination of the perturbative running to scales of O (2 GeV), a relative suppression of ReA2 through the cancelation of the two dominant contributions, and the corresponding enhancement of ReA0. QCD and electroweak penguin operators make only very small contributions at such scales.
         
      
      
        
          
            
  
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 PhysRevLett.110.152001
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      Published date: 9 April 2013
 
    
  
  
    
  
    
  
    
  
    
  
    
  
    
  
    
     
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        Local EPrints ID: 350975
        URI: http://eprints.soton.ac.uk/id/eprint/350975
        
          
        
        
        
        
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  Date deposited: 11 Apr 2013 14:01
  Last modified: 14 Mar 2024 13:34
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      Contributors
      
          
          Author:
          
            
            
              P.A. Boyle
            
          
        
      
          
          Author:
          
            
            
              N.H. Christ
            
          
        
      
          
          Author:
          
            
            
              N. Garron
            
          
        
      
          
          Author:
          
            
            
              E.J. Goode
            
          
        
      
          
          Author:
          
            
            
              T. Janowski
            
          
        
      
          
          Author:
          
            
            
              C. Lehner
            
          
        
      
          
          Author:
          
            
            
              Q. Liu
            
          
        
      
          
          Author:
          
            
            
              A. T. Lytle
            
          
        
      
        
      
          
          Author:
          
            
            
              A. Soni
            
          
        
      
          
          Author:
          
            
            
              D. Zhang
            
          
        
      
      
      
    
  
   
  
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