An exploratory lattice study of ΔI = 3/2 K → pi pi decays at next-to-leading order in the chiral expansion
An exploratory lattice study of ΔI = 3/2 K → pi pi decays at next-to-leading order in the chiral expansion
 
  We present the first direct evaluation of ΔI =3/2 K ππ matrix elements with the aim of determining all the low-energy constants at NLO in the chiral expansion. Our numerical investigation demonstrates that it is indeed possible to determine the K → ππ matrix elements directly for the masses and momenta used in the simulation with good precision. In this range however, we find that the matrix elements do not satisfy the predictions of NLO chiral perturbation theory. For the chiral extrapolation we therefore use a hybrid procedure which combines the observed polynomial behavior in masses and momenta of our lattice results, with NLO chiral perturbation theory at lower masses. In this way we find stable results for the quenched matrix elements of the electroweak penguin operators (I=2 ⟨ππ|O8|K0⟩ = (0.68 ± 0.09) GeV3 and I=2 ⟨ππ|O7|K0⟩ = (0.12 ± 0.02) GeV3 in the NDR-‾MS scheme at the scale 2 GeV), but not for the matrix elements of O4 (for which there are too many low-energy constants at NLO for a reliable extrapolation). For all three operators we find that the effect of including the NLO corrections is significant (typically about 30%). We present a detailed discussion of the status of the prospects for the reduction of the systematic uncertainties.
  
  
  175-211
  
    
      Boucaud, Philippe
      
        b9cf7d17-6e2d-40cb-aa82-e66d202b3bcf
      
     
  
    
      Giménez, Vicent
      
        a7e2c06d-63d3-4972-b884-07bb57d846bb
      
     
  
    
      Lin, C.-J. David
      
        3b3ab1f2-efb6-4bd6-a92f-79a23d4b9945
      
     
  
    
      Lubicz, Vittorio
      
        801148ad-141c-41dc-9128-d0cd748bd5d3
      
     
  
    
      Martinelli, Guido
      
        9ce48c45-c91f-439b-a088-6cdcfb8b41cc
      
     
  
    
      Papinutto, Mauro
      
        e7cba614-180e-44a2-8502-2648f80c68c8
      
     
  
    
      Sachrajda, Chris T.
      
        0ed6568b-f52f-4314-8677-4aeeb925d6f7
      
     
  
  
   
  
  
    
      15 August 2005
    
    
  
  
    
      Boucaud, Philippe
      
        b9cf7d17-6e2d-40cb-aa82-e66d202b3bcf
      
     
  
    
      Giménez, Vicent
      
        a7e2c06d-63d3-4972-b884-07bb57d846bb
      
     
  
    
      Lin, C.-J. David
      
        3b3ab1f2-efb6-4bd6-a92f-79a23d4b9945
      
     
  
    
      Lubicz, Vittorio
      
        801148ad-141c-41dc-9128-d0cd748bd5d3
      
     
  
    
      Martinelli, Guido
      
        9ce48c45-c91f-439b-a088-6cdcfb8b41cc
      
     
  
    
      Papinutto, Mauro
      
        e7cba614-180e-44a2-8502-2648f80c68c8
      
     
  
    
      Sachrajda, Chris T.
      
        0ed6568b-f52f-4314-8677-4aeeb925d6f7
      
     
  
       
    
 
  
    
      
  
  
  
  
  
  
    Boucaud, Philippe, Giménez, Vicent, Lin, C.-J. David, Lubicz, Vittorio, Martinelli, Guido, Papinutto, Mauro and Sachrajda, Chris T.
  
  
  
  
   
    (2005)
  
  
    
    An exploratory lattice study of ΔI = 3/2 K → pi pi decays at next-to-leading order in the chiral expansion.
  
  
  
  
    Nuclear Physics B, 721 (1-3), .
  
   (doi:10.1016/j.nuclphysb.2005.05.025). 
  
  
   
  
  
  
  
  
   
  
    
      
        
          Abstract
          We present the first direct evaluation of ΔI =3/2 K ππ matrix elements with the aim of determining all the low-energy constants at NLO in the chiral expansion. Our numerical investigation demonstrates that it is indeed possible to determine the K → ππ matrix elements directly for the masses and momenta used in the simulation with good precision. In this range however, we find that the matrix elements do not satisfy the predictions of NLO chiral perturbation theory. For the chiral extrapolation we therefore use a hybrid procedure which combines the observed polynomial behavior in masses and momenta of our lattice results, with NLO chiral perturbation theory at lower masses. In this way we find stable results for the quenched matrix elements of the electroweak penguin operators (I=2 ⟨ππ|O8|K0⟩ = (0.68 ± 0.09) GeV3 and I=2 ⟨ππ|O7|K0⟩ = (0.12 ± 0.02) GeV3 in the NDR-‾MS scheme at the scale 2 GeV), but not for the matrix elements of O4 (for which there are too many low-energy constants at NLO for a reliable extrapolation). For all three operators we find that the effect of including the NLO corrections is significant (typically about 30%). We present a detailed discussion of the status of the prospects for the reduction of the systematic uncertainties.
        
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      Published date: 15 August 2005
 
    
  
  
    
  
    
  
    
  
    
  
    
  
    
  
    
  
    
  
  
        Identifiers
        Local EPrints ID: 57105
        URI: http://eprints.soton.ac.uk/id/eprint/57105
        
          
        
        
        
          ISSN: 0550-3213
        
        
          PURE UUID: ecef4d7a-9cdd-481f-bafa-3f0a8574497a
        
  
    
        
          
        
    
        
          
        
    
        
          
        
    
        
          
        
    
        
          
        
    
        
          
        
    
        
          
            
          
        
    
  
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  Date deposited: 15 Aug 2008
  Last modified: 15 Mar 2024 11:05
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      Contributors
      
          
          Author:
          
            
            
              Philippe Boucaud
            
          
        
      
          
          Author:
          
            
            
              Vicent Giménez
            
          
        
      
          
          Author:
          
            
            
              C.-J. David Lin
            
          
        
      
          
          Author:
          
            
            
              Vittorio Lubicz
            
          
        
      
          
          Author:
          
            
            
              Guido Martinelli
            
          
        
      
          
          Author:
          
            
            
              Mauro Papinutto
            
          
        
      
        
      
      
      
    
  
   
  
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