Weak corrections to four-parton processes
Weak corrections to four-parton processes
 
  We report on a calculation of the ‘mixed’ strong and (purely) weak corrections through the order αS2αW to parton–parton processes in all possible channels at hadron colliders entering the single jet inclusive cross section. At both Tevatron and LHC, such effects are always negligible (below permille level) in the total integrated cross section whilst they become sizable in differential rates. Specifically, if such corrections are defined with respect to the full leading-order result of [equ'n], we find that, at the FNAL accelerator, they can reach the -5% benchmark in the jet transverse energy (at the kinematical limit of the machine, rendering their detection quite difficult). At the CERN collider, in the same observable, they exceed the -10% level already at 1 TeV and can reach -40% at 4 TeV, kinematic regions where such corrections will be comfortably observable for standard luminosity. In addition, such corrections are somewhat sensitive to the factorisation/renormalisation scale choice.
  hadron colliders, electroweak physics, higher-order calculations
  
  
  50-82
  
    
      Moretti, S.
      
        b57cf0f0-4bc3-4e02-96e3-071255366614
      
     
  
    
      Nolten, M.R.
      
        4f2ad5b9-777d-4337-ab8c-0de1605b4ea2
      
     
  
    
      Ross, D.A.
      
        eb79bbfe-fb97-4bb3-813c-98f278e5a55f
      
     
  
  
   
  
  
    
      18 December 2006
    
    
  
  
    
      Moretti, S.
      
        b57cf0f0-4bc3-4e02-96e3-071255366614
      
     
  
    
      Nolten, M.R.
      
        4f2ad5b9-777d-4337-ab8c-0de1605b4ea2
      
     
  
    
      Ross, D.A.
      
        eb79bbfe-fb97-4bb3-813c-98f278e5a55f
      
     
  
       
    
 
  
    
      
  
  
  
  
  
  
    Moretti, S., Nolten, M.R. and Ross, D.A.
  
  
  
  
   
    (2006)
  
  
    
    Weak corrections to four-parton processes.
  
  
  
  
    Nuclear Physics B - Proceedings Supplements, 759 (1-2), .
  
   (doi:10.1016/j.nuclphysb.2006.09.028). 
  
  
   
  
  
  
  
  
   
  
    
      
        
          Abstract
          We report on a calculation of the ‘mixed’ strong and (purely) weak corrections through the order αS2αW to parton–parton processes in all possible channels at hadron colliders entering the single jet inclusive cross section. At both Tevatron and LHC, such effects are always negligible (below permille level) in the total integrated cross section whilst they become sizable in differential rates. Specifically, if such corrections are defined with respect to the full leading-order result of [equ'n], we find that, at the FNAL accelerator, they can reach the -5% benchmark in the jet transverse energy (at the kinematical limit of the machine, rendering their detection quite difficult). At the CERN collider, in the same observable, they exceed the -10% level already at 1 TeV and can reach -40% at 4 TeV, kinematic regions where such corrections will be comfortably observable for standard luminosity. In addition, such corrections are somewhat sensitive to the factorisation/renormalisation scale choice.
        
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      Published date: 18 December 2006
 
    
  
  
    
  
    
  
    
  
    
  
    
  
    
     
        Keywords:
        hadron colliders, electroweak physics, higher-order calculations
      
    
  
    
  
    
  
  
        Identifiers
        Local EPrints ID: 57486
        URI: http://eprints.soton.ac.uk/id/eprint/57486
        
          
        
        
        
          ISSN: 0920-5632
        
        
          PURE UUID: c99bc80f-7cf3-43a6-b932-8f7e4eecb858
        
  
    
        
          
            
              
            
          
        
    
        
          
        
    
        
          
            
          
        
    
  
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  Date deposited: 14 Aug 2008
  Last modified: 16 Mar 2024 03:34
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      Contributors
      
        
      
          
          Author:
          
            
            
              M.R. Nolten
            
          
        
      
        
      
      
      
    
  
   
  
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