Holographic Nambu Jona-Lasinio interactions
Holographic Nambu Jona-Lasinio interactions
 
  Nambu–Jona-Lasinio (NJL) interactions are introduced into the D3/probe D7 system using Witten’s double trace operator prescription which includes the operator as a classical term in the effective potential. In the supersymmetric system the interactions do not induce chiral symmetry breaking, which we attribute to the flat effective potential with quark mass in the supersymmetric theory. If additional supersymmetry breaking is introduced, then standard NJL behavior is realized. In examples where chiral symmetry breaking is not preferred, such as with a B field plus an IR cutoff, chiral condensation is triggered by the NJL interaction at a second-order transition after a finite critical coupling. If the model already contains chiral symmetry breaking, for example in the B field case with no IR cutoff, then the NJL interaction enhances the quark mass at all values of the NJL coupling. We also consider the system at finite temperature: the temperature discourages condensation, but when combined with a magnetic field, we find regions of parameter space where the NJL interaction triggers a first-order chiral transition above a critical coupling.
  
  
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      Evans, Nicholas
      
        33dfbb52-64dd-4c1f-9cd1-074faf2be4b3
      
     
  
    
      Young, Keun
      
        122a4f92-f849-49ba-a29f-c9949f709c3a
      
     
  
  
   
  
  
    
    
  
    
      15 March 2016
    
    
  
  
    
      Evans, Nicholas
      
        33dfbb52-64dd-4c1f-9cd1-074faf2be4b3
      
     
  
    
      Young, Keun
      
        122a4f92-f849-49ba-a29f-c9949f709c3a
      
     
  
       
    
 
  
    
      
  
  
  
  
  
  
    Evans, Nicholas and Young, Keun
  
  
  
  
   
    (2016)
  
  
    
    Holographic Nambu Jona-Lasinio interactions.
  
  
  
  
    Physical Review D, 93 (66002), .
  
   (doi:10.1103/PhysRevD.93.066002). 
  
  
   
  
  
  
  
  
   
  
    
    
      
        
          Abstract
          Nambu–Jona-Lasinio (NJL) interactions are introduced into the D3/probe D7 system using Witten’s double trace operator prescription which includes the operator as a classical term in the effective potential. In the supersymmetric system the interactions do not induce chiral symmetry breaking, which we attribute to the flat effective potential with quark mass in the supersymmetric theory. If additional supersymmetry breaking is introduced, then standard NJL behavior is realized. In examples where chiral symmetry breaking is not preferred, such as with a B field plus an IR cutoff, chiral condensation is triggered by the NJL interaction at a second-order transition after a finite critical coupling. If the model already contains chiral symmetry breaking, for example in the B field case with no IR cutoff, then the NJL interaction enhances the quark mass at all values of the NJL coupling. We also consider the system at finite temperature: the temperature discourages condensation, but when combined with a magnetic field, we find regions of parameter space where the NJL interaction triggers a first-order chiral transition above a critical coupling.
         
      
      
        
          
            
  
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      Accepted/In Press date: 27 February 2016
 
    
      Published date: 15 March 2016
 
    
  
  
    
  
    
  
    
  
    
  
    
  
    
  
    
     
        Organisations:
        Theoretical Partical Physics Group
      
    
  
    
  
  
  
    
  
  
        Identifiers
        Local EPrints ID: 397417
        URI: http://eprints.soton.ac.uk/id/eprint/397417
        
          
        
        
        
          ISSN: 1550-7998
        
        
          PURE UUID: aa3441ff-5c62-4d28-b5bc-e9e3f3993b6b
        
  
    
        
          
            
          
        
    
        
          
        
    
  
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  Date deposited: 01 Jul 2016 08:30
  Last modified: 21 Aug 2025 14:18
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      Contributors
      
        
      
          
          Author:
          
            
            
              Keun Young
            
          
        
      
      
      
    
  
   
  
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