Changes between Version 2 and Version 3 of GeneralFCNTop


Ignore:
Timestamp:
10/23/15 02:54:34 (19 months ago)
Author:
arturamorim
Comment:

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  • GeneralFCNTop

    v2 v3  
    77=== Model Implementation === 
    88Our lagrangian was derived in the context of an effective field theory using dimension-six gauge invariant operators. In general this lagrangian can be written as[[BR]] 
    9 [[Image()]] 
     9[[Image(leff.png)]][[BR]] 
     10where Cx is a complex number and Ox is a dimension-six gauge invariant operator. In [1, 2] we can find the list of the most relevant and non-redundant operators Ox that are responsible for top anomalous interactions, in partic- ular for flavour changing neutral interactions. Using the results from those papers we arrive at the lagrangian of equation 2 wich is added to the SM lagrangian[[BR]] 
     11[[Image(lfcnc.png)]] 
     12 
     13=== References === 
     14[1] J.A. Aguilar Saavedra, A minimal set of top anomalous couplings, arXiv:0811.3842v2 [hep-ph], 2008[[BR]] 
     15[2] J.A. Aguilar Saavedra, A minimal set of top-Higgs anomalous couplings, arXiv:0904.2387v2 [hep-ph], 2009