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Renormalization group theory flow equations

Let us now embed the renormalization group, Constructed in Chap. 8, iftto this general framework. As mentioned above, relation (8.5) shows that the RG we are searching for must be a nonlinear representation of the group of dilatations in the space of parameters. , n,/ e). These are the microscopic parameters of the model, and the representation shall leave macroscopic observables invariant. Furthermore we want the representation to show a nontrivial fixed point. In Sect. 8.2 we have constructed such a representation based on first order perturbation theory. The invariance constraint is obeyed within deviations of order 1+e 2, no = n(A = 1). Equations (8.38), (8.42) give the parameter flow under this nonlinear representation in the standard form (10.28),... [Pg.165]


See other pages where Renormalization group theory flow equations is mentioned: [Pg.672]    [Pg.47]    [Pg.49]    [Pg.497]    [Pg.498]    [Pg.820]    [Pg.822]    [Pg.134]    [Pg.828]    [Pg.830]    [Pg.676]    [Pg.127]    [Pg.181]    [Pg.182]    [Pg.127]    [Pg.168]    [Pg.181]    [Pg.182]    [Pg.72]    [Pg.264]   
See also in sourсe #XX -- [ Pg.133 ]




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