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Published byIrwan Sugiarto Modified over 5 years ago
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Basic diffusion propagator in small freq. & wave number limit
Gaussian Propagators Paramagnon propagator spin-singlet spin-triplet heat diffusion Basic diffusion propagator in small freq. & wave number limit
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Perturbation theory to all orders
3 points vertices The one-loop renormalization is a finite number (scale like (d-2)) n-loop skeleton diagrams scale like n(d-2) 4 points vertices vertex k2 - GH renorm. of k dependent part -> finite number renorm. of dependent part can give log singularities HOWEVER one-loop renorm of H from 4-point vertex is identical to that obtained by renormalizing the 2-point vertex
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Perturbation theory to all orders
2 points vertices One-loop renormalization of the mixed 2 point vertex One-loop renormalization of the magnetic 2 point vertex One-loop renormalization of the fermionic 2 point vertex Renormalization to all orders fermionic vertex magnetization vertex D(in)=1/GH(i n) Ds(k, in)=u2 (k, in)/GKt D(0)=D0[g(ln 1/)]-1 Ds(k 0, 0)= Ds0(k)d-2[g(2ln kF/k)]-1
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