Schrieffer–Wolff transformation
The Schrieffer–Wolff transformation is a unitary transformation enabling one to obtain effective low energy physics from a given interacting and non-interacting Hamiltonians.[1] An important application of Schrieffer–Wolff method is the derivation of Kondo model from single impurity Anderson model, as first noticed by J.R. Schrieffer and P.A. Wolff.[2]
References
- ↑ Bravyi, S., DiVincenzo, D. and Loss, D. "Schrieffer-Wolff transformation for quantum many-body systems". Annals of Physics. 326 (10): 2793–2826. arXiv:1105.0675
. Bibcode:2011AnPhy.326.2793B. doi:10.1016/j.aop.2011.06.004. - ↑ Schrieffer, J.R.; Wolff, P.A. (September 1966). "Relation between the Anderson and Kondo Hamiltonians". Physical Review. 149 (2): 491–492. Bibcode:1966PhRv..149..491S. doi:10.1103/PhysRev.149.491.
Further reading
- Phillips, Philip (2012). Advanced Solid State Physics (Second ed.). New York: Cambridge University Press. pp. 109–114. ISBN 978-1-107-49346-9.
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