Anderson orthogonality theorem

The Anderson orthogonality theorem is a theorem in physics by the physicist P. W. Anderson.

It relates to the introduction of a magnetic impurity in a metal. When a magnetic impurity is introduced into a metal, the conduction electrons will tend to screen the potential $V(r)$ that the impurity creates. The N-electron ground state for the system when $V(r)=0$, which corresponds to the absence of the impurity and $V(r)\neq 0$, which corresponds to the introduction of the impurity are orthogonal in the thermodynamic limit $N\to \infty$.

References

• P. W. Anderson (1967). "Infrared Catastrophe in Fermi Gases with Local Scattering Potentials". Physical Review Letters. 18 (24): 1049. Bibcode:1967PhRvL..18.1049A. doi:10.1103/PhysRevLett.18.1049.
• P. W. Anderson (1967). "Ground State of a Magnetic Impurity in a Metal". Physical Review. 164 (2): 352. Bibcode:1967PhRv..164..352A. doi:10.1103/PhysRev.164.352.