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 ${\displaystyle V(r)}$ that the impurity creates. The N-electron ground state for the system when ${\displaystyle V(r)=0}$, which corresponds to the absence of the impurity and ${\displaystyle V(r)\neq 0}$, which corresponds to the introduction of the impurity are orthogonal in the thermodynamic limit ${\displaystyle N\to \infty }$.

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.

This condensed matter physics-related article is a stub. You can help Wikipedia by expanding it.

• v
• t
• e