Anderson impurity model

The Anderson impurity model, named after Philip Warren Anderson, is a Hamiltonian that is used to describe magnetic impurities embedded in metals. It is often applied to the description of Kondo effect-type problems, such as heavy fermion systems and Kondo insulators. In its simplest form, the model contains a term describing the kinetic energy of the conduction electrons, a two-level term with an on-site Coulomb repulsion that models the impurity energy levels, and a hybridization term that couples conduction and impurity orbitals. For a single impurity, the Hamiltonian takes the form

$H=\sum _{k,\sigma }\epsilon _{k}c_{k\sigma }^{\dagger }c_{k\sigma }+\sum _{\sigma }\epsilon _{f}f_{\sigma }^{\dagger }f_{\sigma }+Uf_{\uparrow }^{\dagger }f_{\uparrow }f_{\downarrow }^{\dagger }f_{\downarrow }+\sum _{k,\sigma }V_{k}(f_{\sigma }^{\dagger }c_{k\sigma }+c_{k\sigma }^{\dagger }f_{\sigma })$,

where the $c$ operator is the annihilation operator of a conduction electron, and $f$ is the annihilation operator for the impurity, $k$ is the conduction electron wavevector, and $\sigma$ labels the spin. The on–site Coulomb repulsion is $U$, and $V$ gives the hybridization.

For heavy-fermion systems, a lattice of impurities is described by the periodic Anderson model. The one-dimensional model is

$H=\sum _{k,\sigma }\epsilon _{k}c_{k\sigma }^{\dagger }c_{k\sigma }+\sum _{j,\sigma }\epsilon _{f}f_{j\sigma }^{\dagger }f_{j\sigma }+U\sum _{j}f_{j\uparrow }^{\dagger }f_{j\uparrow }f_{j\downarrow }^{\dagger }f_{j\downarrow }+\sum _{j,k,\sigma }V_{jk}(e^{ikx_{j}}f_{j\sigma }^{\dagger }c_{k\sigma }+e^{-ikx_{j}}c_{k\sigma }^{\dagger }f_{j\sigma })$,

where $x_{j}$ is the position of impurity site $j$. The hybridization term allows f-orbital electrons in heavy fermion systems to interact, although they are separated by a distance greater than the Hill limit.

There are other variants of the Anderson model, such as the SU(4) Anderson model, which is used to describe impurities which have an orbital, as well as a spin, degree of freedom. This is relevant in carbon nanotube quantum dot systems. The SU(4) Anderson model Hamiltonian is

$H=\sum _{k,\sigma }\epsilon _{k}c_{k\sigma }^{\dagger }c_{k\sigma }+\sum _{i,\sigma }\epsilon _{f}f_{i\sigma }^{\dagger }f_{i\sigma }+\sum _{i,\sigma ,i'\sigma '}{\frac {U}{2}}n_{i\sigma }n_{i'\sigma '}+\sum _{i,k,\sigma }V_{k}(f_{i\sigma }^{\dagger }c_{k\sigma }+c_{k\sigma }^{\dagger }f_{i\sigma })$,

where $i$ and $i'$ label the orbital degree of freedom (which can take one of two values), and $n$ represents the number operator for the impurity.

See also

• Kondo effect
• Kondo model
• Anderson localization

References

• Anderson, P. W. (1961). "Localized Magnetic States in Metals". Phys. Rev. 124 (1): 41–53. Bibcode:1961PhRv..124...41A. doi:10.1103/PhysRev.124.41.
• Hewson, A. C. (1993). The Kondo Problem to Heavy Fermions. New York: Cambridge University Press.