Physics:Four-fermion interactions

Short description: Point interactions with four fermions

In quantum field theory, fermions are described by anticommuting spinor fields. A four-fermion interaction describes a local interaction between four fermionic fields at a point in spacetime. A theory involving such an interaction might be an effective field theory or it might be fundamental.

In four spacetime dimensions, such theories are not renormalisable.

Relativistic models

Some examples are the following:

• Fermi's theory of the weak interaction. The interaction term has a V − A (vector minus axial) form.
• The Gross–Neveu model. This is a four-fermi theory of Dirac fermions without chiral symmetry and as such, it may or may not be massive.
• The Thirring model. This is a four-fermi theory of fermions with a vector coupling.
• The Nambu–Jona-Lasinio model. This is a four-fermi theory of Dirac fermions with chiral symmetry and as such, it has no bare mass.

Nonrelativistic models

A nonrelativistic example is the BCS theory at large length scales with the phonons integrated out so that the force between two dressed electrons is approximated by a contact term.

See also

• Oblique correction
• Peskin–Takeuchi parameter

References

• Klevansky, S. P. (1992). "The Nambu—Jona-Lasinio model of quantum chromodynamics". Reviews of Modern Physics 64 (3): 649–708. doi:10.1103/revmodphys.64.649. 
• Kondo, Kei-ichi (1995). "Thirring model as a gauge theory". Nuclear Physics B 450 (1-2): 251–266. doi:10.1016/0550-3213(95)00316-K. 
• Thies, Michael (2014). "Integrable Gross-Neveu models with fermion-fermion and fermion-antifermion pairing". Physical Review D 90 (10). doi:10.1103/PhysRevD.90.105017. 
• Zee, Anthony (2010). Quantum Field Theory in a Nutshell (2nd ed.). Princeton University Press. ISBN 978-0-691-14034-6.