Soler model

Type of 3+1 dimensional quantum field theory From Wikipedia, the free encyclopedia

The soler model is a quantum field theory model of Dirac fermions interacting via four fermion interactions in 3 spatial and 1 time dimension. It was introduced in 1938 by Dmitri Ivanenko [1] and re-introduced and investigated in 1970 by Mario Soler[2] as a toy model of self-interacting electron.

This model is described by the Lagrangian density

where is the coupling constant, in the Feynman slash notations, . Here , , are Dirac gamma matrices.

The corresponding equation can be written as

,

where , , and are the Dirac matrices. In one dimension, this model is known as the massive Gross–Neveu model.[3][4]

Generalizations

Summarize
Perspective

A commonly considered generalization is

with , or even

,

where is a smooth function.

Features

Internal symmetry

Besides the unitary symmetry U(1), in dimensions 1, 2, and 3 the equation has SU(1,1) global internal symmetry.[5]

Renormalizability

The Soler model is renormalizable by the power counting for and in one dimension only, and non-renormalizable for higher values of and in higher dimensions.

Solitary wave solutions

The Soler model admits solitary wave solutions of the form where is localized (becomes small when is large) and is a real number.[6]

Reduction to the massive Thirring model

In spatial dimension 2, the Soler model coincides with the massive Thirring model, due to the relation , with the relativistic scalar and the charge-current density. The relation follows from the identity , for any .[7]

See also

References

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