Physics:Thirring–Wess model
The Thirring–Wess model or Vector Meson model is an exactly solvable quantum field theory, describing the interaction of a Dirac field with a vector field in dimension two.
Definition
The Lagrangian density is made of three terms:
the free vector field [math]\displaystyle{ A^\mu }[/math] is described by
- [math]\displaystyle{ {(F^{\mu\nu})^2 \over 4} +{\mu^2\over 2} (A^\mu)^2 }[/math]
for [math]\displaystyle{ F^{\mu\nu}= \partial^\mu A^\nu - \partial^\nu A^\mu }[/math] and the boson mass [math]\displaystyle{ \mu }[/math] must be strictly positive; the free fermion field [math]\displaystyle{ \psi }[/math] is described by
- [math]\displaystyle{ \overline{\psi}(i\partial\!\!\!/-m)\psi }[/math]
where the fermion mass [math]\displaystyle{ m }[/math] can be positive or zero. And the interaction term is
- [math]\displaystyle{ qA^\mu(\bar\psi\gamma^\mu\psi) }[/math]
Although not required to define the massive vector field, there can be also a gauge-fixing term
- [math]\displaystyle{ {\alpha\over 2} (\partial^\mu A^\mu)^2 }[/math]
for [math]\displaystyle{ \alpha \ge 0 }[/math]
There is a remarkable difference between the case [math]\displaystyle{ \alpha \gt 0 }[/math] and the case [math]\displaystyle{ \alpha = 0 }[/math]: the latter requires a field renormalization to absorb divergences of the two point correlation.
History
This model was introduced by Thirring and Wess as a version of the Schwinger model with a vector mass term in the Lagrangian .
When the fermion is massless ([math]\displaystyle{ m = 0 }[/math]), the model is exactly solvable. One solution was found, for [math]\displaystyle{ \alpha = 1 }[/math], by Thirring and Wess [1] using a method introduced by Johnson for the Thirring model; and, for [math]\displaystyle{ \alpha = 0 }[/math], two different solutions were given by Brown[2] and Sommerfield.[3] Subsequently Hagen[4] showed (for [math]\displaystyle{ \alpha = 0 }[/math], but it turns out to be true for [math]\displaystyle{ \alpha \ge 0 }[/math]) that there is a one parameter family of solutions.
References
- ↑ Thirring, WE; Wess, JE (1964). "Solution of a field theoretical model in one space one time dimensions". Annals of Physics 27 (2): 331–337. doi:10.1016/0003-4916(64)90234-9. Bibcode: 1964AnPhy..27..331T.
- ↑ Brown, LS (1963). "Gauge invariance and Mass in a Two-Dimensional Model". Il Nuovo Cimento 29 (3): 617–643. doi:10.1007/BF02827786. Bibcode: 1963NCim...29..617B.
- ↑ Sommerfield, CM (1964). "On the definition of currents and the action principle in field theories of one spatial dimension". Annals of Physics 26 (1): 1–43. doi:10.1016/0003-4916(64)90273-8. Bibcode: 1964AnPhy..26....1S.
- ↑ Hagen, CR (1967). "Current definition and mass renormalization in a Model Field Theory". Il Nuovo Cimento A 51 (4): 1033–1052. doi:10.1007/BF02721770. Bibcode: 1967NCimA..51.1033H.
External links
Original source: https://en.wikipedia.org/wiki/Thirring–Wess model.
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