Supersymmetric gauge theory
This article reads like a quality standards . (September 2015) |
In
Gauge theory
A
Quantum chromodynamics and quantum electrodynamics are famous examples of gauge theories.
Supersymmetry
In
This unification is given by an
For instance, the supersymmetry generator can take a photon as an argument and transform it into a photino and vice versa. This happens through translation in the (parameter) space. This superspace is a -graded vector space , where is the bosonic Hilbert space and is the fermionic Hilbert space.
SUSY gauge theory
The motivation for a supersymmetric version of gauge theory can be the fact that gauge invariance is consistent with supersymmetry. The first examples were discovered by Bruno Zumino and Sergio Ferrara, and independently by Abdus Salam and James Strathdee in 1974.
Both the half-integer spin fermions and the integer spin bosons can become gauge particles. The gauge vector fields and its spinorial superpartner can be made to both reside in the same representation of the internal symmetry group.
Suppose we have a gauge transformation , where is a vector field and is the gauge function. The main difficulty in construction of a SUSY Gauge Theory is to extend the above transformation in a way that is consistent with SUSY transformations.
The
N = 1 SUSY in 4D (with 4 real generators)
In four dimensions, the minimal N = 1 supersymmetry may be written using a superspace. This superspace involves four extra fermionic coordinates , transforming as a two-component spinor and its conjugate.
Every superfield, i.e. a field that depends on all coordinates of the superspace, may be expanded with respect to the new fermionic coordinates. There exists a special kind of superfields, the so-called
V is the vector superfield (prepotential) and is real (V = V). The fields on the right hand side are component fields.
The
where Λ is any chiral superfield.
It's easy to check that the chiral superfield
is gauge invariant. So is its complex conjugate .
A non-supersymmetric covariant gauge which is often used is the Wess–Zumino gauge. Here, C, χ, M and N are all set to zero. The residual gauge symmetries are gauge transformations of the traditional bosonic type.
A chiral superfield X with a charge of q transforms as
Therefore Xe−qVX is gauge invariant. Here e−qV is called a bridge since it "bridges" a field which transforms under Λ only with a field which transforms under Λ only.
More generally, if we have a real gauge group G that we wish to supersymmetrize, we first have to
Differential superforms
Let's rephrase everything to look more like a conventional
leave us with
A similar constraint for antichiral superfields leaves us with Fαβ = 0. This means that we can either gauge fix or Aα = 0 but not both simultaneously. Call the two different gauge fixing schemes I and II respectively. In gauge I, and in gauge II, dα X = 0. Now, the trick is to use two different gauges simultaneously; gauge I for chiral superfields and gauge II for antichiral superfields. In order to bridge between the two different gauges, we need a gauge transformation. Call it e−V (by convention). If we were using one gauge for all fields, XX would be gauge invariant. However, we need to convert gauge I to gauge II, transforming X to (e−V)qX. So, the gauge invariant quantity is Xe−qVX.
In gauge I, we still have the residual gauge eΛ where and in gauge II, we have the residual gauge eΛ satisfying dα Λ = 0. Under the residual gauges, the bridge transforms as
Without any additional constraints, the bridge e−V wouldn't give all the information about the gauge field. However, with the additional constraint , there's only one unique gauge field which is compatible with the bridge modulo gauge transformations. Now, the bridge gives exactly the same information content as the gauge field.
Theories with 8 or more SUSY generators (N > 1)
In theories with higher supersymmetry (and perhaps higher dimension), a vector superfield typically describes not only a gauge field and a Weyl fermion but also at least one complex scalar field.
Examples
Pure supersymmetric gauge theories
Supersymmetric gauge theories with matter
- Super QCD
- MSSM (Minimal supersymmetric Standard Model)
- NMSSM(Next-to-minimal supersymmetric Standard Model)
See also
- superpotential
- D-term
- F-term
- current superfield
- Supersymmetric quantum mechanics
References
- Stephen P. Martin. A Supersymmetry Primer, arXiv:hep-ph/9709356.
- Prakash, Nirmala. Mathematical Perspective on Theoretical Physics: A Journey from Black Holes to Superstrings, World Scientific (2003).
- Kulshreshtha, D. S.; Mueller-Kirsten, H. J. W. (1991). "Quantization of systems with constraints: The Faddeev-Jackiw method versus Dirac's method applied to superfields". Physical Review D. Phys. Rev. D43, 3376-3383. 43 (10): 3376–3383. .