Abstract
We introduce the core concepts and formalisms that are needed in our search for a noncommutative geometric description of supersymmetric theories. We start with a concise overview of supersymmetry and the minimal supersymmetric extension of the Standard Model (MSSM). We then provide a bird’s eye view of noncommutative geometry, geared towards its applications in high-energy physics.
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Notes
- 1.
The possible values for N, the number of supersymmetry generators, depend on the space-time dimension. For example, for \(d = 4\), \(N = 1, 2, 4\) or 8.
- 2.
This makes it an example of \(N=1\) supersymmetry.
- 3.
One should keep in mind though that Minkowski space is not an example of a Riemannian manifold. Rather it is pseudo-Riemannian since its metric is diagonal with negative entries.
- 4.
The parameter \(\varLambda \) more or less serves as a cut-off, and will in the derivation of the SM (Sect. 1.2.3 ahead) be interpreted as the GUT-scale.
- 5.
To be explicit, the element \((\lambda , q, m)\in \mathscr {A}_F\) acts on—say—\({\mathbf {2}} \otimes {\mathbf {3}}^o \ni v\otimes \bar{w}\) as \(qv \otimes \bar{w} m = qv \otimes \overline{m^*w}\).
- 6.
An exception to this rule is when one component of the algebra acts in the same way on more than one different representations in \(\mathscr {H}_F\).
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Beenakker, W., van den Broek, T., van Suijlekom, W.D. (2016). Introduction. In: Supersymmetry and Noncommutative Geometry. SpringerBriefs in Mathematical Physics, vol 9. Springer, Cham. https://doi.org/10.1007/978-3-319-24798-4_1
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