In theoretical physics, the R-symmetry is the symmetry transforming different supercharges in a theory with supersymmetry into each other. More precisely, it is the only such symmetry commuting with Lorentz transformations which is allowed by the Haag–Łopuszański–Sohnius theorem. In the simplest case of the N = 1 {\displaystyle {\mathcal {N}}=1} supersymmetry, such an R-symmetry is isomorphic to a global U ( 1 ) {\displaystyle \operatorname {U} (1)} group or a discrete subgroup thereof (for the Z2 subgroup it is called R-parity). This symmetry is realised, for example, in special cases of the Wess-Zumino model. For extended supersymmetry, the R-symmetry group becomes a global U ( N ) {\displaystyle \operatorname {U} ({\mathcal {N}})} non-abelian group (it can also be SU ( 4 ) {\displaystyle \operatorname {SU} (4)} in the N = 4 {\displaystyle {\mathcal {N}}=4} case). In a model that is classically invariant under both N = 1 {\displaystyle {\mathcal {N}}=1} supersymmetry and conformal transformations (such as the massless version of aforementioned Wess-Zumino model), the closure of the superconformal algebra (at least on-shell) needs the introduction of a further bosonic generator that is associated to the R-symmetry.
References José M. Figueroa-O'Farrill (2001). "BUSSTEPP lectures on supersymmetry". arXiv:hep-th/0109172v1. Haag, R.; Łopuszański, J.T.; Sohnius, M. (1975). "All possible generators of supersymmetries of the S-matrix". Nuclear Physics B. 88 (2): 257–274. Bibcode:1975NuPhB..88..257H. doi:10.1016/0550-3213(75)90279-5. Bernard de Wit (2002). "Supergravity". arXiv:hep-th/0212245. Antoine Van Proeyen (1999). "Tools for supersymmetry". arXiv:hep-th/9910030.
