We investigate the behaviour of two-dimensional quantum field theories with N = (0, 2) supersymmetry under a deformation induced by the "TT " composite operator. We show that the deforming operator can be defined by a point-splitting regularisation in such a way as to preserve N = (0, 2) supersymmetry. As an example of this construction, we work out the deformation of a free N = (0, 2) theory, compare to that induced by the Noether stress-energy tensor and argue that, despite their apparent difference, they are equivalent on-shell. Finally, we show that the N = (0, 2) supersymmetric deformed action actually possesses N = (2, 2) symmetry, half of which is non-linearly realised. arXiv:1904.04760v3 [hep-th]