We study a two loop diagram of propagator type with general parameters through the Symmetries of Feynman Integrals (SFI) method. We present the SFI group and equation system, the group invariant in parameter space and a general representation as a line integral over simpler diagrams. We present close form expressions for three sectors, each with three or four energy scales, for any spacetime dimension d as well as the expansion. We determine the singular locus and the diagram's value on it. arXiv:1809.05040v3 [hep-th] 19 May 2019 ∂ 2 O 3 I(M 2 , m 2 t, m 2 4 , p 2 ) = J bubble (1, 1; M 2 , m 2 4 , p 2 )J tad (2; m 2 t) (5.37) with J tad and J bubble defined in (A.1) and (A.2) and given explicitly by J bubble (1, 1; M 2 , m 2 4 , p 2 ) = i 1−d π d/2 (−m 2 4 )