The Galerkin difference (GD) basis is a set of continuous, piecewise polynomials defined using a finite difference like grid of degrees of freedom. The one dimensional GD basis functions are naturally extended to multiple dimensions using the tensor product constructions to quadrilateral elements for discretizing partial differential equations. Here we propose two approaches to handling complex geometries using the GD basis within a discontinuous Galerkin finite element setting: (1) using non-conforming, curvilinear GD elements and (2) coupling affine GD elements with curvilinear simplicial elements. In both cases the (semidiscrete) discontinuous Galerkin method is provably energy stable even when variational crimes are committed and in both cases a weight-adjusted mass matrix is used, which ensures that only the reference mass matrix must be inverted. Additionally, we give sufficient conditions on the treatment of metric terms for the curvilinear, nonconforming GD elements to ensure that the scheme is both constant preserving and conservative. Numerical experiments confirm the stability results and demonstrate the accuracy of the coupled schemes.which means that for GD these calculations can be performed along the grid lines. We then define the metric terms needed at the quadrature nodes as the interpolation of these metric derivatives. Namely, we definewhere the operator diag(·) turns a vector into a diagonal matrix. When needed, the Jacobian determinant can be computed from these interpolated values as:An important property of our approach to computing the metric terms is that we preserve discretely the divergence theorem, which will enable us to show that the scheme can be made both conservative and constant preserving.