The use of exact Dirac-Coulomb propagators allows the evaluation of binding corrections to the Schwinger correction in ground state muonium hyperfine splitting to all orders. The calculational method is described and the results are used firstly to verify recent perturbative calculations of higherorder binding corrections and secondly to evaluate the residual terms of still higher order. Implications for muonium hyperfine splitting are discussed. [S0031-9007(97)03490-X] PACS numbers: 36.10. Dr, 12.20.Ds, 31.30.Gs Calculations of radiative corrections in atomic physics are frequently expressed in terms of a double expansion in the fine structure constant a and the quantity Za, where Z is the nuclear charge. This is done even when Z 1, as it serves to distinguish purely radiative effects from binding corrections, which are effects arising from the expansion of the Dirac-Coulomb propagator in terms of interactions with the nuclear Coulomb potential. In atomic physics, these binding corrections can have large coefficients, which has two consequences. One is that at high Z, these large coefficients now multiply the no longer small quantity Za, and a complete breakdown of the series may result, in the sense that the value of the series terminated at a given order can change in sign and order of magnitude when the next order is included. For highly charged ions there is no substitute for a nonperturbative evaluation to all orders in Za. The second is that even at Z 1, adequate comparison with high-accuracy experiments can require relatively high orders of perturbation theory to be considered. Given that the already quite precisely determined hyperfine splitting of the ground state of muonium [1], Dn exp 4 463 302.88͑16͒ kHz , (1) is in the process of being even more accurately measured [2], a complete treatment of these high-order terms has become an important problem for QED theory.It is convenient to define a set of functions D ͑2n͒ ͑Za͒ that parametrize radiative corrections to the ground-state hyperfine splitting. Specifically, in the nonrecoil, pointnucleus limit, radiative corrections to muonium hyperfine splitting can be written as