We investigate the formation of rashbon bound states and strong-coupling effects in an ultracold Fermi gas with a spherical spin-orbit interaction, H so = λ p p p · σ (where σ = (σ x , σ y , σ z ) are Pauli matrices). Extending the strong-coupling theory developed by Nozières and Schmitt-Rink (NSR) to include this spin-orbit coupling, we determine the superfluid phase transition temperature T c , as functions of the strength of a pairing interaction U s , as well as the spin-orbit coupling strength λ . Evaluating poles of the NSR particleparticle scattering matrix describing fluctuations in the Cooper channel, we clarify the region where rashbon bound states dominate the superfluid phase transition in the U s -λ phase diagram. Since the antisymmetric spin-orbit interaction H so breaks the inversion symmetry of the system, rashbon bound states naturally have, not only a spin-singlet and even-parity symmetry, but also a spin-triplet and odd-parity symmetry. Thus, our results would be also useful for the study of this parity mixing effect in the BCS-BEC crossover regime of a spinorbit coupled Fermi gas.