I can agree to everything than the last phrase. If this were true, quantum theory couldn't be the most successful theory ever. Of course, to empirically check probabilistic predictions you need an ensemble, i.e., many "individual measurements", but it must be well-defined ensemble, i.e., the preparation procedure must be describable correctly by the model to be able to define the ensemble given by individual realizations to be measured on. Each individual measurement is of course random in its outcome, but that's precisely what QT describes! It does even more, it also gives clear probability distributions (or probabilities in the discrete part of the spectra of the measured observable) for these outcomes.
Of course, Schwinger has the issue right (at least in the book compiled by Englert from his lecture notes: Quantum Mechanics, Symbolism for atomic measurements, Springer): QT is a causal probabilistic theory, which is describing the indeterminism of observable depending on the state the system is prepared in. In any state only a few independent observables have determined values, all others are indetermined and thus there's no definite outcome when properly measureing these observables (of course for those observables the state provides determined values you get a definite outcome of each individual measurement).