@MikeMiller It's more that they're invisible to
physical perturbation theory. That assumes a
small coupling $g$, and the instanton contributions are typically $\propto\exp\left(-\frac{1}{g}\right)$ in the "perturbative expansion" (cf.
nlab). Additionally, perturbative theory also expands around a classical vacuum solution, so seeing the influence of other vacuum solutions on the sector you are perturbatively investigating is...difficult