Shorter wavelength and larger aperture improve resolution.
With atmosphere on, “seeing” can dominate unless AO helps.
Model notesRayleigh + seeing
Diffraction-limited scaling:
$$\theta_\mathrm{diff} \approx 1.22\,\frac{\lambda}{D}$$
where $\lambda$ is wavelength and $D$ is effective aperture.
Atmosphere (toy model): without AO we take $\max(\theta_\mathrm{diff},\,\theta_\mathrm{seeing})$; with AO we reduce seeing and combine in quadrature.
Status cutoffs are didactic: resolved if separation $\ge \theta_\mathrm{eff}$, marginal if $\ge 0.8\,\theta_\mathrm{eff}$.
Visualization: diffraction uses an Airy PSF $I(x)=[2J_1(x)/x]^2$; with atmosphere on we use a blurred PSF for clarity (not a full turbulence simulation).