Image Details
Caption: Figure 2.
Differential intensity response, R 4 − R 3, of a double Bracewell nuller in the case of an ideal (left) and a perturbed (right) instrument at 10 μm at a given instant in time. The impact of the perturbations is highly exaggerated (rms(δA k ) = 10%, rms(δϕ k ) ≈ 0.28 rad, rms(δθ k ) = 0.4 rad) here for illustrative purposes. The dashed line corresponds to the path that a planet traces out as the interferometer array rotates around its line of sight to the star.
© 2025. The Author(s). Published by the American Astronomical Society.