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Table 2.

Key features of the visibility amplitudes of the various models considered at νobs=230 GHz.

Model 40 Gλ 100 Gλ n = 1 n = 2
a = 0.01 circular thin 9.2 mJy 2.4 mJy (150 Gλ, 1 mJy) (1400 Gλ, 25 μJy)

10 mJy 2.7 mJy (140 Gλ, 2 mJy) (1300 Gλ, 20 μJy)

a = 0.01 radial thin 14.4 mJy 2.2 mJy (54 Gλ, 10 mJy) (800 Gλ, 10 μJy)

12 mJy 3.3 mJy (65 Gλ, 7.5 mJy) (900 Gλ, 5.6 μJy)

a = 0.01 circular thick 8.6 mJy 2.4 mJy (54 Gλ, 6.8 mJy) (650 Gλ, 55 μJy)

7.7 mJy 2.8 mJy (44 Gλ, 7.7 mJy) (650 Gλ, 43.2 μJy)

a = 0.01 radial thick 12.2 mJy 2.2 mJy (35 Gλ, 14.4 mJy) (660 Gλ, 23 μJy)

11.2 mJy 2.1 mJy (34 Gλ, 12.8 mJy) (660 Gλ, 14.9 μJy)

a = 0.94 circular thin   12.0 mJy   2.0 mJy (112 Gλ, 1.8 mJy) (700 Gλ, 57 μJy)

11.2 mJy 1.8 mJy (N/A, N/A) (N/A, N/A)

a = 0.94 radial thin 10.4 mJy 1.3 mJy (44.2 Gλ, 9.7 mJy) (896 Gλ, 0.25 μJy)

7.1 mJy 1.4 mJy (54 Gλ, 5.5 mJy) (N/A, N/A)

a = 0.94 circular thick 10.7 mJy 1.8 mJy (54 Gλ, 6 mJy) (328 Gλ, 180 μJy)

7.3 mJy 0.7 mJy (63.8 Gλ, 3.5 mJy) (N/A, N/A)

a = 0.94 radial thick 7.4 mJy 0.6 mJy (34.4 Gλ, 10.0 mJy) (847 Gλ, 0.01 μJy)

6.2 mJy 0.5 mJy (34.4 Gλ, 7.3 mJy) (N/A, N/A)

Notes. For each model, we list the visibility amplitude |V(u,φ)| at u = 40 Gλ and 100 Gλ, as well as the baseline thresholds b1(φ) and b2(φ) (and the corresponding visibility amplitudes) past which the n = 1 and n = 2 contributions start to dominate the signal (Eq. (15)). For each model, two lines are provided, corresponding to a baseline polar angle φ = 90° (aligned with spin, upper line) or φ = 0° (perpendicular to spin, lower line). The percent level p of Eq. (15) is 5% everywhere, except for the numbers in red, where it is set to 10% (in these cases, the ring never dominates according to the 5% criterion). The “N/A” in the n = 2 column for the high-spin cases at φ = 0° mean that the n = 2 signal never dominates even for p = 10%.

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