Table 2.
Field-of-view deformation.
Characteristic | Array 1 | Array 3 | Array 2 |
---|---|---|---|
λ [mm] | 1.15 | 1.15 | 2.0 |
Design detectors | 1140 | 1140 | 616 |
Selected KID (a) | 866 | 808 | 488 |
Well-placed KID (b) | 864 | 808 | 488 |
Deviation (c) [″] | 1.01 | 0.95 | 0.75 |
Distortion (d) [″] | 1.09 | 1.01 | 0.84 |
Array centre (e) [″] | (1.9, −5.1) | (2.3, −6.2) | (9.6, −7.8) |
Scaling (f) [″ mm−1] | 4.9 | 4.9 | 4.9 |
Rotation angle (g) [°] | 77.3 | 76.3 | 78.2 |
Grid step (h) [″, mm] | 9.8, 2.00 | 9.7, 2.00 | 13.3, 2.75 |
Grid step (i) [λ/D] | 1.11 | 1.10 | 0.87 |
Modelled grid step (j) [λ/D] | 1.09 | 1.09 | 0.93 |
Notes. Example of mapping of the observed KID positions in the sky to their mechanically designed positions. The initial table of selected KIDs is given by the focal plane geometry procedure, as described in Sect. 5.1, and applied to a beammap scan acquired during the N2R12 campaign. More than 90% of the detectors are within less than 5″ of their expected position.
Number of KIDs for which the best-fit sky position is less than 4″ away from the expected position.
Centre-to-centre distance between neighbour detectors using the reference frequencies (260 GHz and 150 GHz) and a 27-m entrance pupil diameter (see Sect. 2.2).
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