Table 6
Comparison between different evaluations of the acoustic radius.
| Target | Δνrecalc. |
|
|
R ⋆ /R |
| (in μHz) | (in s) | (in s) | ||
|
|
||||
| Aardvark | 144.698 ± 0.009 | 3455.5 ± 0.2 | 3370.5 | 1.0006128 |
| Blofeld | 94.271 ± 0.008 | 5303.9 ± 0.5 | 5106.8 | 1.0000000 |
| Coco | 162.474 ± 0.013 | 3077.4 ± 0.2 | 2998.7 | 1.0007149 |
| Diva | 96.023 ± 0.009 | 5207.1 ± 0.5 | 5082.4 | 1.0007380 |
| Elvis | 120.231 ± 0.009 | 4158.6 ± 0.3 | 4045.3 | 1.0007033 |
| Felix | 69.559 ± 0.015 | 7188.2 ± 1.5 | 7014.1 | 1.0009181 |
| George | 70.466 ± 0.022 | 7095.6 ± 2.2 | 6930.2 | 1.0009409 |
| Henry | 116.698 ± 0.022 | 4284.6 ± 0.8 | 4199.0 | 1.0008149 |
| Izzy | 116.095 ± 0.022 | 4306.8 ± 0.8 | 4219.4 | 1.0007725 |
| Jam | 86.605 ± 0.034 | 5773.3 ± 2.2 | 5666.2 | 1.0008475 |
Notes. The smallest difference between τTot. and is 78.6 s for Coco, whereas the largest difference is 197.1 s for Blofeld. The last column gives R⋆, the upper integration bound used when calculating τTot.. This radius corresponded an optical depth of τopt. = 10-3 (the last mesh point in the stellar targets), except for Blofeld where the atmosphere was truncated at the photospheric radius.
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