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Table 1

“Observational” parameters of the stellar targets and their exact values.

Name (L/L)obs (L/L)exact Δνobs Δνexact [Fe/H]obs [Fe/H]exact

Aardvark 5720 ± 85 5735 0.87 ± 0.03 0.89 149.6 ± 2.9 144.7 3503 ± 165 3372 0.02 ± 0.09 0.00
Blofeld 5808 ± 85 5921 2.02 ± 0.06 2.04 97.4 ± 1.9 94.3 1750 ± 100 2015 0.04 ± 0.09 0.09
Coco 5828 ± 85 5914 0.73 ± 0.02 0.73 160.9 ± 3.3 162.5 3634 ± 179 3587 −0.74 ± 0.09 −0.70
Diva 5893 ± 85 5932 2.14 ± 0.06 2.04 100.0 ± 1.9 96.0 2059 ± 101 2031 0.03 ± 0.09 0.16
Elvis 5900 ± 85 5822 1.22 ± 0.04 1.22 118.3 ± 2.4 120.2 2493 ± 127 2606 0.04 ± 0.09 0.00
Felix 6175 ± 85 6256 4.13 ± 0.12 4.07 70.0 ± 1.4 69.6 1290 ± 66 1337 0.06 ± 0.09 0.00
George 6253 ± 85 6406 4.31 ± 0.13 4.36 68.8 ± 1.4 70.5 1311 ± 67 1356 −0.03 ± 0.09 0.00
Henry 6350 ± 85 6400 1.94 ± 0.06 1.95 117.6 ± 2.3 116.7 2510 ± 124 2493 −0.35 ± 0.09 −0.36
Izzy 6431 ± 85 6390 2.01 ± 0.06 1.95 114.6 ± 2.3 116.1 2319 ± 124 2481 −0.34 ± 0.09 −0.25
Jam 6503 ± 85 6586 3.65 ± 0.11 3.65 86.4 ± 1.7 86.6 1758 ± 89 1785 0.09 ± 0.09 0.00

Notes. The exact large separations are a least-squares fit to all of the modes, using the “observational” error bars to decide the weights on each mode. The “exact” νmax values were obtained by applying the νmax scaling relation using the reference values given in Table 4.

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