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Table 2

Measured (Col. 8) and calculated (Col. 7) effective temperature for well-known δ Scuti stars (see text).

N CID (%)a a νmax (μHz)b (K)b Teff(i) (K)b Teff (K)a References
1 1043 25 ± 3 70 ± 5 111 ± 4 7280 ± 180 7270 ± 180 7300 ± 200 Hareter et al. (2014)
2 123 38 ± 2 76–82 119 ± 8c 7320 ± 180 7310 ± 130 7510 ± 130 Chen et al. (2016)
3 8669 70 ± 7 55–90 135 ± 6 7400 ± 190 7250 ± 210 7000 ± 200 Barceló Forteza et al. (2017)
4 5685 26 45 173 ± 4 7600 ± 220 7600 ± 230 7700 ± 200d Escorza et al. (2016)
5 546 31 ± 3 15–35 179 ± 11 7630 ± 230 7660 ± 250 7660 ± 250 Barceló Forteza et al. (2017)
6 8170 50 ± 5 73.2 ± 0.6 216 ± 5c 7830 ± 250 7780 ± 260 7750 ± 250 Creevey et al. (2009)
7 7528 60 ± 10 45–70 284 ± 9 8200 ± 300 8100 ± 350 7600 ± 200 García Hernández et al. (2013)
8 7613 100 ± 14e 51 ± 2 370 ± 12 8300 ± 230 8400 ± 280 8000 ± 200 García Hernández et al. (2009)

Notes. (a) Those parameters have been taken from the literature. The authors are listed in the “Reference” column. (b) The frequency at maximum power (νmax), the mean effective temperature(), and the effective temperaturefor a given inclination (Teff(i)) have been calculated using Eqs. (4), (7), and (9), respectively (see text). (c) The frequencies and the amplitudes of the modes to calculate νmax of CID 123 and CID 8170 have been taken from Poretti et al. (2009) and Costa et al. (2007), respectively. (d) The effective temperature of CID 5685 have been taken from Poretti et al. (2005). (e) We obtained the rotation rate of CID 7613 studying the power spectrum of the star (see text).

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