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Table 3

Results of the mode identification from spectroscopic and Strömgren observations, as well as the values of n and obtained in the model fitting (last two columns).

Spectroscopy Strömgren photometry CoRoT photometry Model fit
Freq. (d-1μHz) Ampl. S/N (± 1) m(± 1) Freq. (d-1) Freq. (d-1) Ampl. (mmag) n

6.801−78.72 0.033 6.5 15 −15
18.131−209.85 0.023 3.8 3 1 F8 = 18.135 0.231 3 −2
21.427−248.00 0.031 4.6 1 1 21.421 2, 3, 1&3 F3 = 21.420 2.093
23.152−267.96 0.044 8.2 1 −1 2 0
23.192−268.43 0.056 13.0 1 −1 23.195 0, 1 F1 = 23.195 6.290 0 2
24.122−279.19 0.028 5.3 1 −1 1 1
25.023−289.62 0.035 7.0 7 5
26.025−301.22 0.042 11.0 8 8 F171 = 26.026 0.0090
26.955−311.98 0.041 7.9 2 1 26.956 0, 1, 2 F2 = 26.958 5.103 2 1
26.982−312.29 0.033 7.7 7 3 F46 = 26.962 0.0312
27.535−318.69 0.028 6.4 8 4 F172 = 27.543 0.0088
27.709−320.71 0.042 10.7 3 3 F4 = 27.715 0.997
27.720−320.83 0.048 11.3 2 2 F4 = 27.715 0.997
30.093−348.30 0.027 4.9 2 2 F67 = 30.101 0.0221
30.954−358.26 0.028 5.6 7 5 F17 = 30.950 0.116
31.171−360.78 0.044 8.9 10 6 F61 = 31.178 0.023
32.026−370.67 0.032 7.7 10 5
32.561−376.86 0.041 7.9 11 9

Notes. The spectroscopic amplitudes are in continuum units as defined by Zima (2006). Columns 8 and 9 show the corresponding CoRoT photometric frequencies. Spectroscopic frequencies 27.709 and 27.720 d-1 are uncertain.

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