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Table 1.

Frequencies of the low-radial-order (k), low-degree (ℓ = 1, 2) g-modes computed for the optimal seismic model of KIC 08626021 derived by Giammichele et al. (2018), which does not include neutrino cooling (ν0), and for the equivalent model including this effect (ν2).

k ν0 (μHz) ν2 (μHz) ν0 − ν2 (μHz)
1 1 8068.0321 8110.3577 −42.3256
1 2 6067.6415 6034.7152 +32.9263
1 3 * 5073.2341 5007.8906 +65.3435
1 4 * 4309.9149 4269.5782 +40.3367
1 5 * 3681.8029 3656.3533 +25.4496
1 6 * 3294.3693 3246.8780 +47.4913
1 7 2971.7185 2935.9436 +35.7749
1 8 2616.2037 2599.0472 +17.1565
1 9 2420.5893 2380.5206 +40.0687
1 10 2221.6371 2194.8451 +26.7920

2 2 9825.0553 9842.7756 −17.7203
2 3 8088.3782 8063.0609 +25.3173
2 4 * 6981.2613 6909.0377 +72.2236
2 5 6110.7566 6081.0542 +29.7024
2 6 5399.5510 5370.1025 +29.4485
2 7 4859.1436 4774.7813 +84.3623
2 8 * 4398.3723 4371.7608 +26.6115
2 9 3994.3952 3965.6973 +28.6979
2 10 * 3677.9937 3604.7042 +73.2895
2 11 3406.5703 3386.6587 +19.9116
2 12 3138.9597 3114.3881 +24.5716
2 13 2967.7865 2913.2948 +54.4917
2 14 2808.2635 2789.5232 +18.7403
2 15 * 2658.7774 2649.2922 +9.4852
2 16 2531.8834 2489.6276 +42.2558
2 17 2424.0703 2391.7391 +32.3312
2 18 2266.5570 2254.9941 +11.5629
2 19 2166.4153 2127.2743 +39.1410
2 20 2083.2448 2056.7203 +26.5245

Notes. The modes marked by an asterisk are those fitted to the observed frequencies that closely match ν0. The last column lists the frequency differences for each mode, between the two models.

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