Meredith L. Rawls edited begin_deluxetable_lcccc_tablecolumns_5__.tex  over 8 years ago

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\tablecaption{Oscillation modes in KIC 9246715 fit with \textsc{D\large{iamonds}}.}  \centering  \tablehead{  \colhead{Frequency} & \colhead{$(\ell, m)$} & \colhead{Amplitude or Height\tablenotemark{a}} & \colhead{Linewidth} & \colhead{Significance} \colhead{Detection Probability\tablenotemark{b}}  \\ \colhead{($\mu \rm{Hz}$)} & \colhead{} & \colhead{(ppm) or (ppm$^2 \ \mu \rm{Hz}^{-1}$)} & \colhead{($\mu \rm{Hz}$)} & \colhead{}  }  \startdata  $76.50 \pm 0.01$ & (0, 0) & $5.2 \pm 0.4$ & $0.61 \pm 0.05$ & 0.914 0.91  \\ $84.43 \pm 0.02$ & (0, 0) & $10.9 \pm 0.4$ & $0.60 \pm 0.05$ & 1.000 1.00  \\ $86.01 \pm 0.01$ & (3, 0) & $3.1 \pm 0.1$ & $0.27 \pm 0.02$ & 0.680 0.68  \\ $87.714 \pm 0.001$ & (1, ?) & $402\substack{+11 \\ -12}$ & \nodata & 0.970 0.97  \\ $88.40 \pm 0.01$ & (1, -1) & $1.6 \pm 0.1$ & $0.088 \pm 0.006$ & 0.751 0.75  \\ $88.70 \pm 0.01$ & (1, 1) & $5.0 \pm 0.2$ & $0.26 \pm 0.02$ & 0.998 0.99  \\ $89.19 \pm 0.01$ & (1, -1) & $1.7 \pm 0.1$ & $0.17 \pm 0.01$ & 0.575 0.585  \\ $89.422 \pm 0.001$ & (1, 1) & $461\substack{+11 \\ -12}$ & \nodata & 0.994 0.99  \\ $91.84 \pm 0.01$ & (2, 0) & $1.7 \pm 0.1$ & $0.25 \pm 0.02$ & 0.634 0.63  \\ $92.54 \pm 0.01$ & (0, 0) & $13.2 \pm 0.3$ & $0.36 \pm 0.02$ & 1.000 1.00  \\ $96.12 \pm 0.01$ & (1, 1) & $2.8 \pm 0.5$ & $0.10 \pm 0.01$ & 0.896 0.90  \\ $96.62 \pm 0.02$ & (1, -1) & $7.6 \pm 1.0$ & $0.35 \pm 0.06$ & 0.563 0.56  \\ $97.00 \pm 0.03$ & (1, 1) & $7.9 \pm 1.0$ & $0.34 \pm 0.05$ & 0.802 0.80  \\ $99.63 \pm 0.04$ & (2, 0) & $11.1 \pm 1.0$ & $0.82 \pm 0.11$ & 1.000 1.00  \\ $100.75 \pm 0.02$ & (0, 0) & $15.7 \pm 0.6$ & $0.60 \pm 0.07$ & 1.000 1.00  \\ $103.26 \pm 0.01$ & (1, -1) & $3.7 \pm 0.2$ & $0.23 \pm 0.02$ & 0.185 0.19  \\ $103.66 \pm 0.01$ & (1, 1) & $6.3 \pm 0.4$ & $0.33 \pm 0.03$ & 0.095 0.10  \\ $104.67 \pm 0.01$ & (1, -1) & $6.1 \pm 0.3$ & $0.17 \pm 0.01$ & 1.000 1.00  \\ $105.04 \pm 0.01$ & (1, 1) & $8.7 \pm 0.4$ & $0.18 \pm 0.02$ & 1.000 1.00  \\ $105.50 \pm 0.01$ & (1, -1) & $5.9 \pm 0.3$ & $0.14 \pm 0.01$ & 0.993 0.99  \\ $105.89 \pm 0.01$ & (1, 1) & $8.4 \pm 0.5$ & $0.33 \pm 0.03$ & 1.000 1.00  \\ $108.24 \pm 0.02$ & (2, 0) & $11.6 \pm 1.2$ & $0.78 \pm 0.11$ & 1.000 1.00  \\ $109.06 \pm 0.01$ & (0, 0) & $14.6 \pm 0.4$ & $0.46 \pm 0.03$ & 1.000 1.00  \\ $111.940 \pm 0.001$ & (1, -1) & $435\substack{+16 \\ -33}$ & \nodata & 0.999 0.99  \\ $112.28 \pm 0.01$ & (1, 1) & $3.5 \pm 0.3$ & $0.19 \pm 0.02$ & 0.785 0.79  \\ $113.13 \pm 0.01$ & (1, -1) & $7.7 \pm 0.4$ & $0.14 \pm 0.01$ & 1.000 1.00  \\ $113.39 \pm 0.01$ & (1, 1) & $12.3 \pm 0.5$ & $0.25 \pm 0.02$ & 1.000 1.00  \\ $114.74 \pm 0.01$ & (1, ?) & $2.9 \pm 0.2$ & $0.01 \pm 0.01$ & 0.926 0.93  \\ $116.54 \pm 0.01$ & (2, 0) & $13.3 \pm 0.5$ & $1.00 \pm 0.08$ & 1.000 1.00  \\ $117.37 \pm 0.01$ & (0, 0) & $12.6 \pm 0.4$ & $0.30 \pm 0.02$ & 1.000 1.00  \\ $120.59 \pm 0.03$ & (1, 1) & $5.4 \pm 0.7$ & $0.39 \pm 0.10$ & 0.997 0.99  \\ $121.60 \pm 0.01$ & (1, -1) & $6.8 \pm 0.6$ & $0.12 \pm 0.02$ & 0.999 0.99  \\ $121.88 \pm 0.02$ & (1, 1) & $9.6 \pm 0.6$ & $0.28 \pm 0.04$ & 1.000 1.00  \\ $122.74 \pm 0.02$ & (1, -1) & $4.3 \pm 0.4$ & $0.16 \pm 0.03$ & 0.999 0.99  \\ $123.101 \pm 0.003$ & (1, 1) & $347\substack{+36 \\ -29}$ & \nodata & 1.000 1.00  \\ $125.06 \pm 0.03$ & (2, 0) & $10.8 \pm 0.8$ & $0.84 \pm 0.15$ & 1.000 1.00  \\ $125.92 \pm 0.04$ & (0, 0) & $9.8 \pm 0.7$ & $0.48 \pm 0.07$ & 1.000 1.00  \\ $128.53 \pm 0.01$ & (1, ?) & $3.2 \pm 0.3$ & $0.10 \pm 0.01$ & 0.981 0.98  \\ $129.23 \pm 0.01$ & (1, -1) & $3.7 \pm 0.4$ & $0.11 \pm 0.01$ & 0.976 0.98  \\ $129.52 \pm 0.02$ & (1, 1) & $1.3 \pm 0.1$ & $0.07 \pm 0.01$ & 0.621 0.62  \\ $129.95 \pm 0.02$ & (1, -1) & $6.0 \pm 0.3$ & $0.32 \pm 0.05$ & 0.557 0.56  \\ $130.20 \pm 0.01$ & (1, 1) & $4.8 \pm 0.3$ & $0.16 \pm 0.02$ & 0.146 0.15  \\ $130.47 \pm 0.02$ & (1, -1) & $3.9 \pm 0.3$ & $0.19 \pm 0.03$ & 0.721 0.72  \\ $130.74 \pm 0.02$ & (1, 1) & $6.1 \pm 0.5$ & $0.29 \pm 0.05$ & 0.998 0.99  \\ $131.14 \pm 0.02$ & (1, -1) & $1.7 \pm 0.1$ & $0.08 \pm 0.01$ & 0.134 0.13  \\ $133.35 \pm 0.02$ & (2, 0) & $9.3 \pm 0.6$ & $0.85 \pm 0.09$ & 1.000 1.00  \\ $134.53 \pm 0.02$ & (0, 0) & $9.1 \pm 0.7$ & $0.91 \pm 0.07$ & 1.000 1.00  \\ $137.30 \pm 0.03$ & (1, -1) & $5.0 \pm 0.7$ & $0.41 \pm 0.13$ & 0.971 0.97  \\ $137.74 \pm 0.07$ & (1, 1) & $3.3 \pm 0.8$ & $0.53 \pm 0.18$ & 0.313 0.31  \\ $138.65 \pm 0.04$ & (1, -1) & $7.7 \pm 0.9$ & $1.10 \pm 0.26$ & 1.000 1.00  \\ $139.06 \pm 0.02$ & (1, 1) & $4.2 \pm 0.5$ & $0.13 \pm 0.03$ & 0.999 0.99  \enddata  \label{appendixtable}  \tablenotetext{a}{An amplitude is measured when the peak is a resolved Lorentzian, while height is measured instead when the peak is an unresolved Sinc$^2$ function. Linewidth is not defined in the latter case.}  \tablenotetext{b}{Values of 0.99 and above are ensured to be significant.}  \end{deluxetable}