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Table D.1

Results of spectral fitting to X-ray selected STONKS alert sources. We list here the STONKS alert class and parameters derived from fitting the X-ray spectra to X-ray sources.

No. Alert OBSID Model NH kT kT2 kT3 Abund α dof χν2$\chi_{\nu}^{2}$ N C-stat
1 FD 0886010101 bbody 68.38-+217.29$68.38_{-\infty}^{+217.29}$ 1.22-0.93+6.99$1.22_{-0.93}^{+6.99}$ 7 1.29
powerlaw 84.38-+119.10$84.38_{-\infty}^{+119.10}$ 3.86-6.46+$3.86_{-6.46}^{+\infty}$ 7 1.30
apec 39.50-20.35+34.30$39.50_{-20.35}^{+34.30}$ 57.59-51.86+$57.59_{-51.86}^{+\infty}$ 1.0 7 1.40
bremss 78.16-56.16+223.95$78.16_{-56.16}^{+223.95}$ 2.81-+$2.81_{-\infty}^{+\infty}$ 7 1.30
bremss + gauss 0.77-0.77+8.27$0.77_{-0.77}^{+8.27}$ 22.79-22.73+$22.79_{-22.73}^{+\infty}$ 6.7 5 0.86
2 FD 0886010401 bbody 1.19-1.03+2.39$1.19_{-1.03}^{+2.39}$ 1.66-0.58+1.03$1.66_{-0.58}^{+1.03}$ 10 0.76
powerlaw 2.75-2.10+4.67$2.75_{-2.10}^{+4.67}$ 1.08-1.11+1.70$1.08_{-1.11}^{+1.70}$ 10 0.72
apec 4.12+3.53 7.80-5.58+$7.80_{-5.58}^{+\infty}$ 1.0 10 0.51
bremss 3.05-0.96+1.42$3.05_{-0.96}^{+1.42}$ 199.36-+$199.36_{-\infty}^{+\infty}$ 10 0.72
3 FD 0886010401 bbody 1.40-+2.80$1.40_{-\infty}^{+2.80}$ 1.70-0.72+2.31$1.70_{-0.72}^{+2.31}$ 9 1.80
powerlaw 3.14-2.26+3.83$3.14_{-2.26}^{+3.83}$ 1.38-1.33+1.80$1.38_{-1.33}^{+1.80}$ 9 1.62
apec 2.98-1.17+2.57$2.98_{-1.17}^{+2.57}$ 63.93-+$63.93_{-\infty}^{+\infty}$ 1.0 9 1.63
bremss 2.95-1.22+2.92$2.95_{-1.22}^{+2.92}$ 95.24-+$95.24_{-\infty}^{+\infty}$ 9 1.63

Notes. The Model column indicates the model which has been combined with ISM absorption (tbabs*) to provide the spectral fit. The NH column gives the neutral hydrogen column density in units of × 102 2 cm−2. The kT (also kT2 and kT3), Abundance, and α columns indicate the characteristic temperature(s) in units of keV, solar abundance as fixed for model fitting, or power law index derived from the spectral fit as required. The final four columns indicate the quality of the fit. They either give the give the number of degrees of freedom and the reduced chi-squared value, or the number of photons and the Cash stat value. Where the errors on physical parameters cannot be bound by fitting this is indicated as ∞. The full Table is available at the CDS.

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