SDSSJ061401.59+332927.6 · Culpan knownhsd
χ²/N = 0.99
The whole reduced spectrum above, the region marked on it below. Shaded bands are the intervals the fit used; a tick under the axis marks a pixel the rejection mask cancelled.

| Teff [K] | 50226 ± 2246 |
| log g | 5.681 ± 0.120 |
| log n(He)/n(H) | -3.279 ± 0.209 |
| reduced χ² | 0.988 over 745 points |
| radial velocity | -129.0 km s−1 |
| resolution (FWHM) | 2.50 Å |
| lines fitted | 15 |
| grids | HE-0.041.fits HE-0.125.fits HE-0.300.fits HE-0.550.fits +9 more |
| fitted | 04/09/2026 18:27:23 |
| Teff [K] | 52700 ± 2130 |
| log g | 5.300 ± 0.150 |
| log n(He)/n(H) | -3.320 ± 0.340 |
| grids | Lei et al. 2019, ApJ 881, 135 SYNSPEC 49 spectra from NLTE TLUSTY 204 model atmospheres, through XTgrid |
| cosmic rays | 16 pixels cancelled |
| source file | spec-56630-GAC091N33M1_sp06-026.fits.gz |
| Gaia DR3 source | 3440046359151100032 |
| parallax [mas] | 0.5076 ± 0.0701 |
| G | 16.666 |
| Gabs | 5.296 |
| μα [mas/yr] | 2.188 |
| μδ [mas/yr] | -1.629 |
| l, b | 179.035, 7.527 |
| class (Culpan) | sdO |
| class (SIMBAD) | sd |
| Teff [K] | 52700 ± 2130 |
| log g | 5.30 ± 0.15 |
| log y | -3.32 ± 0.34 |
| reference | 2019ApJ...881..135L |
| line | λ [Å] | shift [Å] | continuum at | ±avg | fitted over |
| Hβ | 4861.32 | -2.09 | -40.0, 40.0 | 5.0 | -45.0, 45.0 |
| Hγ | 4340.46 | -1.87 | -40.0, 36.8 | 4.5 | -43.0, 43.0 |
| Hδ | 4101.73 | -1.76 | -40.0, 31.6 | 4.2 | -43.0, 43.0 |
| Hε | 3970.07 | -1.71 | -28.0, 30.0 | 4.1 | -30.0, 35.0 |
| Hζ | 3889.05 | -1.67 | -20.0, 26.2 | 4.0 | -31.8, 32.0 |
| Hη | 3835.38 | -1.65 | -20.0, 14.6 | 4.0 | -20.7, 21.8 |
| Hθ | 3797.90 | -1.63 | -16.0, 16.0 | 3.9 | -15.6, 16.7 |
| Hι | 3770.63 | -1.62 | -13.0, 13.0 | 3.9 | -11.7, 11.6 |
| He II 4686 | 4685.70 | -2.02 | -11.9, 11.9 | 4.9 | -15.0, 13.8 |
| He II 5412 | 5411.52 | -2.33 | -15.0, 15.0 | 5.6 | -15.0, 15.0 |
| He II 4542 | 4541.59 | -1.95 | -15.0, 20.0 | 4.7 | -20.0, 20.0 |
| He II 4200 | 4199.84 | -1.81 | -23.5, 33.8 | 4.3 | -20.0, 20.0 |
| He I 4472 | 4471.60 | -1.92 | -15.0, 15.0 | 4.6 | -15.0, 15.0 |
| He I 4026 | 4026.29 | -1.73 | -24.2, 15.0 | 4.2 | -15.0, 15.0 |
| He I 4922 | 4921.93 | -2.12 | -15.0, 15.0 | 5.1 | -15.0, 15.0 |