LAMOSTJ181632.50+345549.2 · Culpan knownhsd
χ²/N = 1.00
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] | 48339 ± 690 |
| log g | 5.809 ± 0.047 |
| log n(He)/n(H) | -2.859 ± 0.050 |
| reduced χ² | 1.000 over 745 points |
| radial velocity | -121.0 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 18:32:53 |
| Teff [K] | 47780 ± 1720 |
| log g | 5.480 ± 0.030 |
| log n(He)/n(H) | -2.920 ± 0.110 |
| grids | Lei et al. 2020, ApJ 889, 117 SYNSPEC 49 spectra from NLTE TLUSTY 204 model atmospheres, through XTgrid |
| cosmic rays | 13 pixels cancelled |
| source file | spec-58612-GACII274N33M1_sp15-206.fits.gz |
| Gaia DR3 source | 4605575383775753856 |
| parallax [mas] | 0.4936 ± 0.0441 |
| G | 16.002 |
| Gabs | 4.448 |
| μα [mas/yr] | -8.155 |
| μδ [mas/yr] | -5.993 |
| l, b | 62.131, 21.824 |
| class (Culpan) | sdO |
| Teff [K] | 50712 ± 424 |
| log g | 6.05 ± 0.03 |
| log y | -2.79 ± 0.11 |
| reference | 2021ApJS..256...28L |
| line | λ [Å] | shift [Å] | continuum at | ±avg | fitted over |
| Hβ | 4861.32 | -1.96 | -40.0, 40.0 | 5.0 | -45.0, 45.0 |
| Hγ | 4340.46 | -1.75 | -40.0, 36.8 | 4.5 | -43.0, 43.0 |
| Hδ | 4101.73 | -1.66 | -40.0, 31.6 | 4.2 | -43.0, 43.0 |
| Hε | 3970.07 | -1.60 | -28.0, 30.0 | 4.1 | -30.0, 35.0 |
| Hζ | 3889.05 | -1.57 | -20.0, 26.2 | 4.0 | -31.8, 32.0 |
| Hη | 3835.38 | -1.55 | -20.0, 14.6 | 4.0 | -20.7, 21.8 |
| Hθ | 3797.90 | -1.53 | -16.0, 16.0 | 3.9 | -15.6, 16.7 |
| Hι | 3770.63 | -1.52 | -13.0, 13.0 | 3.9 | -11.7, 11.6 |
| He II 4686 | 4685.70 | -1.89 | -11.9, 11.9 | 4.9 | -15.0, 13.8 |
| He II 5412 | 5411.52 | -2.18 | -15.0, 15.0 | 5.6 | -15.0, 15.0 |
| He II 4542 | 4541.59 | -1.83 | -15.0, 20.0 | 4.7 | -20.0, 20.0 |
| He II 4200 | 4199.84 | -1.70 | -23.5, 33.8 | 4.3 | -20.0, 20.0 |
| He I 4472 | 4471.60 | -1.80 | -15.0, 15.0 | 4.6 | -15.0, 15.0 |
| He I 4026 | 4026.29 | -1.63 | -24.2, 15.0 | 4.2 | -15.0, 15.0 |
| He I 4922 | 4921.93 | -1.99 | -15.0, 15.0 | 5.1 | -15.0, 15.0 |