19:37:00.50 62:16:14.20 · Culpan hotsd
outside the grid χ²/N = 0.98
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] | 57534 ± 921 |
| log g | 6.401 ± 0.109 |
| log n(He)/n(H) | -1.300 ± 0.106 |
| reduced χ² | 0.984 over 744 points |
| radial velocity | 26.0 km s−1 |
| resolution (FWHM) | 2.00 Å |
| lines fitted | 15 |
| grids | HE-0.041.fits HE-0.125.fits HE-0.300.fits HE-0.550.fits +9 more |
| settled | outside the grid |
| fitted | 04/09/2026 19:10:23 |
| telescope | SDSS 2.5-M |
| survey / programme | MWM / mwm_cb |
| field · MJD | 101807 · 59886 |
| date | 2022-11-03 |
| catalogid | 27021597842073713 |
| exposure | 2700 s in 3 |
| airmass | 1.98 |
| seeing (50%) | 1.44″ |
| E(B−V) | 0.059 |
| pipeline | v6_2_1 |
| cosmic rays | 6 pixels cancelled |
| S/N (classifier) | 39.1 |
| source file | spec-101807-59886-27021597842073713.fits |
| Gaia DR3 source | 2240950009039260160 |
| parallax [mas] | 0.5494 ± 0.0403 |
| G | 15.388 |
| BP − RP | -0.507 |
| Gabs | 4.087 |
| μα [mas/yr] | -7.144 |
| μδ [mas/yr] | 3.010 |
| RUWE | 1.071 |
| l, b | 94.132, 18.773 |
| selection | f_plx |
NEW
auto: He II/He I 7.5, EW 1.12; CONTINUUM WAVY (0.025, typical 0.008) -- Balmer jump and continuum shape unreliable
| line | λ [Å] | shift [Å] | continuum at | ±avg | fitted over |
| Hβ | 4861.32 | 0.42 | -40.0, 40.0 | 5.0 | -45.0, 45.0 |
| Hγ | 4340.46 | 0.38 | -40.0, 36.8 | 4.5 | -43.0, 43.0 |
| Hδ | 4101.73 | 0.36 | -40.0, 31.6 | 4.2 | -43.0, 43.0 |
| Hε | 3970.07 | 0.34 | -28.0, 30.0 | 4.1 | -30.0, 35.0 |
| Hζ | 3889.05 | 0.34 | -20.0, 26.2 | 4.0 | -31.8, 32.0 |
| Hη | 3835.38 | 0.33 | -20.0, 14.6 | 4.0 | -20.7, 21.8 |
| Hθ | 3797.90 | 0.33 | -16.0, 16.0 | 3.9 | -15.6, 16.7 |
| Hι | 3770.63 | 0.33 | -13.0, 13.0 | 3.9 | -11.7, 11.6 |
| He II 4686 | 4685.70 | 0.41 | -11.9, 11.9 | 4.9 | -15.0, 13.8 |
| He II 5412 | 5411.52 | 0.47 | -15.0, 15.0 | 5.6 | -15.0, 15.0 |
| He II 4542 | 4541.59 | 0.39 | -15.0, 20.0 | 4.7 | -20.0, 20.0 |
| He II 4200 | 4199.84 | 0.36 | -23.5, 33.8 | 4.3 | -20.0, 20.0 |
| He I 4472 | 4471.60 | 0.39 | -15.0, 15.0 | 4.6 | -15.0, 15.0 |
| He I 4026 | 4026.29 | 0.35 | -24.2, 15.0 | 4.2 | -15.0, 15.0 |
| He I 4922 | 4921.93 | 0.43 | -15.0, 15.0 | 5.1 | -15.0, 15.0 |