17:28:39.70 15:46:10.34 · Culpan hotsd
outside the grid χ²/N = 0.96
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] | 55069 ± 1858 |
| log g | 6.287 ± 0.149 |
| log n(He)/n(H) | 0.375 ± 0.159 |
| reduced χ² | 0.963 over 749 points |
| radial velocity | 73.0 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 19:09:59 |
| telescope | SDSS 2.5-M |
| survey / programme | MWM / mwm_cb |
| field · MJD | 100100 · 60418 |
| date | 2024-04-18 |
| catalogid | 63050395763428017 |
| exposure | 900 s in 1 |
| airmass | 1.05 |
| seeing (50%) | 1.28″ |
| E(B−V) | 0.091 |
| pipeline | v6_2_1 |
| cosmic rays | 3 pixels cancelled |
| S/N (classifier) | 28.4 |
| source file | spec-100100-60418-63050395763428017.fits |
| Gaia DR3 source | 4543793310014586368 |
| parallax [mas] | 0.3703 ± 0.0404 |
| G | 15.590 |
| BP − RP | -0.352 |
| Gabs | 3.433 |
| μα [mas/yr] | 5.170 |
| μδ [mas/yr] | -10.603 |
| RUWE | 1.040 |
| l, b | 38.439, 25.251 |
| selection | f_plx |
NEW
auto: He II/He I 3.0, EW 1.73, Mg I b suggests a companion but Ca II does not (-2.7 sigma)
| line | λ [Å] | shift [Å] | continuum at | ±avg | fitted over |
| Hβ | 4861.32 | 1.18 | -40.0, 40.0 | 5.0 | -45.0, 45.0 |
| Hγ | 4340.46 | 1.06 | -40.0, 36.8 | 4.5 | -43.0, 43.0 |
| Hδ | 4101.73 | 1.00 | -40.0, 31.6 | 4.2 | -43.0, 43.0 |
| Hε | 3970.07 | 0.97 | -28.0, 30.0 | 4.1 | -30.0, 35.0 |
| Hζ | 3889.05 | 0.95 | -20.0, 26.2 | 4.0 | -31.8, 32.0 |
| Hη | 3835.38 | 0.93 | -20.0, 14.6 | 4.0 | -20.7, 21.8 |
| Hθ | 3797.90 | 0.92 | -16.0, 16.0 | 3.9 | -15.6, 16.7 |
| Hι | 3770.63 | 0.92 | -13.0, 13.0 | 3.9 | -11.7, 11.6 |
| He II 4686 | 4685.70 | 1.14 | -11.9, 11.9 | 4.9 | -15.0, 13.8 |
| He II 5412 | 5411.52 | 1.32 | -15.0, 15.0 | 5.6 | -15.0, 15.0 |
| He II 4542 | 4541.59 | 1.11 | -15.0, 20.0 | 4.7 | -20.0, 20.0 |
| He II 4200 | 4199.84 | 1.02 | -23.5, 33.8 | 4.3 | -20.0, 20.0 |
| He I 4472 | 4471.60 | 1.09 | -15.0, 15.0 | 4.6 | -15.0, 15.0 |
| He I 4026 | 4026.29 | 0.98 | -24.2, 15.0 | 4.2 | -15.0, 15.0 |
| He I 4922 | 4921.93 | 1.20 | -15.0, 15.0 | 5.1 | -15.0, 15.0 |