Table 3
DIBs for which the measured values of λ0 and/or FWHM are significantly different for LS III +46 11 and LS III +46 12 when compared with the reference values.
| λ0 | FWHM | ||
| (Å) | (Å) | ||
| Old | New | Old | New |
|
|
|||
| 4427.94 | 4428.42 | 24.15 | 17.30 |
| 4761.12 | 4765.0 | 19.72 | 22.00 |
| 4779.69 | 5.48 | 3.00 | |
| 4963.85 | 2.62 | 0.66 | |
| 4984.59 | 1.33 | 0.55 | |
| 5236.29 | 2.27 | 1.56 | |
| 5449.83 | 5451.1 | 14.06 | |
| 5487.23 | 6.63 | 4.78 | |
| 5494.29 | 1.90 | 0.71 | |
| 6010.75 | 6010.43 | 3.27 | |
| 6283.84 | 6284.36 | 4.77 | |
| 6590.42 | 6591.5 | 7.53 | 12.82 |
| 8621.20 | 8620.65 | 1.86 | 4.69 |
Notes. A single value indicates no apparent change. The number of significant digits in λ0 reflects the precision of the value, which is worse for weak/broad DIBs than for strong/narrow DIBs. The values listed here originate from both high- and intermediate-resolution spectroscopy (see Table 2) but the latter is not used for narrow DIBs to avoid resolution issues.
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