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Table 1

Temperature, total extinction and luminosity values for the 11 objects in common with Kamath et al. (2022).

Object A(V)(1) (mag) A(V)(2) (mag) Teff(1) (K) Teff(2) (K) Log[L](1) Log[L](2)
HD 56126 2.0 1.33(*) 7250 ±125 7485 ± 250 3.940.05+0.04${3.94_{ - 0.05}^{ + 0.04}}$ 3.740.04+0.05${3.74_{ - 0.04}^{ + 0.05}}$
HD 107369 0.3 0.22 7500 ±125 7533 ± 250 2.990.06+0.06${2.99_{ - 0.06}^{ + 0.06}}$ 2.960.05+0.04${2.96_{ - 0.05}^{ + 0.04}}$
HD 133656 1.0 0.90 8250 ±125 8238 ± 250 3.740.04+0.04${3.74_{ - 0.04}^{ + 0.04}}$ 3.720.03+0.04${3.72_{ - 0.03}^{ + 0.04}}$
HD 148743 0.6 0.34 6750 ±125 6728 ± 250 4.510.08+0.07${4.51_{ - 0.08}^{ + 0.07}}$ 4.410.06+0.07${4.41_{ - 0.06}^{ + 0.07}}$
HD 161796 0.75 0.40 6000 ±125 6139 ± 250 3.880.05+0.04${3.88_{ - 0.05}^{ + 0.04}}$ 3.760.04+0.04${3.76_{ - 0.04}^{ + 0.04}}$
HD 187885 1.8 1.74 8000 ±125 8239 ± 250 3.890.21+0.14${3.89_{ - 0.21}^{ + 0.14}}$ 3.850.06+0.06${3.85_{ - 0.06}^{ + 0.06}}$
HD 235858 2.8 2.73 5250 ±125 5325 ± 250 3.940.04+0.03${3.94_{ - 0.04}^{ + 0.03}}$ 3.750.03+0.04${3.75_{ - 0.03}^{ + 0.04}}$
IRAS 01259+6823 3.0 3.20 5500 ±125 5510 ± 250 3.470.04+0.04${3.47_{ - 0.04}^{ + 0.04}}$ 2.530.19+0.28${2.53_{ - 0.19}^{ + 0.28}}$
IRAS 12360-5740 2.7 3.10 7500 ±125 7273 ± 250 3.880.11+0.08${3.88_{ - 0.11}^{ + 0.08}}$ 3.800.09+0.10${3.80_{ - 0.09}^{ + 0.10}}$
V* LN Hya 1.0 0.93 6250 ±125 6393 ± 250 4.020.04+0.04${4.02_{ - 0.04}^{ + 0.04}}$ 4.030.03+0.04${4.03_{ - 0.03}^{ + 0.04}}$
V* V1401 Aql 1.0 1.24 6750 ±125 6985 ± 250 3.470.02+0.02${3.47_{ - 0.02}^{ + 0.02}}$ 3.550.01+0.02${3.55_{ - 0.01}^{ + 0.02}}$

Notes. (*)Note the A(V) difference between both works, higher than 0.5 mag. Rao et al. (2012) did not find a C/O ratio greater than 1 nor s-process enrichment in HD 107369, as it is expected for an AGB star. In the present study, this star is classified as an unconfirmed post-AGB candidate. (1)Calculated by VOSA, (2)Kamath et al. (2022).

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