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Table 2.

Atmosphere parameters and best-fit Li and Ca pseudo-dynamical abundances for the sample of massive AGB stars.

IRAS name Teff (K) log g β (M yr−1) νexp(OH) (km s−1) log ε(Li)static log ε(Li)dyn log ε(Ca)static log ε(Ca)dyn
01085+3022* 3300 −0.5 0.2 1.0 × 10−7 13 2.4 2.2
02095−2355 3300** −0.5 0.8 1.0 × 10−9 12 1.6 1.6 6.3 6.3
05027−2158 2800 −0.5 0.4 1.0 × 10−7 8 1.1 1.1 5.8 5.8
05098−6422 3000 −0.5 1.4 1.0 × 10−8 6 ≤−1.0 ≤0.0 6.1 6.1
05151+6312 3000 −0.5 1.0 1.0 × 10−8 15 ≤0.0 ≤0.2 6.0 6.0
05559+3825 2900 −0.5 1.6 1.0 × 10−7 12 0.6 0.5 5.8 5.8
06300+6058 3000 −0.5 0.2 1.0 × 10−7 12 0.7 0.8 ≤5.8 ≤5.8
07304−2032 2700 −0.5 0.4 1.0 × 10−7 7 0.9 1.0 ≤5.8 ≤5.8
09429−2148 3300** −0.5 1.6 1.0 × 10−8 12 2.2 2.2 5.3 5.3
10261−5055 3000 −0.5 0.2 1.0 × 10−9 4 ≤−1.0 ≤0.0 5.8 5.8
11081−4203 3000 −0.5 1.6 5.0 × 10−8 8 1.3 1.1 5.8 5.8
14266−4211 2900 −0.5 0.2 5.0 × 10−8 9 ≤0.0 0.2 ≤5.3 ≤5.3
14337−6215* 3300 −0.5 0.2 5.0 × 10−8 20 2.41 2.41
15193+3132 2800 −0.5 1.6 1.0 × 10−9 3 ≤0.0 ≤0.0 ≤5.8 ≤5.8
15211−4254 3300** −0.5 1.6 1.0 × 10−9 11 2.3 2.3 5.8 5.8
15255+1944 2900 −0.5 0.2 5.0 × 10−7 7 1.0 0.9 6.0 6.0
15576−1212 3000 −0.5 0.2 1.0 × 10−8 10 1.1 1.2 5.7 5.7
16030−5156* 3000 −0.5 0.2 1.0 × 10−8 10 1.5 1.5
16037+4218 2900 −0.5 1.2 1.0 × 10−8 4 ≤−1.0 ≤0.0 6.3 6.3
16260+3454 3300** −0.5 0.2 1.0 × 10−9 12 2.7 2.6 5.4 5.4
17034−1024 3300** −0.5 0.8 1.0 × 10−8 8 ≤0.0 ≤0.0 6.2 6.2
18413+1354 3300** −0.5 1.2 1.0 × 10−8 15 1.8 1.7 ≤5.3 ≤5.3
18429−1721 3000 −0.5 0.2 1.0 × 10−8 7 1.2 1.1 5.8 5.8
19129+2803 3300** −0.5 0.2 1.0 × 10−8 11 3.11 3.11 5.5 5.5
19361−1658 3000 −0.5 0.2 1.0 × 10−9 8 1.9 2.0 5.8 5.8
20052+0554* 3300 −0.5 0.2 1.0 × 10−7 16 2.6 2.3
20343−3020 3000 −0.5 1.2 1.0 × 10−9 8 ≤−1.0 ≤0.0 6.0 6.0
RU Cyg 3000 −0.5 1.6 1.0 × 10−7 12 2.0 1.7 6.2 6.2
SV Cas 3000 −0.5 1.6 1.0 × 10−7 12 3.5 3.3 6.3 6.3
R Cen2 3000 −0.5 1.6 1.0 × 10−7 5 4.3 4.0

Notes. (†)These stars only display a single peak in the 1612 MHz OH maser, so we adopt an average velocity in the abundance analysis exploring OH expansion velocities of other stars with similar variability periods. (*)The S/N at Ca I 6463 Å is very low to derive any Ca abundance estimate. (**)The best fitting Teff in the Ca I 6463 Å spectral region is cooler (3000 K) than the one around the Li I 6708 Å line. (1)The line is resolved in two components (circumstellar and photospheric) and the abundance obtained corresponds to the photospheric one. (2)R Cen was not observed in the Ca I line region.

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