2002A&A...393..167L


Query : 2002A&A...393..167L

2002A&A...393..167L - Astronomy and Astrophysics, volume 393167-181 (2002/10-1)

The modelling of intermediate-age stellar populations. II. Average spectra for upper AGB stars, and their use.

LANCON A. and MOUHCINE M.

Abstract (from CDS):

The upper Asymptotic Giant Branch (AGB) is populated with oxygen rich and carbon rich Long Period Variables (LPVs). These stars are essential contributors to the near-IR light of intermediate age stellar populations. Individual observed spectra of LPVs are so diverse that they cannot be used directly in the synthesis of galaxy spectra. In this paper, the library of individual spectra of Lancon & Wood (2000A&A...353..322A) is used to construct averages that can be incorporated conveniently in population synthesis work. The connection between such spectra and stellar evolution tracks is discussed. In order to select a sorting criterion and to define averaging bins for the LPV spectra, correlations between their spectrophotometric properties are reexamined. While optical properties and broad baseline colours such as (I-K) are well correlated, a large dispersion is observed when these indices are plotted against near-IR ones. This is partly due to the intrinsic width of the upper AGB, which is illustrated by locating each of the multiple observations of individual LPVs on the HR diagram. It is argued that broad baseline colour-temperatures are the most sensible sorting criteria. The properties of the resulting sequence of average spectra indeed vary regularly. We further address: (i) the bolometric corrections and temperature scales needed to associate a spectrum with a given point on a theoretical stellar evolution track (or isochrone), (ii) the simplifying assumptions that will be implicitely made when using the average spectra, (iii) potential biases in the sample of Lancon & Wood and their effects, (iv) the small contribution of LPVs to the interstellar hydrogen emission lines in galaxies. It is emphasized that an a posteriori calibration of the effective temperature scale remains necessary, until consistent models for the evolution, the pulsation and the spectral appearance of LPVs become available. We suggest a recipe for the use of the average spectra at various metallicities.

Abstract Copyright: ∼

Journal keyword(s): stars: AGB and post-AGB - stars: late-type - stars: variable: general - Hertzsprung-Russell diagram - infrared: stars - galaxies: stellar content

VizieR on-line data: <Available at CDS (J/A+A/393/167): 36 averaged spectra extending from 510 to 2490nm>

CDS comments: V584 Apl is a misprint for V584 Aql.

Simbad objects: 32

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Number of rows : 32
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 V* VY Cas AB* 00 51 26.0014485360 +62 55 14.872790748   10.94 9.62     M6/7III 60 0
2 IRC +10011 OH* 01 06 25.9879717848 +12 35 52.896392052   20.7   18.26 14.01 M8 436 0
3 V* CE And AB* 01 29 33.2705595168 +46 39 33.032270376   11.65 10.13     M5 27 0
4 V* RS Hor Mi* 02 35 52.2155533128 -62 35 00.460442076   15.413 14.015 12.165   M3e 21 0
5 V* X Men OH* 03 32 29.6297747184 -76 26 55.031558748           M3e 35 0
6 V* T Cae C* 04 47 18.9236637528 -36 12 33.571330524 13.27 10.05 7.73     C-N4IV: 64 0
7 V* R Lep C* 04 59 36.3486921120 -14 48 22.502479140 15.06 13.51 7.76 4.90 3.42 C7,6e 360 0
8 V* RU Pup C* 08 07 29.8292965296 -22 54 45.272487204   12.07 8.45 7.35   C-N5III: 71 0
9 V* R Cha Mi* 08 21 46.4588734296 -76 21 18.302197932   11.94 10.55     M4.5e 65 0
10 V* SY Vel AB* 09 12 25.7260697400 -43 46 38.706262860   9.40 8.12     M5/6III 23 0
11 V* UZ Hya Mi* 09 16 46.2068618472 -04 35 12.832336716   12.86 11.39 12.97   M4e 17 0
12 V* CM Car Mi* 09 47 55.5824251656 -67 27 07.030380348       13.56   M2e 22 0
13 V* Y Hya C* 09 51 03.7177289688 -23 01 02.351120088 17.75 10.45 6.63     C-N4.5III: 118 0
14 V* S Car Mi* 10 09 21.8927735544 -61 32 56.433503472 9.38 7.63 5.71 5.20 3.64 K5-M6e 144 0
15 V* RZ Car Mi* 10 35 37.2540220752 -70 43 00.190278408     8.80     M7-8II?e 39 0
16 V* RS Hya Mi* 10 51 19.0356495120 -28 37 40.482529176     12 9.57   Me 33 0
17 V* KV Car AB* 11 03 02.6141965944 -67 07 37.250924844   9.55 7.83     M4III 22 1
18 V* U Crt Mi* 11 12 45.3032864448 -07 17 54.561095196   12.76 11.20 10.61   M0e 29 0
19 V* BD Hya Mi* 11 16 11.7723641760 -30 10 51.395707920   11.47 10.21 9.24   M0e 10 1
20 V* BH Cru C* 12 16 16.7900401416 -56 17 09.626993196   10.60 7.96     C8,2 86 1
21 V* S Cen C* 12 24 33.9185490504 -49 26 24.728127180 11.92 9.45 7.60     C-R4 53 0
22 V* T Cen Mi* 13 41 45.5635339752 -33 35 50.560017864 8.59 7.49 6.05     K5-M4e 77 0
23 RAFGL 1686 OH* 14 11 17.5995820440 -07 44 49.834416336       16.28   M9III 73 0
24 V* S Lib Mi* 15 21 23.9864456016 -20 23 18.410047008   10.9 7.50 8.92   M1.5-4e 83 0
25 V* RS Lib Mi* 15 24 19.7909986800 -22 54 39.843703260   10.59 7.00 6.85   M7-8e 129 0
26 V* WW Sco Mi* 16 27 22.1483956920 -31 18 14.416024536     12     M9 27 0
27 V* SV Tel Mi* 18 56 17.9276298192 -49 28 09.769749240   11.68 10.95     M4e 15 0
28 V* V1351 Cyg LP* 19 42 04.1469995832 +55 27 47.597570424 9.65 8.09 6.48     M5III 54 0
29 V* V584 Aql AB* 20 10 29.8266386760 -01 37 40.821495780   10.55 9.19     M4(III) 33 0
30 V* SV Peg AB* 22 05 42.0835861728 +35 20 54.562625016   10.06 9.20     M7 146 0
31 V* R Phe Mi* 23 56 27.5567081328 -49 47 12.603031980   10.580 7.50 9.93 8.692 M4/5(III)e 47 0
32 V* S Phe AB* 23 59 04.5698011104 -56 34 32.294635896 9.80 8.57 6.93     M5e 55 0

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