The LM method was applied four times, as described in Sect. 3, once for each photometric bandpass: V - results already presented in Mennessier et al. (1997b) -, K, 12 and 25 - in the present paper. In principle, one could assign a joint luminosity distribution to two or more bandpass magnitudes simultaneously, and the LM method would separate the sample into stellar groups consistent with all the photometric measurements together. This option, however, requires a perfectly well known relationship between the different magnitudes in order to define a joint distribution function as realistic as possible for all the band passes. The correlation between the near-infrared (K) and IRAS infrared properties presently cannot be well modeled and very likely has a non-unique form depending on the stellar and circumstellar evolutive stage along the AGB. Thus, we decided not to couple the photometric band passes and to calibrate each luminosity separately. Furthermore, bandpasses are related to different physical processes and can provide separate interesting information: V is greatly affected by absorption molecular lines, K reflects the stellar emission, and IRAS bandpasses depend on the nature and density of grains in the circumstellar envelope.
The LM method is simultaneously sensitive to kinematics and luminosity and thus the number of significant discriminating groups depends on both these characteristics and is not necessarily the same for the different bandpass analyses. Furthermore, the samples used are not the same, and this can also affect the number of discriminated groups.
Six distinct groups are identified in the V magnitudes, three in K and four in each of the two IRAS magnitudes. Those are successively analyzed in terms of the classical galactic populations. Although the number of groups is found to be different for each analysis, the groups present similarities in their kinematical composition and with respect to the galactic populations (see Sect. 6).
An analysis of the six groups identified in the V band has been presented in Mennessier et al. (1997b). In order to compare these results with the ones obtained for infrared calibrations, the main results are summarized here. Table 1 reviews the estimated mean parameters for the analysis corresponding to the V luminosity at the phase of maximum light. The LPVs are found to belong to all galactic populations from disk to very extended disk. We wish to emphasize three points:
Group | BD | D | OD1 | OD2 | TD | ED |
MV | -3.6 | -1.0 | -1.2 | -0.2 | -1.2 | -2.8 |
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1.4 | 0.8 | 0.2 | 1.0 | 0.5 | 1.2 |
U0 | -10 | -6 | -44 | -1 | -34 | -61 |
V0 | -11 | -6 | -35 | -21 | -84 | -235 |
W0 | -13 | -6 | -6 | -10 | -19 | -20 |
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13 | 24 | 28 | 37 | 77 | 188 |
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14 | 14 | 25 | 23 | 29 | 126 |
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9 | 9 | 22 | 23 | 65 | 72 |
Z0 | 104 | 126 | 217 | 249 | 409 | 1227 |
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8 | 25 | 13 | 44 | 8 | 2 |
Only three groups are identified in the K band. From their kinematics and spatial distribution, given in Table 2, they can be interpreted as the galactic disk (D), old disk (OD) and extended disk (ED) populations. They are similar to the four main groups identified in the V band (Sect. 4.1), except that the disk and a part of the old disk population seem to be mixed.
In a previous analysis of a sample restricted to O-rich Miras (Alvarez
et al. 1997), only two groups were found. One corresponded to the
extended disk population, with a percentage of 17, in agreement
with our result i.e.
of O-rich Miras belonging to the ED
group (see Table 7).
The other group mixed disk and old
disk populations. In the present paper, a more numerous sample allows a
more refined separation of the kinematic populations.
Group D | Group OD | Group ED | ||||
est. | ![]() |
est. | ![]() |
est. | ![]() |
|
K0 | -6.1 | 0.4 | -6.0 | 0.7 | -5.3 | 0.8 |
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1.1 | 0.3 | 0.7 | 0.4 | 1.4 | 0.5 |
U0 | -7 | 10 | -17 | 27 | -21 | 14 |
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29 | 9 | 45 | 16 | 111 | 11 |
V0 | -12 | 8 | -36 | 25 | -123 | 12 |
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16 | 5 | 27 | 11 | 69 | 18 |
W0 | -9 | 6 | -6 | 9 | -20 | 19 |
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12 | 3 | 26 | 13 | 90 | 25 |
Z0 | 184 | 44 | 268 | 85 | 782 | 313 |
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60 | 35 | 5 |
Group D | Group ODb | Group ODf | Group ED | |||||
est. | ![]() |
est. | ![]() |
est. | ![]() |
est. | ![]() |
|
120 | -6.4 | 0.3 | -8.0 | 0.4 | -6.4 | 0.5 | -6.2 | 1.0 |
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1.7 | 0.1 | 1.2 | 0.2 | 0.6 | 0.4 | 1.6 | 0.2 |
U0 | -6 | 9 | -12 | 5 | -10 | 9 | -30 | 37 |
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22 | 6 | 35 | 8 | 39 | 6 | 106 | 45 |
V0 | -7 | 8 | -26 | 7 | -24 | 8 | -97 | 54 |
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12 | 5 | 26 | 11 | 22 | 6 | 65 | 64 |
W0 | -9 | 4 | -9 | 5 | -8 | 5 | -2 | 44 |
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9 | 8 | 21 | 8 | 21 | 7 | 75 | 29 |
Z0 | 161 | 55 | 258 | 56 | 256 | 79 | 1065 | 724 |
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29 | 32 | 29 | 10 |
Group D | Group ODb | Group ODf | Group ED | |||||
est. | ![]() |
est. | ![]() |
est. | ![]() |
est. | ![]() |
|
250 | -7.1 | 0.5 | -8.6 | 0.4 | -6.5 | 0.3 | -6.8 | 0.8 |
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1.7 | 0.1 | 1.2 | 0.2 | 0.6 | 0.4 | 1.6 | 0.5 |
U0 | -6 | 6 | -10 | 4 | -10 | 7 | -39 | 48 |
![]() |
21 | 8 | 36 | 10 | 38 | 6 | 111 | 33 |
V0 | -6 | 4 | -26 | 7 | -22 | 6 | -99 | 63 |
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13 | 4 | 27 | 9 | 22 | 5 | 69 | 23 |
W0 | -10 | 4 | -9 | 5 | -8 | 4 | 1 | 42 |
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11 | 7 | 21 | 8 | 20 | 4 | 75 | 37 |
Z0 | 158 | 43 | 277 | 34 | 270 | 107 | 1610 | 1180 |
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28 | 32 | 30 | 10 |
The four LPV groups identified in the IRAS 12 and 25 bands are given in Tables 3 and 4, respectively. They are similar to those identified in the K band (Table 2), except that the old disk group is further divided into "bright'' (ODb) and "faint'' (ODf) subgroups. Let us remember here that the method allows us to distinguish groups with similar mean kinematics but different luminosities (ODb and ODf) or groups with a similar luminosity distribution but different kinematics (D and ED for instance). Moreover, it is important to remark that D, ODb and ED have, on average, a similar color index 25-12 = -0.6 mag corresponding to a thick circumstellar envelope, while ODf has a mean index of 0.1 mag that suggests that the majority of the stars in this last group have thin envelopes.
Let us finally point out that the kinematic parameters ( U0,V0,W0) associated with each of the four groups are very similar for both the 12 and 25 calibrations.
Copyright ESO 2001