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| Query : 2007MNRAS.377..645S |
2007MNRAS.377..645S - Mon. Not. R. Astron. Soc., 377, 645-656 (2007/May-2)
Amplitude saturation in β Cephei models.
SMOLEC R. and MOSKALIK P.
Abstract (from CDS):
Several models of different masses and metallicities were converged to limit cycles through the Stellingwerf relaxation technique. The resulting peak-to-peak amplitudes are of the order of ΔV = 0.3 mag. Such amplitudes are significantly larger than those observed in β Cephei pulsators. Assuming that all acoustic modes are similar, we show that collective saturation of the driving mechanism by several acoustic modes can easily lower predicted saturation amplitudes to the observed level. Our calculations predict a significant decrease in saturation amplitudes as we go to high-mass/high-luminosity models. However, this effect is not strong enough to explain the scarcity of high-mass β Cephei variables. A possible weakness of the collective saturation scenario is that the estimated line-broadening, resulting from excitation of many high-l modes, might be higher than that observed in some of the β Cephei stars. We argue that this difficulty can be overcome by allowing g-modes to participate in the saturation process.
We also discuss robust double-mode (DM) behaviour, encountered in our radiative models. On a single evolutionary track we identify two DM domains with two different mechanisms responsible for DM behaviour. The non-resonant DM domain separates the first overtone and fundamental-mode pulsation domains. The resonant DM domain appears in the middle of the first overtone pulsation domain. Its origin can be traced to the 2ω1= ω0+ ω2 parametric resonance, which destabilizes the first overtone limit cycle.
Abstract Copyright: 2007 The Authors. Journal compilation © 2007 RAS
Journal keyword(s): hydrodynamics - stars: early-type - stars: oscillations - stars: variables: other
CDS comments: In table 1 : NGC 6910 v24 is a misprint for NGC 6910 v27
Simbad objects: 27
| Number of rows : 27 |
| 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 | * gam Peg | bC* | 00 13 14.1523490172 | +15 11 00.954346538 | 1.75 | 2.61 | 2.84 | 2.94 | 3.13 | B2IV | 720 | 0 |
| 2 | BD+56 501 | bC* | 02 18 29.8336293096 | +57 09 03.164872428 | 8.98 | 9.631 | 9.4150 | B0.5I | 41 | 0 | ||
| 3 | BD+56 520 | bC* | 02 19 00.2068359360 | +57 08 44.320290036 | 9.71 | 10.20 | 10.0010 | B1.5IV | 34 | 0 | ||
| 4 | V* V595 Per | bC* | 02 22 08.5707880560 | +57 07 28.398038160 | 8.80 | 9.37 | 8.3166 | 7.7657 | B0.5IV | 59 | 0 | |
| 5 | * del Cet | bC* | 02 39 28.9568473856 | +00 19 42.631195332 | 2.97 | 3.85 | 4.07 | B2IV | 395 | 0 | ||
| 6 | NAME Magellanic Clouds | GrG | 03 00 | -71.0 | ~ | 7988 | 0 | |||||
| 7 | * ksi01 CMa | bC* | 06 31 51.3662820799 | -23 25 06.319934859 | 3.10 | 4.09 | 4.33 | 4.45 | 4.72 | B0.7IV | 336 | 0 |
| 8 | V* KK Vel | bC* | 09 07 42.5207085395 | -44 37 56.750000545 | 6.03 | 6.76 | 6.80 | B2II/III | 68 | 0 | ||
| 9 | V* V1228 Cen | bC* | 11 33 18.0211695240 | -63 06 16.213109580 | 9.07 | 9.77 | 9.62 | 9.95 | B1III | 31 | 0 | |
| 10 | CPD-62 2707 | bC? | 12 22 12.8654135976 | -63 20 47.806965096 | 9.43 | 10.09 | 10.07 | 10.16 | B2III | 25 | 0 | |
| 11 | CPD-59 4549 | bC* | 12 53 43.8838517496 | -60 22 29.353445652 | 9.04 | 9.92 | 9.78 | 10.04 | B1.5V | 41 | 0 | |
| 12 | LS 2814 | bC* | 12 53 52.0067925720 | -60 22 15.879036216 | 8.92 | 9.54 | 9.38 | 9.81 | B1V | 34 | 0 | |
| 13 | CPD-59 4562 | bC* | 12 53 53.0059575120 | -60 21 30.852990432 | 9.71 | 10.363 | 10.204 | B2Vn | 23 | 0 | ||
| 14 | * tau01 Lup | bC* | 14 26 08.2244287979 | -45 13 17.123883210 | 3.68 | 4.393 | 4.553 | B2IV | 158 | 0 | ||
| 15 | HD 133823 | bC? | 15 09 54.5953566408 | -65 30 22.612602132 | 8.98 | 9.64 | 9.59 | B3II | 23 | 0 | ||
| 16 | * del Lup | bC* | 15 21 22.3138254072 | -40 38 51.109328940 | 2.12 | 2.995 | 3.190 | B1.5IV | 230 | 0 | ||
| 17 | CPD-46 8213 | * | 16 46 30.2421031488 | -47 01 10.392834792 | 11.03 | 11.44 | 10.89 | ~ | 12 | 1 | ||
| 18 | HD 328906 | bC? | 16 49 38.6234223792 | -44 31 41.185389756 | 12.34 | 11.25 | B2 | 8 | 0 | |||
| 19 | HD 152477 | Pu* | 16 55 53.6490838344 | -48 08 51.966884940 | 9.5 | 9.66 | 9.10 | 8.73 | 9.314 | B1Ib | 30 | 0 |
| 20 | HD 164340 | bC* | 18 02 32.9452043448 | -40 05 16.419321528 | 8.2 | 9.16 | 9.25 | B0/0.5(III) | 46 | 0 | ||
| 21 | BD-14 5047 | Be* | 18 26 39.3110276784 | -14 38 19.354958556 | 10.60 | 10.99 | 10.29 | 10.25 | B0e | 26 | 0 | |
| 22 | HD 180642 | bC* | 19 17 14.8038514896 | +01 03 33.904495728 | 7.83 | 8.47 | 8.29 | B1.5II-III | 107 | 0 | ||
| 23 | LS III +40 12 | bC* | 20 23 07.5749623752 | +40 46 08.882776740 | 11.058 | 11.239 | 10.412 | 18.755 | 9.355 | B0.5V | 31 | 0 |
| 24 | NGC 6910 27 | bC* | 20 23 33.7529737579 | +40 45 19.930686094 | 12.82 | 11.77 | B1III | 21 | 0 | |||
| 25 | V* BW Vul | bC* | 20 54 22.3947588600 | +28 31 19.190976132 | 5.47 | 6.40 | 6.54 | B2IIIv | 301 | 0 | ||
| 26 | V* HN Aqr | bC* | 22 37 38.2846689672 | -18 39 51.268772880 | 11.293 | 11.426 | 11.813 | B | 70 | 0 | ||
| 27 | Cl* NGC 663 P V4 | V* | ~ | ~ | 11.1 | ~ | 2 | 0 |
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