2007MNRAS.377..645S


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):

Although the driving mechanism acting in β Cephei pulsators is well known, problems concerning the identification of the amplitude limitation mechanism and the non-uniform filling of the theoretical instability strip remain to be solved. In the present analysis, these problems are addressed by non-linear modelling of radial pulsations of these stars. In this approach radial modes are treated as representative of all acoustic oscillations.

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

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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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