2006ApJ...650.1111S


Query : 2006ApJ...650.1111S

2006ApJ...650.1111S - Astrophys. J., 650, 1111-1118 (2006/October-3)

MOST(1) detects g- and p-modes in the B supergiant HD 163899 (B2 Ib/II).

SAIO H., KUSCHNIG R., GAUTSCHY A., CAMERON C., WALKER G.A.H., MATTHEWS J.M., GUENTHER D.B., MOFFAT A.F.J., RUCINSKI S.M., SASSELOV D. and WEISS W.W.

Abstract (from CDS):

The Microvariability and Oscillations of Stars (MOST) satellite observed the B supergiant HD 163899 (B2 Ib/II) for 37 days as a guide star and detected 48 frequencies ≲2.8 cycles/day with amplitudes of a few millimagnitudes (mmag) and less. The frequency range embraces g- and p-mode pulsations. It was generally thought that no g-modes are excited in less luminous B supergiants because strong radiative damping is expected in the core. Our theoretical models, however, show that such g-modes are excited in massive post-main-sequence stars, in accordance with these observations. The nonradial pulsations excited in models between 20 M☉at logTeff~4.41 and 15 M☉at logTeff~4.36 are roughly consistent with the observed frequency range. Excitation by the Fe bump in opacity is possible because g-modes can be partially reflected at a convective zone associated with the hydrogen-burning shell, which significantly reduces radiative damping in the core. The MOST light curve of HD 163899 shows that such a reflection of g-modes actually occurs and reveals the existence of a previously unrecognized type of variable, slowly pulsating B supergiants (SPBsg) distinct from α Cyg variables. Such g-modes have great potential for asteroseismology.

Abstract Copyright: ∼

Journal keyword(s): Stars: Early-Type - stars: individual (HD 163899) - Stars: Oscillations - Stars: Supergiants

Simbad objects: 13

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Number of rows : 13
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 * del Cet bC* 02 39 28.9568473856 +00 19 42.631195332 2.97 3.85 4.07     B2IV 395 0
2 * iot CMa s*b 06 56 08.2245944314 -17 03 15.259069948 3.62 4.297 4.385 6.40   B3Ib 184 0
3 HD 54764 Pu* 07 09 33.3632699976 -16 14 04.233013116 5.320 6.120 6.080 7.42   B1Ib/II 85 0
4 * J Pup s*b 07 53 18.1574768969 -48 06 10.566474468 3.11 4.10 4.24 4.26 4.38 B0.5Ib 249 0
5 V* V536 Car bC* 11 18 18.3434633112 -62 58 28.471439604 8.56 9.55 9.49 9.48   B2.5Ib/II 38 1
6 HD 141318 Pu* 15 51 06.8041626360 -55 03 19.928655972 5.13 5.756 5.767 7.08   B2III 93 0
7 * zet Oph Be* 16 37 09.5400587698 -10 34 01.509742704 1.73 2.58 2.56 2.46 2.50 O9.2IVnn 1908 0
8 HD 163830 Pu* 17 59 40.8979752504 -33 39 10.541067156   9.26 9.27     B5II/III 11 0
9 HD 163899 Pu* 17 59 56.3483552352 -33 53 26.956220568 7.88 8.51 8.31 9.17 8.59 B2Ib/II 53 0
10 HD 163868 Be* 17 59 56.4314226144 -33 24 29.980813608 6.69 7.311 7.354     B5Ve 72 0
11 HD 164270 WR* 18 01 43.1453595672 -32 42 55.161329040 8.52 8.97 8.74 9.51   WC9d+? 233 0
12 HD 164388 * 18 02 17.6232410184 -33 46 04.823740668   8.12 7.97     A2IV 15 0
13 V* QR Ser SB* 18 18 58.6907022768 -13 59 28.456622916 7.92 8.55 8.28 9.07   O9.5III+B3-5V/III 91 0

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