2013A&A...554A..46G


Query : 2013A&A...554A..46G

2013A&A...554A..46G - Astronomy and Astrophysics, volume 554A46-46 (2013/6-1)

Atmospheric dynamics in RR Lyrae stars. The Blazhko effect.

GILLET D.

Abstract (from CDS):

Discovered in 1907, the Blazhko effect is a modulation of the light variations of about half of the RR Lyr stars. It has remained unexplained for over 100 years, despite more than a dozen proposed explanations. Today it represents an ongoing challenge in variable-star research. We propose a new explanation. It is based on the observation that Blazhko stars seem to be located in the region of the instability strip where fundamental and first overtone modes are excited at the same time. An analysis of nonlinear and nonadiabatic pulsation models of RR Lyrae stars shows that a specific shock (called first overtone shock) may be generated by the perturbation of the fundamental mode by the transient first overtone. The first overtone shock induces a sharp slowdown of the atmospheric layers during their infalling motion. This slowdown in turn affects the compression rate on the deep photospheric layers and the intensity of the κ-mechanism. After an amplification phase, the intensity of the main shock wave before the Blazhko maximum becomes high enough to provoke large radiative losses. These can be at least equal to 70% of the total energy flux of the shock, which induces a small decrease of the effective temperature at each pulsation cycle. In these conditions, when the intensity of the main shock reaches its highest critical value at the Blazhko maximum, it completely desynchronizes the motion of the phostospheric layers. At this point, the atmosphere relaxes and reaches a new synchronous state that occurs at the Blazhko minimum. The combined effects of these two shocks on the atmosphere cause the Blazhko effect. This effect can only exist if the first overtone mode is excited together with the fundamental mode. Because the involved physical mechanisms are essentially nonlinear (shocks, atmospheric dynamics, radiative losses, mode excitations), the Blazhko process is expected to be unstable and irregular. Consequently, the Blazhko process has a specific random nature that is in contrast with the pulsation of non-Blazhko stars.

Abstract Copyright: ∼

Journal keyword(s): shock waves - stars: atmospheres - stars: variables: RR Lyrae - stars: individual: RR Lyr

Simbad objects: 33

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Number of rows : 33
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 ESO 193-37 G 00 13 21.4024634424 -49 21 43.726819824   14.63   13.57   ~ 14 0
2 V* RU Psc RR* 01 14 26.0371799376 +24 24 56.367501264   10.34 10.15     kA6hF3 90 0
3 V* XY And RR* 01 26 42.4340330568 +34 04 06.883141332   12.98 13.72     ~ 34 0
4 V* RR Cet RR* 01 32 08.1731409309 +01 20 30.230098757 9.46 9.33 9.15     A9V 237 0
5 V* SS For RR* 02 07 51.9781810872 -26 51 57.716828856   10.45 10.20     kF5hF8 119 0
6 V* X Ari RR* 03 08 30.8846437148 +10 26 45.218712967 9.45 9.25 8.97     F0.5 305 0
7 V* RX Eri RR* 04 49 44.2915145832 -15 44 28.242958128 9.64 9.43 9.22     kA8.5hF6.5 196 0
8 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
9 V* RR Gem RR* 07 21 33.5312487888 +30 52 59.459320164   12.34 11.92     kA2hA7.5 217 0
10 V* SS Cnc RR* 08 06 25.5852208464 +23 15 05.630616828   12.40 12.11     kA3.5hA8.5 109 0
11 V* UZ Vir RR* 13 08 44.3344481376 +13 24 08.384399280     13.62     ~ 28 0
12 M 53 GlC 13 12 55.25 +18 10 05.4     7.79     ~ 907 0
13 NGC 5139 GlC 13 26 47.28 -47 28 46.1           ~ 3677 0
14 V* TV Boo RR* 14 16 36.5814789480 +42 21 35.712985824   11.23 10.93     kB9.5hF1 132 0
15 M 5 GlC 15 18 33.22 +02 04 51.7     5.95     ~ 2095 0
16 V* RW Dra RR* 16 35 31.6036225488 +57 50 23.167269564   11.87 11.48     kA7hF6.5 164 0
17 Z 300-12 G 17 20 14.335 +57 55 16.39   12.40 10.6     ~ 1428 1
18 NGC 6362 GlC 17 31 54.99 -67 02 54.0           ~ 637 0
19 V* BL Her WV* 18 01 09.2240599584 +19 14 56.696475012   10.54 9.70     F0 182 0
20 V* MW Lyr RR* 18 19 53.8179512304 +31 58 54.622695360           ~ 50 0
21 V* RZ Lyr RR* 18 43 37.8850558416 +32 47 53.951055936   11.78 11.57     kA3.5hF6 122 0
22 V* V350 Lyr RR* 18 49 08.3623722840 +46 11 54.943897272           ~ 32 0
23 V* V354 Lyr RR* 18 52 50.3556721536 +41 33 49.358051388     15.99 16.61   ~ 37 0
24 V* V445 Lyr RR* 18 58 25.6944987672 +41 35 49.188746868   15.3       ~ 36 0
25 V* V360 Lyr RR* 19 01 58.6389312552 +46 26 45.637097856       16.71   ~ 34 0
26 2MASS J19102676+4233375 RR* 19 10 26.7692571672 +42 33 37.471655916           ~ 21 0
27 V* RR Lyr RR* 19 25 27.9129605304 +42 47 03.693258204   7.36   7.6   kA3hF0 951 0
28 ATO J291.6554+01.2262 RR* 19 26 37.3219673784 +01 13 34.777336800   15.6 15.928 14.8   ~ 25 0
29 M 55 GlC 19 39 59.71 -30 57 53.1     6.49     ~ 913 0
30 V* DM Cyg RR* 21 21 11.5417679280 +32 11 28.708593720   11.83 11.63     kF4hF7.5 127 0
31 V* BV Aqr RR* 22 02 53.9976005136 -21 31 32.147256936   11.27 11.05     ~ 52 0
32 V* CZ Lac RR* 22 19 30.7339244592 +51 28 14.820549168   11.10 11.20     kB8.5hF0 87 0
33 NAME Galactic Bulge reg ~ ~           ~ 4794 0

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