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Long-Term Variability in o Ceti and Other Mira Variables: Signs of Supergranular Convection?
- Source :
- AIP Conference Proceedings; 9/16/2009, Vol. 1170 Issue 1, p164-166, 3p, 2 Graphs
- Publication Year :
- 2009
-
Abstract
- We describe our study of long-term variability of o Ceti (Mira A), the prototype of the Mira-type pulsating stars. Our study was originally undertaken to search for coherent long-period variability, but the results of our analysis didn’t uncover this. However, we detected a low-frequency “red noise” in the Fourier spectrum of the o Ceti century-long light curve. We have since found similar behavior in other Miras and pulsating giant stars and have begun a study of a large sample of Mira variables. Similar red noise has been previously detected in red supergiants and attributed to supergranular convection. Its presence in Miras suggests the phenomenon may be ubiquitous in cool giant pulsators. These results support high-angular resolution observations of Miras and supergiants showing asymmetries in their surface brightness distributions, which may be due to large supergranular convection cells. Theoretical modeling, and numerical simulations of pulsation processes in late-type giants and supergiants should therefore take into account the effects of deep convection and large supergranular structures, which in turn may provide important insights into the behavior of Miras and other giant and supergiant pulsators. In this work, we summarize our results for o Ceti, present preliminary results of our broader study of Mira variables, and discuss how the results of this study may be used by future studies of AGB variables. [ABSTRACT FROM AUTHOR]
- Subjects :
- STARS
VARIABLE stars
ASTROPHYSICS
ASTRONOMICAL observations
PULSATING stars
Subjects
Details
- Language :
- English
- ISSN :
- 0094243X
- Volume :
- 1170
- Issue :
- 1
- Database :
- Complementary Index
- Journal :
- AIP Conference Proceedings
- Publication Type :
- Conference
- Accession number :
- 44292552
- Full Text :
- https://doi.org/10.1063/1.3246434