Bibcode
Vauclair, G.; Solheim, J.-E.; Fu, J.-N.; Chevreton, M.; Dolez, N.; O'Brien, M. S.; Mukadam, A. S.; Kim, S.-L.; Park, B.-G.; Handler, G.; Medupe, R.; Wood, M.; González Perez, J.; Hashimoto, O.; Kinugasa, K.; Taguchi, H.; Kambe, E.; Dobrovolskas, V.; Provencal, J. L.; Dreizler, S.; Schuh, S.; Leibowitz, E. M.; Lipkin, Y.; Zhang, X.-B.; Paparo, M.; Szeidl, B.; Virághalmy, G.; Zsuffa, D.
Referencia bibliográfica
15th European Workshop on White Dwarfs ASP Conference Series, Vol. 372, proceedings of the conference held 7-11 August, 2006 in Leicester, United Kingdom. Edited by Ralf Napiwotzki and Matthew R. Burleigh. San Francisco: Astronomical Society of the Pacific, 2007., p.641
Fecha de publicación:
9
2007
Número de citas
1
Número de citas referidas
0
Descripción
While Abell 43 is entering the PG 1159 instability strip, in fact as an
"hybrid-PG 1159" nucleus of a planetary nebula, PG 0122+200 presently
defines its red edge. So these two stars define the limits of the
instability strip along the evolutionary sequence from the planetary
nebula nuclei to the pre-white dwarf PG 1159 stars. We describe the new
observations that have been obtained recently on these two extreme PG
1159 pulsators. Abell 43, the second discovered "hybrid-PG 1159"
pulsator after HS 2324+3944, is a multi-periodic low amplitude pulsator
with the longest period observed so far in PG 1159 pulsators. As it
shows amplitude variations, follow-up observations are needed to obtain
a sufficient number of frequencies to start an asteroseismological
analysis. We summarize the status of the presently available data. On PG
0122+200, new observations were obtained in 2001 and 2002. Together with
previous data, they allow us to detect 23 frequencies, including seven
triplets and two single frequencies. We interpret the triplets as
ℓ=1 modes split by rotation and confirm an average rotation period
of 1.55 days. From the up-dated average period spacing of 22.9 s, we
derive a mass of 0.59 ± 0.02 M&sun;, in better
agreement with the spectroscopically derived mass than from previous
estimates, and a luminosity log(L/L&sun;)= 1.3 ± 0.5.
The uncertainty on the luminosity is dominated by the poorly determined
surface gravity. We discuss the impact of that new mass determination on
the predicted neutrino luminosity.