TY - JOUR
T1 - The high ratio of44Ti/56Ni in Cassiopeia a and the axisymmetric collapse-driven supernova explosion
AU - Nagataki, Shigehiro
AU - Hashimoto, Masa Aki
AU - Sato, Katsuhiko
AU - Yamada, Shoichi
AU - Mochizuki, Yuko S.
N1 - Funding Information:
We would like to thank F. X. Timmes for useful comments. We are also grateful to S. Hardy and L. van Waer-beke for their kind review of the manuscript. This research has been supported in part by a Grant-in-Aid for the Center-of-Excellence (COE) Research (07CE2002) and for the Scientific Research Fund (05243103, 07640386, 3730) of the Ministry of Education, Science, and Culture in Japan, and by the Japan Society for the Promotion of Science Postdoctoral Fellowships for Research Abroad.
PY - 1998
Y1 - 1998
N2 - The large abundance ratio of 44Ti/56Ni in Cassiopeia A is puzzling. In fact, the ratio seems to be larger than the theoretical constraint derived by Woosley & Hoffman. However, this constraint is obtained on the assumption that the explosion is spherically symmetric, whereas Cas A is famous for the asymmetric form of the remnant. Recently, Nagataki et al. calculated the explosive nucleosynthesis of axisymmetrically deformed collapse-driven supernova. They reported that the ratio of 44Ti/56Ni was enhanced by the stronger alpha-rich freezeout in the polar region. In this Letter, we apply these results to Cas A and examine whether this effect can explain the large amount of 41Ti and the large ratio of 44Ti/56Ni. We demonstrate that the conventional, spherically symmetric explosion model cannot explain the 44Ti mass produced in Cas A if its lifetime is shorter than ∼80 yr and the intervening space is transparent to the gamma-ray line from the decay of 44Ti. On the other hand, we show that the axisymmetric explosion models can solve the problem. We expect the same effect from a three-dimensionally asymmetric explosion, since the stronger alpha-rich freezeout will also occur in that case in the region where the larger energy is deposited.
AB - The large abundance ratio of 44Ti/56Ni in Cassiopeia A is puzzling. In fact, the ratio seems to be larger than the theoretical constraint derived by Woosley & Hoffman. However, this constraint is obtained on the assumption that the explosion is spherically symmetric, whereas Cas A is famous for the asymmetric form of the remnant. Recently, Nagataki et al. calculated the explosive nucleosynthesis of axisymmetrically deformed collapse-driven supernova. They reported that the ratio of 44Ti/56Ni was enhanced by the stronger alpha-rich freezeout in the polar region. In this Letter, we apply these results to Cas A and examine whether this effect can explain the large amount of 41Ti and the large ratio of 44Ti/56Ni. We demonstrate that the conventional, spherically symmetric explosion model cannot explain the 44Ti mass produced in Cas A if its lifetime is shorter than ∼80 yr and the intervening space is transparent to the gamma-ray line from the decay of 44Ti. On the other hand, we show that the axisymmetric explosion models can solve the problem. We expect the same effect from a three-dimensionally asymmetric explosion, since the stronger alpha-rich freezeout will also occur in that case in the region where the larger energy is deposited.
KW - Nuclear reactions, nucleosynthesis, abundances
KW - Supernovae: general
KW - supernovae: individual (Cassiopeia A, SN 1987A)
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U2 - 10.1086/311089
DO - 10.1086/311089
M3 - Article
AN - SCOPUS:33144489202
SN - 0004-637X
VL - 492
SP - L45-L48
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 1 PART II
ER -