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First Detection of X-Ray Line Emission from Type IIn Supernova 1978K with XMM-Newton's RGS

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Takahashi,  K.
Computational Relativistic Astrophysics, AEI-Golm, MPI for Gravitational Physics, Max Planck Society;

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2001.01975.pdf
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Citation

Chiba, Y., Katsuda, S., Yoshida, T., Takahashi, K., & Umeda, H. (2020). First Detection of X-Ray Line Emission from Type IIn Supernova 1978K with XMM-Newton's RGS. Publications of the Astronomical Society of Japan, 72(2): 25. doi:10.1093/pasj/psz148.


Cite as: https://hdl.handle.net/21.11116/0000-0006-B8A8-D
Abstract
We report on robust measurements of elemental abundances of the Type IIn
supernova SN 1978K, based on the high-resolution X-ray spectrum obtained with
the Reflection Grating Spectrometer (RGS) onboard XMM-Newton. The RGS clearly
resolves a number of emission lines, including N Ly$\alpha$, O Ly$\alpha$, O
Ly$\beta$, Fe XVII, Fe XVIII, Ne He$\alpha$ and Ne Ly$\alpha$ for the first
time from SN 1978K. The X-ray spectrum can be represented by an absorbed,
two-temperature thermal emission model, with temperatures of $kT \sim 0.6$ keV
and $2.7$ keV. The elemental abundances are obtained to be N $=$
$2.36_{-0.80}^{+0.88}$, O $=$ $0.20 \pm{0.05}$, Ne $=$ $0.47 \pm{0.12}$, Fe $=$
$0.15_{-0.02}^{+0.01}$ times the solar values. The low metal abundances except
for N show that the X-ray emitting plasma originates from the circumstellar
medium blown by the progenitor star. The abundances of N and O are far from
CNO-equilibrium abundances expected for the surface composition of a luminous
blue variable, and resemble the H-rich envelope of less-massive stars with
masses of 10-25 M$_\odot$. Together with other peculiar properties of SN 1978K,
i.e., a low expansion velocity of 500-1000 km s$^{-1}$ and SN IIn-like optical
spectra, we propose that SN 1978K is a result of either an electron-capture SN
from a super asymptotic giant branch star, or a weak Fe core-collapse explosion
of a relatively low-mass ($\sim$10 M$_\odot$) or high-mass ($\sim$20-25
M$_\odot$) red supergiant star. However, these scenarios can not naturally
explain the high mass-loss rate of the order of $\dot{M} \sim 10^{-3}
\rm{M_{\odot}\ yr^{-1}}$ over $\gtrsim$1000 yr before the explosion, which is
inferred by this work as well as many other earlier studies. Further
theoretical studies are required to explain the high mass-loss rates at the
final evolutionary stages of massive stars.