4.6 Article

Kinematics, structure and abundances of supernova remnant 0540-69.3

期刊

ASTRONOMY & ASTROPHYSICS
卷 658, 期 -, 页码 -

出版社

EDP SCIENCES S A
DOI: 10.1051/0004-6361/202141931

关键词

ISM; supernova remnants; supernovae; general; pulsars; individual

资金

  1. Swedish Research Council
  2. Wallenberg Foundation
  3. Swedish Institute
  4. Russian Foundation for Basic Research (RFBR) [19-52-12013]

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The aim of this study is to investigate the structure, elemental abundances, physical conditions, and surroundings of supernova remnant 0540-69.3 in the Large Magellanic Cloud. Imaging and spectroscopic studies were conducted using telescopes of the European Southern Observatory. The results reveal new spectral lines, estimate densities, temperatures, and abundances, and provide insights into the characteristics of the remnant.
Aims. Our goal is to investigate the structure, elemental abundances, physical conditions, and the immediate surroundings of supernova remnant 0540-69.3 in the Large Magellanic Cloud. Methods. Imaging in [O III] and spectroscopic studies through various slits were carried out using European Souther Observatory's Very Large and New Technology Telescopes. Densities, temperatures, and abundances were estimated applying nebular analysis for various parts of the remnant. Results. Several new spectral lines are identified, both from ejecta embedded in the pulsar-wind nebula, and in interstellar clouds shocked by the supernova blast wave. For the filaments in the pulsar-wind nebula, all lines are redshifted by 440 +/- 80kms(-1) with respect to the rest frame of the host galaxy, and a 3D representation of the [O III] emission displays a symmetry axis of ring-like structures which could indicate that the pulsar shares the same general redshift as the central supernova ejecta. We note that [O II], [S II], [Ar III], and H beta share a common more compact structure than [O III], and possibly [Ne III]. The average [O III] temperature for the filaments in the pulsar-wind nebula is 23500 +/- 1800 K, and the electron density derived from [S II] is typically similar to 10(3) cm(-3). By mass, the relative elemental abundances of the shocked ejecta in the pulsar-wind nebula are O:Ne:S:Ar approximate to 1:0.07:0.10:0.02, consistent with explosion models of 13 - 20M(circle dot) progenitors, and similar to that of SN 1987A, as is also the explosive mixing of hydrogen and helium into the center. From H beta and He I lambda 5876, the mass ratio of He/H in the center is estimated to be in excess of similar to 0.8. The rapid cooling of the shocked ejecta could potentially cause variations in the relative abundances if the ejecta are not fully microscopically mixed, and this is highlighted for S/O for the period 1989-2006. Also, [O III] is seen in presumably freely coasting photoionized ejecta outside the pulsar-wind nebula at inferred velocities out to well above 2000kms(-1), and in projection, [O III] is seen out to similar to 10 '' from the pulsar. This was used to estimate that the pulsar age is approximate to 1200 years. The freely coasting [O III]-emitting ejecta have a strictly nonspherical distribution, and their mass is estimated to be similar to 0.12M(circle dot). A possible outer boundary of oxygen-rich ejecta is seen in [O II] lambda lambda 3726,3729 at similar to 2000 - 2100kms(-1). Four filaments of a shocked interstellar medium are identified, and there is a wide range in the degree of ionization of iron, from Fe+ to Fe13+. One filament belongs to a region also observed in X-rays, and another one has a redshift of 85 +/- 30kms(-1) relative to the host. From this we estimate that the electron density of the [O III]-emitting gas is similar to 10(3) cm(-3), and that the line of the most highly ionized ion, [Fe XIV] lambda 5303, comes from an evaporation zone in connection with the radiatively cooled gas emitting, for example, [O III], and not from immediately behind the blast wave. We do not find evidence for nitrogen-enriched ejecta in the southwestern part of the remnant, as was previously suggested. Emission in this region is instead from a severely reddened H II-region.

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