اشترك بالحزمة الذهبية واحصل على وصول غير محدود شمرا أكاديميا
تسجيل مستخدم جديدClumps and rings of ejecta in SNR 0540-69.3 as seen in 3D
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The distribution of ejecta in young supernova remnants offers a powerful observational probe of their explosions and progenitors. Here we present a 3D reconstruction of the ejecta in SNR 0540-69.3, which is an O-rich remnant with a pulsar wind nebula located in the LMC. We use observations from VLT/MUSE to study Hbeta, [O III] lambda lambda 4959, 5007, Halpha, [S II] lambda lambda 6717, 6731, [Ar III] lambda 7136 and [S III] lambda 9069 emission lines. This is complemented by 2D spectra from VLT/X-shooter, which also cover [O II] lambda lambda 3726, 3729 and [Fe II] lambda 12567. We identify three main emission components: (i) Clumpy rings in the inner nebula (<1000 km/s) with similar morphologies in all lines; (ii) Faint extended [O III] emission dominated by an irregular ring-like structure with radius ~1600 km/s and inclination ~40 dg, but with maximal velocities reaching ~3000 km/s; and (iii) A blob of Halpha and Hbeta located southeast of the pulsar at velocities ~1500-3500 km/s. We analyze the geometry using a clump-finding algorithm and use the clumps in the [O III] ring to estimate an age of 1146 pm 116 years. The observations favor an interpretation of the [O III] ring as ejecta, while the origin of the H-blob is more uncertain. An alternative explanation is that it is the blown-off envelope of a binary companion. From the detection of Balmer lines in the innermost ejecta we confirm that SNR 0540 was a Type II supernova and that hydrogen was mixed down to low velocities in the explosion.
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We present observations of the pulsar-wind nebula (PWN) region ofSNR 0540-69.3. The observations were made with the Atacama Compact Array (ACA) in Bands 4 and 6. We also add radio observations from the Australia Compact Array (ATCA) at 3 cm. For 1.44
9 - 233.50 GHz we obtain a synchrotron spectrum $F_{ u} propto u^{-alpha_{ u}}$, with the spectral index $alpha_{ u} = 0.17pm{0.02}$. To conclude how this joins the synchrotron spectrum at higher frequencies we include hitherto unpublished AKARI mid-infrared data, and evaluate published data in the ultraviolet (UV), optical and infrared (IR). In particular, some broad-band filter data in the optical must be discarded from our analysis due to contamination by spectral line emission. For the UV/IR part of the synchrotron spectrum, we arrive at $alpha_{ u} = 0.87^{+0.08}_{-0.10}$. There is room for $2.5times10^{-3}$ solar masses of dust with temperature $sim 55$ K if there are dual breaks in the synchrotron spectrum, one around $sim 9times10^{10}$ Hz, and another at $sim 2times10^{13}$ Hz. The spectral index then changes at $sim 9times10^{10}$ Hz from $alpha_{ u} = 0.14pm0.07$ in the radio, to $alpha_{ u} = 0.35^{-0.07}_{+0.05}$ in the millimetre to far-IR range. The ACA Band 6 data marginally resolves the PWN. In particular, the strong emission 1.5 south-west of the pulsar, seen at other wavelengths, and resolved in the 3-cm data with its 0.8 spatial resolution, is also strong in the millimeter range. The ACA data clearly reveal the supernova remnant shell 20-35 arcsec west of the pulsar, and for the shell we derive $alpha_{ u} = 0.64pm{0.05}$ for the range $8.6-145$~GHz.
The structure, elemental abundances, physical conditions of the LMC supernova remnant (SNR) 0540-69.3 and its surroundings were investigated using [O III] imaging and spectroscopy. Several new spectral lines are identified, both in central filaments
and in interstellar clouds shocked by the supernova blast wave. The central lines are redshifted by $440pm80$ km s$^{-1}$ with respect to the LMC, and 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. [O II], [S II], [Ar III] and H$beta$ have more compact structures than [O III], and possibly [Ne III]. The average [O III] temperature is $23,500 pm 1,800$ K, and the electron density from [S II] is typically $10^3$ cm$^{-3}$. By mass, the relative elemental abundances of the central shocked ejecta are ${rm O:Ne:S:Ar} approx 1:0.07:0.10:0.02$, consistent with explosion models of $13-20$ solar mass progenitors, and similar to that of SN 1987A, as is also the mixing of hydrogen and helium into the center. [O III] is also seen in freely coasting ejecta outside the pulsar-wind nebula out to well above $2,000$ km s$^{-1}$. From this a pulsar age of $approx 1,200$ years is estimated. Four filaments of shocked interstellar medium with a wide range in degree of ionization of iron are identified. One was observed in X-rays, and another has a redshift of $85pm30$ km~s$^{-1}$ relative to LMC. From this the electron density of the [O III]-emitting gas is estimated to be $10^3$ cm$^{-3}$. The line of the most highly ionized ion, [Fe XIV] $lambda$5303, likely comes from an evaporation zone in connection with the radiatively cooled gas emitting, e.g., [O III].
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We have used the ESO NTT/EMMI and VLT/FORS1 instruments to examine the LMC supernova remnant 0540-69.3 as well as its pulsar (PSR B0540-69) and pulsar-powered nebula in the optical range.Spectroscopic observations of the remnant covering the range of
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