scholarly journals Recent Hubble Space Telescope Observations of SN 1987A: Broad Emission Lines

2013 ◽  
Vol 9 (S296) ◽  
pp. 1-8
Author(s):  
Kevin France

AbstractObservations with the Hubble Space Telescope (HST), conducted since 1990, have allowed us to create a “movie” of the evolution of the core-collapse supernova SN 1987A from 3–25 years after the explosion. Critical to understanding the late time evolution of SN 1987A was the successful HST Servicing Mission 4 in May 2009. The repair of the STIS instrument and the installation of the WFC3 imager and COS spectrograph have provided crucial data points for understanding the temporal variability in the physical structure and energy sources for SN 1987A, as well as measurements of the chemical abundances of the ejecta. In this proceeding, I will focus on two topics that have made use of the expanded capability of HST and highlight the importance of access to a UV/optical space observatory for the studies of local supernovae: 1) 2) The decreasing maximum velocity of neutral hydrogen crossing the reverse shock front and the role of soft X-ray/EUV heating in the outer supernova debris and 2) The detection of metals (N4+ and C3+ ions) crossing the reverse shock front and CNO processing in the progenitor star.

2012 ◽  
Vol 8 (S290) ◽  
pp. 137-140
Author(s):  
Valério A. R. M. Ribeiro ◽  
Michael F. Bode ◽  
Robert Williams

AbstractThe nebular remnant of RS Ophiuchi was modelled using combined HST/ACS imaging and ground-based spectroscopy on day 155 after outburst as a two component bipolar expansion with a low velocity innermost hour-glass over density and a more extended high velocity dumbbell structure. The model was evolved to a much later date, day 455 after outburst, when second epoch HST images were secured. However, due to the lack of simultaneous ground-based spectroscopy the evolved model was much harder to constrain. One suggestion put forward was that the dumbbell structure expanded linearly while the inner hour-glass showed signs of deceleration. Archival data in the form of ground-based spectroscopy on day 415 were subsequently obtained. These new data suggest indeed that a non-linear expansion of the system occurred.


1995 ◽  
Vol 446 ◽  
pp. 832 ◽  
Author(s):  
J. W. Percival ◽  
P. T. Boyd ◽  
J. D. Biggs ◽  
J. F. Dolan ◽  
R. C. Bless ◽  
...  

2019 ◽  
Vol 487 (3) ◽  
pp. 3815-3844 ◽  
Author(s):  
A F Marino ◽  
A P Milone ◽  
A Renzini ◽  
F D’Antona ◽  
J Anderson ◽  
...  

Abstract The Hubble Space Telescope UV Legacy Survey of Galactic Globular Clusters (GCs) has investigated GCs and their stellar populations. In previous papers of this series we have introduced a pseudo two-colour diagram, or ‘chromosome map’ (ChM) that maximizes the separation between the multiple populations. We have identified two main classes of GCs: Type I, including ∼83 per cent of the objects, and Type II clusters. Both classes host two main groups of stars, referred to in this series as first (1G) and second generation (2G). Type II clusters host more complex ChMs, exhibiting two or more parallel sequences of 1G and 2G stars. We exploit spectroscopic elemental abundances from the literature to assign the chemical composition to the distinct populations as identified on the ChMs of 29 GCs. We find that stars in different regions of the ChM have different compositions: 1G stars share the same light-element content as field stars, while 2G stars are enhanced in N and Na and depleted in O. Stars with enhanced Al, as well as stars with depleted Mg, populate the extreme regions of the ChM. We investigate the intriguing colour spread among 1G stars observed in many Type I GCs, and find no evidence for internal variations in light elements among these stars, whereas either a ∼0.1 dex iron spread or a variation in He among 1G stars remains to be verified. In the attempt of analysing the global properties of the multiple-population phenomenon, we have constructed a universal ChM, which highlights that, though very variegate, the phenomenon has some common pattern among all the analysed GCs. The universal ChM reveals a tight connection with Na abundances, for which we have provided an empirical relation. The additional ChM sequences observed in Type II GCs are enhanced in metallicity and, in some cases, s-process elements. Omega Centauri can be classified as an extreme Type II GC, with a ChM displaying three main extended ‘streams’, each with its own variations in chemical abundances. One of the most noticeable differences is found between the lower and upper streams, with the latter, associated with higher He, being also shifted towards higher Fe and lower Li abundances. We publicly release the ChMs.


1995 ◽  
Vol 452 ◽  
pp. 680 ◽  
Author(s):  
Christopher J. Burrows ◽  
John Krist ◽  
J. Jeff Hester ◽  
Raghvendra Sahai ◽  
John T. Trauger ◽  
...  

2019 ◽  
Vol 886 (2) ◽  
pp. 147 ◽  
Author(s):  
J. Larsson ◽  
C. Fransson ◽  
D. Alp ◽  
P. Challis ◽  
R. A. Chevalier ◽  
...  

2021 ◽  
Vol 921 (1) ◽  
pp. 64
Author(s):  
Peter K. Blanchard ◽  
Edo Berger ◽  
Matt Nicholl ◽  
Ryan Chornock ◽  
Sebastian Gomez ◽  
...  

1995 ◽  
Vol 439 ◽  
pp. 60 ◽  
Author(s):  
P. Ruiz-Lapuente ◽  
R. P. Kirshner ◽  
M. M. Phillips ◽  
P. M. Challis ◽  
B. P. Schmidt ◽  
...  

1996 ◽  
Vol 465 ◽  
pp. 956 ◽  
Author(s):  
S. Scuderi ◽  
N. Panagia ◽  
R. Gilmozzi ◽  
P. M. Challis ◽  
R. P. Kirshner

1993 ◽  
Vol 155 ◽  
pp. 411-411
Author(s):  
H. Gratl ◽  
J. Pfleiderer

Modelling of PNs from blurred images, as from the Hubble Space Telescope, needs good deconvolution, and the better that is, the more reliable are the results. As an example, we have MIM-deconvolved the HST image of SN 1987A taken in August 1990 by the FOC in [O III] λ5007 Å (F501N). MIM (minimum information method) is a linear deconvolution method with a local smoothness constraint (Pfleiderer 1991). Our results are similar to those already published (Jakobson et al. 1991, Panagia et al. 1991) but we were able to decrease some of the uncertainties. The ring, centered on the SN, has diameter 1680 ± 20 mas (≡ 1.3 ly) and tilt 44.5°±1.5° (Fig 1.). The lumps deviate from the ellipse by up to ≤ 0.05 ly, the ratio of brightest to faintest knots being ≈ 10 (Fig.3). The SN is resolved (Fig.2), being not a uniformly illuminated disk but brighter in the center. Its FWHM is 100 ± 10 mas, i.e. an average expansion velocity since the explosion of v ≈ 3 500 km s−1.


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