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. 2024 Feb;626(8000):737-741.
doi: 10.1038/s41586-023-06759-1. Epub 2023 Oct 25.

Heavy-element production in a compact object merger observed by JWST

Andrew J Levan  1   2 Benjamin P Gompertz  3   4 Om Sharan Salafia  5   6 Mattia Bulla  7   8   9 Eric Burns  10 Kenta Hotokezaka  11   12 Luca Izzo  13   14 Gavin P Lamb  15   16 Daniele B Malesani  17   18   19 Samantha R Oates  3   4 Maria Edvige Ravasio  17   5 Alicia Rouco Escorial  20 Benjamin Schneider  21 Nikhil Sarin  22   23 Steve Schulze  23 Nial R Tanvir  16 Kendall Ackley  24 Gemma Anderson  25 Gabriel B Brammer  18   19 Lise Christensen  18   19 Vikram S Dhillon  26   27 Phil A Evans  16 Michael Fausnaugh  21   28 Wen-Fai Fong  29   30 Andrew S Fruchter  31 Chris Fryer  32   33   34   35 Johan P U Fynbo  18   19 Nicola Gaspari  17 Kasper E Heintz  18   19 Jens Hjorth  13 Jamie A Kennea  36 Mark R Kennedy  37   38 Tanmoy Laskar  17   39 Giorgos Leloudas  40 Ilya Mandel  41   42 Antonio Martin-Carrillo  43 Brian D Metzger  44   45 Matt Nicholl  46 Anya Nugent  29   30 Jesse T Palmerio  47 Giovanna Pugliese  48 Jillian Rastinejad  29   30 Lauren Rhodes  49 Andrea Rossi  50 Andrea Saccardi  47 Stephen J Smartt  46   49 Heloise F Stevance  49   51 Aaron Tohuvavohu  52 Alexander van der Horst  35 Susanna D Vergani  47 Darach Watson  18   19 Thomas Barclay  53 Kornpob Bhirombhakdi  31 Elmé Breedt  54 Alice A Breeveld  55 Alexander J Brown  26 Sergio Campana  5 Ashley A Chrimes  17 Paolo D'Avanzo  5 Valerio D'Elia  56   57 Massimiliano De Pasquale  58 Martin J Dyer  26 Duncan K Galloway  41   42 James A Garbutt  26 Matthew J Green  59 Dieter H Hartmann  60 Páll Jakobsson  61 Paul Kerry  26 Chryssa Kouveliotou  35 Danial Langeroodi  13 Emeric Le Floc'h  62 James K Leung  42   63   64 Stuart P Littlefair  26 James Munday  24   65 Paul O'Brien  16 Steven G Parsons  26 Ingrid Pelisoli  24 David I Sahman  26 Ruben Salvaterra  66 Boris Sbarufatti  5 Danny Steeghs  24   42 Gianpiero Tagliaferri  5 Christina C Thöne  67 Antonio de Ugarte Postigo  68 David Alexander Kann  69
Affiliations

Heavy-element production in a compact object merger observed by JWST

Andrew J Levan et al. Nature. 2024 Feb.

Abstract

The mergers of binary compact objects such as neutron stars and black holes are of central interest to several areas of astrophysics, including as the progenitors of gamma-ray bursts (GRBs)1, sources of high-frequency gravitational waves (GWs)2 and likely production sites for heavy-element nucleosynthesis by means of rapid neutron capture (the r-process)3. Here we present observations of the exceptionally bright GRB 230307A. We show that GRB 230307A belongs to the class of long-duration GRBs associated with compact object mergers4-6 and contains a kilonova similar to AT2017gfo, associated with the GW merger GW170817 (refs. 7-12). We obtained James Webb Space Telescope (JWST) mid-infrared imaging and spectroscopy 29 and 61 days after the burst. The spectroscopy shows an emission line at 2.15 microns, which we interpret as tellurium (atomic mass A = 130) and a very red source, emitting most of its light in the mid-infrared owing to the production of lanthanides. These observations demonstrate that nucleosynthesis in GRBs can create r-process elements across a broad atomic mass range and play a central role in heavy-element nucleosynthesis across the Universe.

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Conflict of interest statement

The authors declare no competing interests.

Figures

Fig. 1
Fig. 1. The high-energy properties of GRB 230307A.
a, The light curve of the GRB at 64-ms time resolution with the Fermi/GBM. The shaded region indicates the region in which saturation may be an issue. The burst begins very hard, with the count rate dominated by photons in the hardest (100–900-keV) band, but rapidly softens, with the count rate in the hard band being progressively overtaken by softer bands (such as 8–25 keV and 25–100 keV) beyond about 20 s. This strong hard-to-soft evolution is reminiscent of GRB 211211A (ref. ) and is caused by the motion of two spectral breaks through the gamma-ray regime (see Methods). b, The X-ray light curves of GRBs from the Swift X-ray telescope. These have been divided by the prompt fluence of the burst, which broadly scales with the X-ray light curve luminosity, resulting in a modest spread of afterglows. The greyscale background represents the ensemble of long GRBs. GRB 230307A is an extreme outlier of the >1,000 Swift GRBs, with an extremely faint afterglow for the brightness of its prompt emission. Other merger GRBs from long bursts, and those suggested to be short with extended emission (EE), occupy a similar region of the parameter space. This suggests that the prompt to afterglow fluence could be a valuable tool in distinguishing long GRBs from mergers and those from supernovae.
Fig. 2
Fig. 2. JWST images of GRB 230307A at 28.5 days post burst.
a, The wide-field image combining the F115W, F150W and F444W images. The putative host is the bright face-on spiral galaxy, whereas the afterglow appears at a 30-arcsec offset, within the white box. The scale bar at the lower left represents 10″. bg, Cut-outs of the NIRCam data around the GRB afterglow location. The source is faint and barely detected in the bluer bands but very bright and well detected in the red bands. In the red bands, a faint galaxy is present northeast of the transient position. This galaxy has a redshift of z = 3.87 but we consider it to be a background object unrelated to the GRB (see Supplementary Information).
Fig. 3
Fig. 3. JWST/NIRSpec spectroscopy of the counterpart of GRB 230307A.
The top portion shows the 2D spectrum rectified to a common wavelength scale. The transient is well detected beyond 2 microns but not shortward, indicative of an extremely red source. Emission lines from the nearby galaxy at z = 3.87 can also be seen offset from the afterglow trace. The lower panel shows the 1D extraction of the spectrum in comparison with the latest (10-day) AT2017gfo epoch and a kilonova model. A clear emission feature can be seen at about 2.15 microns at both 29 and 61 days. This feature is consistent with the expected location of [Te III], whereas redder features are compatible with lines from [Se III] and [W III]. This line is also clearly visible in the scaled late-time spectrum of AT2017gfo (refs. ,), whereas the red colours are also comparable with those of AT2017gfo as measured with Spitzer (ref. ; shown scaled to the 29-day NIRSpec spectrum). Error bars on photometry refer to the 1σ error bar on the y axis and the filter width on the x axis.
Fig. 4
Fig. 4. A comparison of the counterpart of GRB 230307A with AT2017gfo associated with GW170817.
AT2017gfo has been scaled to the same distance as GRB 230307A. Beyond about 2 days, the kilonova dominates the counterpart. The decay rates in both the optical and infrared are very similar to those in AT2017gfo. These are too rapid for any plausible afterglow model. There is also good agreement in the late-time slope between the measurements made at 4.4 microns with the JWST and at 4.5 microns for AT2017gfo with Spitzer. Error bars refer to the 1σ uncertainty.

References

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