The Electromagnetic Counterpart of the Binary Neutron Star Merger LIGO/Virgo GW170817. II. UV, Optical, and Near-infrared Light Curves and Comparison to Kilonova Models
The Electromagnetic Counterpart of the Binary Neutron Star Merger LIGO/Virgo GW170817. II. UV, Optical, and Near-infrared Light Curves and Comparison to Kilonova Models
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DOI:
10.3847/2041-8213/aa8fc7
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发表时间:
2017-10
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通讯作者:
P. Cowperthwaite;E. Berger;V. Villar;B. Metzger;M. Nicholl;R. Chornock;P. Blanchard;W. Fong;R. Margutti;M. Soares-Santos;K. Alexander;S. Allam;J. Annis;D. Brout;D. Brown;R. Butler;H.-Y. Chen;H. Diehl;Zoheyr Doctor;M. Drout;T. Eftekhari;B. Farr;D. Finley;R. Foley;J. Frieman;C. Fryer;J. Garc'ia-Bellido;M. Gill;J. Guillochon;K. Herner;D. Holz;D. Kasen;R. Kessler;J. Marriner;T. Matheson;E. Neilsen;Jr.;E. Quataert;A. Palmese;A. Rest;M. Sako;D. Scolnic;N. Smith;D. Tucker;P. G. Williams;E. Balbinot;J. Carlin;E. Cook;F. Durret;T. Li;P. Lopes;A. C. Lourencco;J. Marshall;G. Medina;J. Muir;R. Muñoz;M. Sauseda;D. Schlegel;L. Secco;A. K. Vivas;W. Wester;A. Zenteno;Y. Zhang;T. Abbott;M. Banerji;K. Bechtol;A. Benoit-Lévy;E. Bertin;E. Buckley-Geer;D. Burke;D. Capozzi;A. Rosell;M. Kind;F. Castander;M. Crocce;C. Cunha;C. D'Andrea;L. Costa;C. Davis;D. Depoy;S. Desai;J. Dietrich;A. Drlica-Wagner;T. Eifler;A. Evrard;E. Fernández;B. Flaugher;P. Fosalba;E. Gaztañaga;D. Gerdes;T. Giannantonio;D. Goldstein;D. Gruen;R. Gruendl;G. Gutiérrez;K. Honscheid;B. Jain;D. James;T. Jeltema;M. Johnson;M. Johnson;S. Kent;E. Krause;R. Kron;K. Kuehn;N. Kuropatkin;O. Lahav;M. Lima;H. Lin;M. Maia;M. March;P. Martini;R. McMahon;F. Menanteau;C. Miller;R. Miquel;J. Mohr;E. Neilsen;R. Nichol;R. Ogando;A. Plazas;N. Roe;A. Romer;A. Roodman;E. Rykoff;E. Sánchez;V. Scarpine;R. Schindler;M. Schubnell;I. Sevilla-Noarbe;M. Smith;R. C. Smith;F. Sobreira;E. Suchyta;M. Swanson;G. Tarlé;D. Thomas;R. Thomas;M. Troxel;V. Vikram;A. Walker;R. Wechsler;J. Weller;B. Yanny;J. Zuntz
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作者:
P. Cowperthwaite;E. Berger;V. Villar;B. Metzger;M. Nicholl;R. Chornock;P. Blanchard;W. Fong;R. Margutti;M. Soares-Santos;K. Alexander;S. Allam;J. Annis;D. Brout;D. Brown;R. Butler;H.-Y. Chen;H. Diehl;Zoheyr Doctor;M. Drout;T. Eftekhari;B. Farr;D. Finley;R. Foley;J. Frieman;C. Fryer;J. Garc'ia-Bellido;M. Gill;J. Guillochon;K. Herner;D. Holz;D. Kasen;R. Kessler;J. Marriner;T. Matheson;E. Neilsen;Jr.;E. Quataert;A. Palmese;A. Rest;M. Sako;D. Scolnic;N. Smith;D. Tucker;P. G. Williams;E. Balbinot;J. Carlin;E. Cook;F. Durret;T. Li;P. Lopes;A. C. Lourencco;J. Marshall;G. Medina;J. Muir;R. Muñoz;M. Sauseda;D. Schlegel;L. Secco;A. K. Vivas;W. Wester;A. Zenteno;Y. Zhang;T. Abbott;M. Banerji;K. Bechtol;A. Benoit-Lévy;E. Bertin;E. Buckley-Geer;D. Burke;D. Capozzi;A. Rosell;M. Kind;F. Castander;M. Crocce;C. Cunha;C. D'Andrea;L. Costa;C. Davis;D. Depoy;S. Desai;J. Dietrich;A. Drlica-Wagner;T. Eifler;A. Evrard;E. Fernández;B. Flaugher;P. Fosalba;E. Gaztañaga;D. Gerdes;T. Giannantonio;D. Goldstein;D. Gruen;R. Gruendl;G. Gutiérrez;K. Honscheid;B. Jain;D. James;T. Jeltema;M. Johnson;M. Johnson;S. Kent;E. Krause;R. Kron;K. Kuehn;N. Kuropatkin;O. Lahav;M. Lima;H. Lin;M. Maia;M. March;P. Martini;R. McMahon;F. Menanteau;C. Miller;R. Miquel;J. Mohr;E. Neilsen;R. Nichol;R. Ogando;A. Plazas;N. Roe;A. Romer;A. Roodman;E. Rykoff;E. Sánchez;V. Scarpine;R. Schindler;M. Schubnell;I. Sevilla-Noarbe;M. Smith;R. C. Smith;F. Sobreira;E. Suchyta;M. Swanson;G. Tarlé;D. Thomas;R. Thomas;M. Troxel;V. Vikram;A. Walker;R. Wechsler;J. Weller;B. Yanny;J. Zuntz
We present UV, optical, and near-infrared (NIR) photometry of the first electromagnetic counterpart to a gravitational wave source from Advanced Laser Interferometer Gravitational-wave Observatory (LIGO)/Virgo, the binary neutron star merger GW170817. Our data set extends from the discovery of the optical counterpart at 0.47–18.5 days post-merger, and includes observations with the Dark Energy Camera (DECam), Gemini-South/FLAMINGOS-2 (GS/F2), and the Hubble Space Telescope (HST). The spectral energy distribution (SED) inferred from this photometry at 0.6 days is well described by a blackbody model with T ≈ 8300 K, a radius of R ≈ 4.5 × 10 14 cm (corresponding to an expansion velocity of v ≈ 0.3 c ), and a bolometric luminosity of L bol ≈ 5 × 10 41 erg s−1. At 1.5 days we find a multi-component SED across the optical and NIR, and subsequently we observe rapid fading in the UV and blue optical bands and significant reddening of the optical/NIR colors. Modeling the entire data set, we find that models with heating from radioactive decay of 56Ni, or those with only a single component of opacity from r-process elements, fail to capture the rapid optical decline and red optical/NIR colors. Instead, models with two components consistent with lanthanide-poor and lanthanide-rich ejecta provide a good fit to the data; the resulting “blue” component has M ej blue ≈ 0.01 M ⊙ and v ej blue ≈ 0.3 c , and the “red” component has M ej red ≈ 0.04 M ⊙ and v ej red ≈ 0.1 c . These ejecta masses are broadly consistent with the estimated r-process production rate required to explain the Milky Way r-process abundances, providing the first evidence that binary neutron star (BNS) mergers can be a dominant site of r-process enrichment.