Polarized kilonovae from black hole–neutron star mergers

Author:

Bulla M1ORCID,Kyutoku K234ORCID,Tanaka M5ORCID,Covino S6,Bruten J R7,Matsumoto T8910,Maund J R7ORCID,Testa V11ORCID,Wiersema K1213

Affiliation:

1. Nordita, KTH Royal Institute of Technology and Stockholm University, Roslagstullsbacken 23, SE-106 91 Stockholm, Sweden

2. Department of Physics, Kyoto University, Kyoto 606-8502, Japan

3. Center for Gravitational Physics, Yukawa Institute for Theoretical Physics, Kyoto University, Kyoto 606-8502, Japan

4. Interdisciplinary Theoretical and Mathematical Sciences Program (iTHEMS), RIKEN, Wako, Saitama 351-0198, Japan

5. Astronomical Institute, Tohoku University, Sendai 980-8578, Japan

6. Istituto Nazionale di Astrofisica / Brera Astronomical Observatory, via Bianchi 46, I-23807 Merate (LC), Italy

7. Department of Physics and Astronomy, University of Sheffield, Hicks Building, Hounsfield Road, Sheffield S3 7RH, UK

8. Racah Institute of Physics, Hebrew University, Jerusalem 91904, Israel

9. Research Center for the Early Universe, Graduate School of Science, University of Tokyo, Tokyo 113-0033, Japan

10. Department of Physics, Graduate School of Science, University of Tokyo, Tokyo 113-0033, Japan

11. Istituto Nazionale di Astrofisica/Osservatorio Astronomico di Roma, Monte Porzio Catone 00078, Italy

12. Department of Physics, University of Warwick, Coventry CV4 7AL, UK

13. School of Physics and Astronomy, University of Leicester, University Road, Leicester LE1 7RH, UK

Abstract

ABSTRACT We predict linear polarization for a radioactively powered kilonova following the merger of a black hole and a neutron star. Specifically, we perform 3D Monte Carlo radiative transfer simulations for two different models, both featuring a lanthanide-rich dynamical ejecta component from numerical-relativity simulations while only one including an additional lanthanide-free disc-wind component. We calculate polarization spectra for nine different orientations at 1.5, 2.5, and 3.5 d after the merger and in the $0.1\!-\!2\, \mu$m wavelength range. We find that both models are polarized at a detectable level 1.5 d after the merger while show negligible levels thereafter. The polarization spectra of the two models are significantly different. The model lacking a disc wind shows no polarization in the optical, while a signal increasing at longer wavelengths and reaching $\sim 1\!-\!6{{\ \rm per\ cent}}$ at $2\, \mu$m depending on the orientation. The model with a disc-wind component, instead, features a characteristic ‘double-peak’ polarization spectrum with one peak in the optical and the other in the infrared. Polarimetric observations of future events will shed light on the debated neutron richness of the disc-wind component. The detection of optical polarization would unambiguously reveal the presence of a lanthanide-free disc-wind component, while polarization increasing from zero in the optical to a peak in the infrared would suggest a lanthanide-rich composition for the whole ejecta. Future polarimetric campaigns should prioritize observations in the first ∼48 h and in the $0.5\!-\!2\, \mu$m range, where polarization is strongest, but also explore shorter wavelengths/later times where no signal is expected from the kilonova and the interstellar polarization can be safely estimated.

Funder

JSPS

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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