{ "id": "2009.07279", "version": "v1", "published": "2020-09-15T18:00:01.000Z", "updated": "2020-09-15T18:00:01.000Z", "title": "Polarized kilonovae from black hole-neutron star mergers", "authors": [ "M. Bulla", "K. Kyutoku", "M. Tanaka", "S. Covino", "J. R. Bruten", "T. Matsumoto", "J. R. Maund", "V. Testa", "K. Wiersema" ], "comment": "8 pages, 4 figures; to be submitted to MNRAS; comments are welcome", "categories": [ "astro-ph.HE" ], "abstract": "We predict linear polarization for a radioactively-powered kilonova following the merger of a black hole and a neutron star. Specifically, we perform 3-D 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 disk 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 disk wind shows no polarization in the optical, while a signal increasing at longer wavelengths and reaching $\\sim1\\%-6\\%$ at $2\\,\\mu$m depending on the orientation. The model with a disk-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 disk-wind component. The detection of optical polarization would unambiguously reveal the presence of a lanthanide-free disk-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 $\\sim48$ hours 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.", "revisions": [ { "version": "v1", "updated": "2020-09-15T18:00:01.000Z" } ], "analyses": { "keywords": [ "black hole-neutron star mergers", "polarized kilonovae", "carlo radiative transfer simulations", "polarization spectrum", "disk-wind component" ], "note": { "typesetting": "TeX", "pages": 8, "language": "en", "license": "arXiv", "status": "editable" } } }