The Astrophysical Journal (Jan 2023)

MIDIS: Strong (Hβ+[O iii]) and Hα Emitters at Redshift z ≃ 7–8 Unveiled with JWST NIRCam and MIRI Imaging in the Hubble eXtreme Deep Field

  • P. Rinaldi,
  • K. I. Caputi,
  • L. Costantin,
  • S. Gillman,
  • E. Iani,
  • P. G. Pérez-González,
  • G. Östlin,
  • L. Colina,
  • T. R. Greve,
  • H. U. Noorgard-Nielsen,
  • G. S. Wright,
  • A. Alonso-Herrero,
  • J. Álvarez-Márquez,
  • A. Eckart,
  • M. García-Marín,
  • J. Hjorth,
  • O. Ilbert,
  • S. Kendrew,
  • A. Labiano,
  • O. Le Fèvre,
  • J. Pye,
  • T. Tikkanen,
  • F. Walter,
  • P. van der Werf,
  • M. Ward,
  • M. Annunziatella,
  • R. Azzollini,
  • A. Bik,
  • L. Boogaard,
  • S. E. I. Bosman,
  • A. Crespo Gómez,
  • I. Jermann,
  • D. Langeroodi,
  • J. Melinder,
  • R. A. Meyer,
  • T. Moutard,
  • F. Peissker,
  • M. Topinka,
  • E. van Dishoeck,
  • M. Güdel,
  • Th. Henning,
  • P.-O. Lagage,
  • T. Ray,
  • B. Vandenbussche,
  • C. Waelkens,
  • R. Navarro-Carrera,
  • V. Kokorev

DOI
https://doi.org/10.3847/1538-4357/acdc27
Journal volume & issue
Vol. 952, no. 2
p. 143

Abstract

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We make use of JWST medium-band and broadband NIRCam imaging, along with ultradeep MIRI 5.6 μ m imaging, in the Hubble eXtreme Deep Field to identify prominent line emitters at z ≃ 7–8. Out of a total of 58 galaxies at z ≃ 7–8, we find 18 robust candidates (≃31%) for (H β + [O iii ]) emitters, based on their enhanced fluxes in the F430M and F444W filters, with EW _0 (H β +[O iii ]) ≃87–2100 Å. Among these emitters, 16 lie in the MIRI coverage area and 12 exhibit a clear flux excess at 5.6 μ m, indicating the simultaneous presence of a prominent H α emission line with EW _0 (H α ) ≃200–3000 Å. This is the first time that H α emission can be detected in individual galaxies at z > 7. The H α line, when present, allows us to separate the contributions of H β and [O iii ] to the (H β +[O iii ]) complex and derive H α -based star formation rates (SFRs). We find that in most cases [O iii ]/H β > 1. Instead, two galaxies have [O iii ]/H β < 1, indicating that the NIRCam flux excess is mainly driven by H β . Most prominent line emitters are very young starbursts or galaxies on their way to/from the starburst cloud. They make for a cosmic SFR density ${\mathrm{log}}_{10}({\rho }_{{\mathrm{SFR}}_{{\rm{H}}\alpha }}/({M}_{\odot }\,{\mathrm{yr}}^{-1}\,{\mathrm{Mpc}}^{-3}))\simeq -2.35$ , which is about a quarter of the total value ( ${\mathrm{log}}_{10}({\rho }_{{\mathrm{SFR}}_{\mathrm{tot}}}/({M}_{\odot }\,{\mathrm{yr}}^{-1}\,{\mathrm{Mpc}}^{-3}))\simeq -1.76$ ) at z ≃ 7–8. Therefore, the strong H α emitters likely had a significant role in reionization.

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