Abstract

We performed a deep optical imaging survey using a narrow-band filter (NB921) centered at |$\lambda = 9196 \,$|Å together with |$i^\prime$| and |$z^\prime$| broadband filters covering an |$814 \,\mathrm{arcmin}^2$| area of the Subaru Deep Field. We obtained a sample of 73 strong NB921-excess objects based on the following two color criteria:|$z^\prime-\mathit{NB}\,921 \gt 1$||$z^\prime-\mathit{NB}\,921 \gt 1$| and |$i^\prime-z^\prime \gt 1.3$||$i^\prime-z^\prime \gt 1.3$|⁠. We then obtained optical spectroscopy of nine objects in our NB921-excess sample, and identified at least two Ly|$\alpha$| emitters at |$z=6.541 \pm 0.002$| and |$z=6.578 \pm 0.002$|⁠, each of which shows the characteristic sharp cutoff together with continuum depression at wavelengths shortward of the line peak. The latter object is more distant than HCM-6A at |$z=6.56$|⁠, which is the most distant known object that has been found so far. These new data allow us to estimate the first meaningful lower limit of the star-formation rate density beyond redshift 6; |$\rho_\mathrm{SFR} \sim 5.2 \times 10^{-4} \,{{{M}_{\odot}}} \,\mathrm{yr}^{-1} \,\mathrm{Mpc}^{-3}$|⁠. Since it is expected that the actual density is several times higher than this value, our new observation reveals that a moderately high level of star formation activity already occurred at |$z \sim 6.6$|⁠.

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