Table 1.
Chandra targets.
| Name | Object | z | FWHM | EW | log L(Lyα) | M1450 |
|---|---|---|---|---|---|---|
| km s−1 | Å | [erg s−1] | mag | |||
| G01 | J142331.71−001809.1 | 6.127 | < 230 | 370 | 44.30 | −21.88 |
| G02 | J084456.62+022640.5 | 6.397 | < 230 | 280 | 44.05 | −21.57 |
| G03 | J093543.32−011033.3 | 6.075 | < 230 | 410 | 44.12 | −21.97 |
| G04 | J125437.08−001410.7 | 6.130 | 310 | 470 | 44.03 | −20.91 |
Notes. Short target names, G01−G04, used in this work are identical to those used in Matsuoka et al. (2025). Object names follow the Subaru HSC survey naming convention and convey right ascension and declination in J2000 co-ordinates for each source. The redshifts shown here are updated values, obtained from the JWST-NIRSpec spectra (Matsuoka et al. 2025). FWHM is the full width at half maximum of Lyα as measured, without correction for absorption of the intergalactic medium. EW is the rest-frame EW of Lyα. M1450 is absolute magnitude at 1450 Å.
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