Table 3.

Quasar candidate at z ∼ 3.3 associated with the QSOP2: HSC J161506 + 423519.*

ParameterValue
RA (J2000.0)16h15m06|${^{\rm s}_{.}}$|24
Dec (J2000.0)+42°35΄19|${^{\prime\prime}_{.}}$|4
g [mag]24.414 ± 0.033
r [mag]22.732 ± 0.008
i [mag]22.272 ± 0.005
z [mag]22.123 ± 0.012
y [mag]22.076 ± 0.025
Ixx   [arcsec2]0.0442
Iyy† [arcsec2]0.0426
(Ixxxx)1.00
(Iyyyy)1.01
ParameterValue
RA (J2000.0)16h15m06|${^{\rm s}_{.}}$|24
Dec (J2000.0)+42°35΄19|${^{\prime\prime}_{.}}$|4
g [mag]24.414 ± 0.033
r [mag]22.732 ± 0.008
i [mag]22.272 ± 0.005
z [mag]22.123 ± 0.012
y [mag]22.076 ± 0.025
Ixx   [arcsec2]0.0442
Iyy† [arcsec2]0.0426
(Ixxxx)1.00
(Iyyyy)1.01

*The HSC magnitudes are extinction-corrected.

Practical adaptive momentum of the object.

Ratio of the object momentum over that of the PSF model: I/ψ. Note that point sources can be extracted with >80% completeness down to i = 23 with (Ixxxx) < 1.1∧(Iyyyy) < 1.1 (see subsection 2.2 of Akiyama et al. 2018).

Table 3.

Quasar candidate at z ∼ 3.3 associated with the QSOP2: HSC J161506 + 423519.*

ParameterValue
RA (J2000.0)16h15m06|${^{\rm s}_{.}}$|24
Dec (J2000.0)+42°35΄19|${^{\prime\prime}_{.}}$|4
g [mag]24.414 ± 0.033
r [mag]22.732 ± 0.008
i [mag]22.272 ± 0.005
z [mag]22.123 ± 0.012
y [mag]22.076 ± 0.025
Ixx   [arcsec2]0.0442
Iyy† [arcsec2]0.0426
(Ixxxx)1.00
(Iyyyy)1.01
ParameterValue
RA (J2000.0)16h15m06|${^{\rm s}_{.}}$|24
Dec (J2000.0)+42°35΄19|${^{\prime\prime}_{.}}$|4
g [mag]24.414 ± 0.033
r [mag]22.732 ± 0.008
i [mag]22.272 ± 0.005
z [mag]22.123 ± 0.012
y [mag]22.076 ± 0.025
Ixx   [arcsec2]0.0442
Iyy† [arcsec2]0.0426
(Ixxxx)1.00
(Iyyyy)1.01

*The HSC magnitudes are extinction-corrected.

Practical adaptive momentum of the object.

Ratio of the object momentum over that of the PSF model: I/ψ. Note that point sources can be extracted with >80% completeness down to i = 23 with (Ixxxx) < 1.1∧(Iyyyy) < 1.1 (see subsection 2.2 of Akiyama et al. 2018).

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