Table 4.

Spectral parameters of optical Fe ii blend and [O iii].

Power lawOptical Fe ii[O iii] λλ5007, λ4959 a
ObjectRedshiftf1000αScaleFWHMFluxFWHMCentroid
0809+27531.51112.70 ± 0.021.36 ± 0.010.258 ± 0.0233478 ± 7803.05 ± 0.09791 ± 75013 ± 0.02
1031+39531.08211.70 ± 0.291.35 ± 0.010.288 ± 0.01690004.09 ± 0.091730 ± 15000 ± 0.06
1044+36560.7015.63 ± 0.041.51 ± 0.010.094 ± 0.0032672 ± 18  
1312+23191.5083.18 ± 0.121.43 ± 0.020.091 ± 0.0033958 ± 1140.04 ± 0.061029 ± 105010 ± 0.14
1324+24522.3570.99 ± 0.041.60 ± 0.020.002 ± 0.0012777 ± 47  0.89 ± 0.122025 ± 3175000
1408+30540.8423.74 ± 0.261.46 ± 0.040.128 ± 0.0122505 ± 117
1427+27091.1702.85 ± 0.051.58 ± 0.020.017 ± 0.00510003.42 ± 2.793957 ± 7795007 ± 0.93
1523+39140.6570.21 ± 0.010.63 ± 0.010.056 ± 0.0047678 ± 2   
Composite17.90 ± 0.451.63 ± 0.010.233 ± 0.0082474 ± 1   0.65 ± 0.85852 ± 225006 ± 0.09
FBQS composite0.78 ± 0.010.12 ± 0.010.069 ± 0.0013786 ± 57  32.83 ± 0.06739 ± 15006 ± 0.01
PG composite15.38 ± 0.131.64 ± 0.000.194 ± 0.0013602 ± 57  4.18 ± 0.08811 ± 195006 ± 0.15
Power lawOptical Fe ii[O iii] λλ5007, λ4959 a
ObjectRedshiftf1000αScaleFWHMFluxFWHMCentroid
0809+27531.51112.70 ± 0.021.36 ± 0.010.258 ± 0.0233478 ± 7803.05 ± 0.09791 ± 75013 ± 0.02
1031+39531.08211.70 ± 0.291.35 ± 0.010.288 ± 0.01690004.09 ± 0.091730 ± 15000 ± 0.06
1044+36560.7015.63 ± 0.041.51 ± 0.010.094 ± 0.0032672 ± 18  
1312+23191.5083.18 ± 0.121.43 ± 0.020.091 ± 0.0033958 ± 1140.04 ± 0.061029 ± 105010 ± 0.14
1324+24522.3570.99 ± 0.041.60 ± 0.020.002 ± 0.0012777 ± 47  0.89 ± 0.122025 ± 3175000
1408+30540.8423.74 ± 0.261.46 ± 0.040.128 ± 0.0122505 ± 117
1427+27091.1702.85 ± 0.051.58 ± 0.020.017 ± 0.00510003.42 ± 2.793957 ± 7795007 ± 0.93
1523+39140.6570.21 ± 0.010.63 ± 0.010.056 ± 0.0047678 ± 2   
Composite17.90 ± 0.451.63 ± 0.010.233 ± 0.0082474 ± 1   0.65 ± 0.85852 ± 225006 ± 0.09
FBQS composite0.78 ± 0.010.12 ± 0.010.069 ± 0.0013786 ± 57  32.83 ± 0.06739 ± 15006 ± 0.01
PG composite15.38 ± 0.131.64 ± 0.000.194 ± 0.0013602 ± 57  4.18 ± 0.08811 ± 195006 ± 0.15

Note. The power law is given as f1000 ∼ λ−α, with flux density units 10−16 erg cm−2 s−1 Å−1. For the emission-line components, we list the integrated flux (in 10−16 erg cm−2 s−1), the centroid (in Å) and the full-width at half-maximum (in km s−1) of the combined line profile. For the Fe ii template, the flux listed is relative to the strength of the I Zw 1 Fe ii emission. When no values are reported for a given component, that component was not used in the fit. When no errors are reported for a given component, that component reached a limit and became fixed in the fit. We report the redshift as determined by the centroid of the total Hα line. In the case of Q 1031+3953, where the Hα is not covered, we use the [O iii] λ5007 line. All wavelengths are reported relative to our optically based redshift. The optically based redshift is also employed in the construction of the composite.

aThe [O iii] doublet was fitted with two Gaussian components. The λ4959 component has the listed flux and FWHM with a centroid of 0.990 4272 times the λ5007 centroid.

Table 4.

Spectral parameters of optical Fe ii blend and [O iii].

Power lawOptical Fe ii[O iii] λλ5007, λ4959 a
ObjectRedshiftf1000αScaleFWHMFluxFWHMCentroid
0809+27531.51112.70 ± 0.021.36 ± 0.010.258 ± 0.0233478 ± 7803.05 ± 0.09791 ± 75013 ± 0.02
1031+39531.08211.70 ± 0.291.35 ± 0.010.288 ± 0.01690004.09 ± 0.091730 ± 15000 ± 0.06
1044+36560.7015.63 ± 0.041.51 ± 0.010.094 ± 0.0032672 ± 18  
1312+23191.5083.18 ± 0.121.43 ± 0.020.091 ± 0.0033958 ± 1140.04 ± 0.061029 ± 105010 ± 0.14
1324+24522.3570.99 ± 0.041.60 ± 0.020.002 ± 0.0012777 ± 47  0.89 ± 0.122025 ± 3175000
1408+30540.8423.74 ± 0.261.46 ± 0.040.128 ± 0.0122505 ± 117
1427+27091.1702.85 ± 0.051.58 ± 0.020.017 ± 0.00510003.42 ± 2.793957 ± 7795007 ± 0.93
1523+39140.6570.21 ± 0.010.63 ± 0.010.056 ± 0.0047678 ± 2   
Composite17.90 ± 0.451.63 ± 0.010.233 ± 0.0082474 ± 1   0.65 ± 0.85852 ± 225006 ± 0.09
FBQS composite0.78 ± 0.010.12 ± 0.010.069 ± 0.0013786 ± 57  32.83 ± 0.06739 ± 15006 ± 0.01
PG composite15.38 ± 0.131.64 ± 0.000.194 ± 0.0013602 ± 57  4.18 ± 0.08811 ± 195006 ± 0.15
Power lawOptical Fe ii[O iii] λλ5007, λ4959 a
ObjectRedshiftf1000αScaleFWHMFluxFWHMCentroid
0809+27531.51112.70 ± 0.021.36 ± 0.010.258 ± 0.0233478 ± 7803.05 ± 0.09791 ± 75013 ± 0.02
1031+39531.08211.70 ± 0.291.35 ± 0.010.288 ± 0.01690004.09 ± 0.091730 ± 15000 ± 0.06
1044+36560.7015.63 ± 0.041.51 ± 0.010.094 ± 0.0032672 ± 18  
1312+23191.5083.18 ± 0.121.43 ± 0.020.091 ± 0.0033958 ± 1140.04 ± 0.061029 ± 105010 ± 0.14
1324+24522.3570.99 ± 0.041.60 ± 0.020.002 ± 0.0012777 ± 47  0.89 ± 0.122025 ± 3175000
1408+30540.8423.74 ± 0.261.46 ± 0.040.128 ± 0.0122505 ± 117
1427+27091.1702.85 ± 0.051.58 ± 0.020.017 ± 0.00510003.42 ± 2.793957 ± 7795007 ± 0.93
1523+39140.6570.21 ± 0.010.63 ± 0.010.056 ± 0.0047678 ± 2   
Composite17.90 ± 0.451.63 ± 0.010.233 ± 0.0082474 ± 1   0.65 ± 0.85852 ± 225006 ± 0.09
FBQS composite0.78 ± 0.010.12 ± 0.010.069 ± 0.0013786 ± 57  32.83 ± 0.06739 ± 15006 ± 0.01
PG composite15.38 ± 0.131.64 ± 0.000.194 ± 0.0013602 ± 57  4.18 ± 0.08811 ± 195006 ± 0.15

Note. The power law is given as f1000 ∼ λ−α, with flux density units 10−16 erg cm−2 s−1 Å−1. For the emission-line components, we list the integrated flux (in 10−16 erg cm−2 s−1), the centroid (in Å) and the full-width at half-maximum (in km s−1) of the combined line profile. For the Fe ii template, the flux listed is relative to the strength of the I Zw 1 Fe ii emission. When no values are reported for a given component, that component was not used in the fit. When no errors are reported for a given component, that component reached a limit and became fixed in the fit. We report the redshift as determined by the centroid of the total Hα line. In the case of Q 1031+3953, where the Hα is not covered, we use the [O iii] λ5007 line. All wavelengths are reported relative to our optically based redshift. The optically based redshift is also employed in the construction of the composite.

aThe [O iii] doublet was fitted with two Gaussian components. The λ4959 component has the listed flux and FWHM with a centroid of 0.990 4272 times the λ5007 centroid.

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