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Table 1.

Kinematic table for CARS sources.

Object z log(L[O III])(a) log(LBLR Hβ) (b) W80(c) Δv(d) σ[O III])(e)
(erg s−1) (erg s−1) (km s−1) (km s−1) (km s−1)
Core Wing
HE0021−1810 0.054 41.10 ± 0.01 40.81 ± 0.02 570 ± 4 −83 ± 2 102 ± 2 288 ± 4
HE0021−1819 0.053 41.29 ± 0.01 40.79 ± 0.01 465 ± 1 −130 ± 1 73 ± 1 296 ± 1
HE0040−1105 0.042 41.31 ± 0.01 41.15 ± 0.01 392 ± 1 −98 ± 1 67 ± 1 254 ± 1
HE0108−4743 0.024 40.57 ± 0.01 40.60 ± 0.01 238 ± 2 −55 ± 2 41 ± 2 114 ± 2
HE0114−0015 0.046 40.47 ± 0.01 40.61 ± 0.01 377 ± 5 9 ± 13 125 ± 1 402 ± 21
HE0119−0118 0.054 41.72 ± 0.01 41.78 ± 0.01 540 ± 1 −210 ± 1 106 ± 1 238 ± 1
HE0212−0059 0.026 40.95 ± 0.01 41.38 ± 0.03 587 ± 9 −276 ± 18 172 ± 1 472 ± 20
HE0224−2834 0.060 41.52 ± 0.01 41.62 ± 0.01 418 ± 1 −26 ± 2 113 ± 1 276 ± 3
HE0227−0913 0.016 40.43 ± 0.01 41.21 ± 0.01 552 ± 5 −452 ± 6 139 ± 1 287 ± 5
HE0232−0900 0.043 42.09 ± 0.01 42.20 ± 0.01 496 ± 1 −29 ± 1 145 ± 1 330 ± 1
HE0253−1641 0.032 41.31 ± 0.01 41.19 ± 0.01 716 ± 3 −249 ± 2 106 ± 1 367 ± 2
HE0345+0056 0.031 41.67 ± 0.01 42.12 ± 0.01 878 ± 4 −335 ± 5 154 ± 2 388 ± 2
HE0351+0240 0.036 41.24 ± 0.01 41.29 ± 0.01 215 ± 1 −19 ± 2 70 ± 1 234 ± 4
HE0412−0803 0.038 42.37 ± 0.01 41.94 ± 0.27 304 ± 23 −21 ± 6 80 ± 9 250 ± 68
HE0429−0247 0.042 41.14 ± 0.01 41.41 ± 0.01 320 ± 1 −52 ± 1 87 ± 1 220 ± 1
HE0433−1028 0.036 41.61 ± 0.01 41.89 ± 0.01 95 ± 27 310 ± 1− 126 ± 1 336 ± 1
HE0853+0102 0.052 40.90 ± 0.01 41.00 ± 0.07 474 ± 51 −35 ± 6 102 ± 5 303 ± 45
HE0934+0119 0.050 41.34 ± 0.01 41.77 ± 0.01 349 ± 1 −123 ± 2 71 ± 1 171 ± 1
HE1011−0403 0.058 41.42 ± 0.01 41.96 ± 0.01 545 ± 2 −212 ± 2 98 ± 1 256 ± 1
HE1017−0305 0.050 41.09 ± 0.01 41.84 ± 0.01 372 ± 6 −63 ± 5 60 ± 2 217 ± 6
HE1029−1831 0.040 41.15 ± 0.01 41.35 ± 0.01 521 ± 2 −135 ± 3 71 ± 2 217 ± 1
HE1107−0813 0.058 40.94 ± 0.03 42.26 ± 0.03 1248 ± 226 −70 ± 28 78 ± 8 598 ± 133
HE1108−2813 0.024 40.80 ± 0.01 41.07 ± 0.01 490 ± 2 −118 ± 1 68 ± 1 235 ± 2
HE1126−0407 0.062 41.79 ± 0.01 42.57 ± 0.01 594 ± 5 −271 ± 5 114 ± 1 344 ± 4
HE1237−0504 0.019 40.49 ± 0.01 40.67 ± 0.01 470 ± 1 −181 ± 2 104 ± 1 300 ± 2
HE1248−1356 0.015 40.32 ± 0.05 39.82 ± 0.01 287 ± 3 −32 ± 4 57 ± 1 210 ± 11
HE1310−1051 0.034 41.51 ± 0.01 41.57 ± 0.01 333 ± 1 −25 ± 2 93 ± 1 214 ± 3
HE1330−1013 0.022 40.18 ± 0.01 40.71 ± 0.01 409 ± 6 −145 ± 9 74 ± 2 229 ± 5
HE1338−1423 0.042 41.80 ± 0.01 42.02 ± 0.01 528 ± 3 13 ± 4 115 ± 4 268 ± 5
HE1353−1917 0.035 41.05 ± 0.01 41.13 ± 0.02 541 ± 4 −187 ± 6 93 ± 1 360 ± 3
HE1417−0909 0.044 41.44 ± 0.01 41.52 ± 0.01 254 ± 1 −33 ± 1 62 ± 1 180 ± 1
HE2128−0221 0.052 41.10 ± 0.01 41.04 ± 0.01 224 ± 2 −32 ± 2 51 ± 2 143 ± 4
HE2211−3903 0.040 41.04 ± 0.01 41.38 ± 0.01 234 ± 3 −92 ± 9 68 ± 1 205 ± 9
HE2222−0026 0.059 40.85 ± 0.01 41.49 ± 0.01 471 ± 15 −164 ± 17 122 ± 7 244 ± 20
HE2233+0124 0.056 40.90 ± 0.01 41.55 ± 0.02 625 ± 15 47 ± 10 164 ± 4 466 ± 35
HE2302−0857 0.047 42.14 ± 0.03 42.06 ± 0.01 651 ± 17 167 ± 9 175 ± 11 452 ± 29

Notes.

(a)

The [O III]λ5007 luminosity,

(b)

the total broad emission line region (BLR) Hβ luminosity,

(c)

velocity width of emission line [O III] λ5007, that contains 80% of the line flux,

(d)

velocity offset between the core and wing components, used to model the of [O III] λ5007 emission-line,

(e)

velocity dispersion of the [O III] λ5007 core and wing components.

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