Table E.1.
Summary of the parameters being used of the individual 33 SLACS lenses selected in Sect. 6 to infer mass profile constraints in combination of imaging and kinematics.
| Name | zlens | zsource | θE [arcsec] | reff [arcsec] | γpl | ζ1/r | κext | σSDSS[km s−1] | IFU |
|---|---|---|---|---|---|---|---|---|---|
| SDSSJ0008–0004 | 0.44 | 1.192 | 1.159 ± 0.020 | 1.710 ± 0.060 | – | 1.47 |  |
228 ± 27 | No |
| SDSSJ0029–0055 | 0.227 | 0.931 | 0.951 ± 0.004 | 2.160 ± 0.076 | 2.46 ± 0.10 | 1.14 |  |
216 ± 15 | No |
| SDSSJ0037–0942 | 0.195 | 0.632 | 1.503 ± 0.017 | 1.800 ± 0.063 | 2.19 ± 0.04 | 1.60 |  |
265 ± 8 | Yes |
| SDSSJ0044+0113 | 0.12 | 0.197 | 0.795 ± 0.020 | 1.920 ± 0.067 | – | 1.68 |  |
267 ± 9 | No |
| SDSSJ0216–0813 | 0.3317 | 0.5235 | 1.160 ± 0.020 | 2.970 ± 0.200 | – | 0.83 |  |
351 ± 19 | Yes |
| SDSSJ0330–0020 | 0.351 | 1.071 | 1.079 ± 0.012 | 0.910 ± 0.032 | 2.16 ± 0.03 | 1.32 |  |
273 ± 23 | No |
| SDSSJ0728+3835 | 0.206 | 0.688 | 1.282 ± 0.006 | 1.780 ± 0.062 | 2.23 ± 0.06 | 1.12 |  |
210 ± 8 | No |
| SDSSJ0912+0029 | 0.164 | 0.324 | 1.627 ± 0.020 | 4.010 ± 0.140 | – | 1.71 |  |
301 ± 9 | Yes |
| SDSSJ0959+4416 | 0.237 | 0.531 | 0.961 ± 0.020 | 1.980 ± 0.069 | – | 1.41 |  |
242 ± 13 | No |
| SDSSJ1016+3859 | 0.168 | 0.439 | 1.090 ± 0.020 | 1.460 ± 0.051 | – | 1.58 |  |
255 ± 10 | No |
| SDSSJ1020+1122 | 0.282 | 0.553 | 1.200 ± 0.020 | 1.590 ± 0.056 | – | 0.54 |  |
282 ± 13 | No |
| SDSSJ1023+4230 | 0.191 | 0.696 | 1.414 ± 0.020 | 1.770 ± 0.062 | – | 1.65 |  |
272 ± 12 | No |
| SDSSJ1112+0826 | 0.273 | 0.629 | 1.422 ± 0.015 | 1.320 ± 0.046 | 2.21 ± 0.06 | 1.96 |  |
260 ± 15 | No |
| SDSSJ1134+6027 | 0.153 | 0.474 | 1.102 ± 0.020 | 2.020 ± 0.071 | – | 1.49 |  |
239 ± 8 | No |
| SDSSJ1142+1001 | 0.222 | 0.504 | 0.984 ± 0.020 | 1.240 ± 0.043 | – | 1.18 |  |
238 ± 16 | No |
| SDSSJ1153+4612 | 0.18 | 0.875 | 1.047 ± 0.020 | 1.160 ± 0.041 | – | 1.55 |  |
211 ± 11 | No |
| SDSSJ1204+0358 | 0.164 | 0.631 | 1.287 ± 0.009 | 1.090 ± 0.038 | 2.18 ± 0.08 | 1.89 |  |
251 ± 12 | Yes |
| SDSSJ1213+6708 | 0.123 | 0.64 | 1.416 ± 0.020 | 1.500 ± 0.052 | – | 1.00 |  |
267 ± 7 | No |
| SDSSJ1218+0830 | 0.135 | 0.717 | 1.450 ± 0.020 | 2.700 ± 0.095 | – | 1.40 |  |
222 ± 7 | No |
| SDSSJ1250+0523 | 0.232 | 0.795 | 1.119 ± 0.029 | 1.320 ± 0.046 | 1.92 ± 0.05 | 1.57 |  |
242 ± 10 | Yes |
| SDSSJ1306+0600 | 0.173 | 0.472 | 1.298 ± 0.013 | 1.250 ± 0.044 | 2.18 ± 0.05 | 1.79 |  |
248 ± 14 | No |
| SDSSJ1402+6321 | 0.205 | 0.481 | 1.355 ± 0.003 | 2.290 ± 0.080 | 2.23 ± 0.07 | 1.73 |  |
274 ± 11 | No |
| SDSSJ1403+0006 | 0.189 | 0.473 | 0.830 ± 0.020 | 1.140 ± 0.040 | – | 1.51 |  |
202 ± 12 | No |
| SDSSJ1432+6317 | 0.123 | 0.664 | 1.258 ± 0.020 | 3.040 ± 0.106 | – | 1.77 |  |
210 ± 6 | No |
| SDSSJ1451–0239 | 0.1254 | 0.5203 | 1.040 ± 0.020 | 2.640 ± 0.200 | – | 1.08 |  |
204 ± 10 | Yes |
| SDSSJ1531–0105 | 0.16 | 0.744 | 1.704 ± 0.008 | 1.970 ± 0.069 | 1.92 ± 0.11 | 1.36 |  |
261 ± 10 | No |
| SDSSJ1621+3931 | 0.245 | 0.602 | 1.263 ± 0.004 | 1.510 ± 0.053 | 2.02 ± 0.06 | 0.97 |  |
234 ± 15 | No |
| SDSSJ1627–0053 | 0.208 | 0.524 | 1.227 ± 0.002 | 1.980 ± 0.069 | 1.85 ± 0.14 | 1.47 |  |
274 ± 11 | Yes |
| SDSSJ1630+4520 | 0.248 | 0.793 | 1.786 ± 0.029 | 1.650 ± 0.058 | 2.00 ± 0.03 | 1.29 |  |
283 ± 13 | No |
| SDSSJ1644+2625 | 0.137 | 0.61 | 1.267 ± 0.020 | 1.550 ± 0.054 | – | 1.86 |  |
208 ± 9 | No |
| SDSSJ2303+1422 | 0.155 | 0.517 | 1.613 ± 0.007 | 2.940 ± 0.103 | 2.00 ± 0.04 | 1.56 |  |
251 ± 13 | Yes |
| SDSSJ2321–0939 | 0.082 | 0.532 | 1.599 ± 0.020 | 4.110 ± 0.144 | – | 1.23 |  |
240 ± 6 | Yes |
| SDSSJ2347–0005 | 0.417 | 0.714 | 1.107 ± 0.020 | 1.140 ± 0.040 | – | 1.39 |  |
404 ± 59 | No |
Notes. Aside the name, lens and source redshift, the Einstein radius θE, half-light radius of the deflector reff, imaging data-only inference on the power-law slope γpl (where available), 1/r weighted galaxy number count ζ1/r, external convergence κext, measured velocity dispersion σSDSS and whether VIMOS IFU data is available are provided.
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