Table 4.

The properties of the reconstructed continuum emission, corrected for lensing magnification. For H1413+117, we give values after correcting the SED for photometric confusion (see Section 2.6). Note that for all except WFI J2033−4723 and PG 1115+080, the quoted sizes include an additional |$\pm 10\,\mathrm{ per\,cent}$| uncertainty due to empirical scatter in the slope of the mass profile (see Section 4.1 for details).

μdustRdustn|$T_{\rm d}^{\rm cold}$||$T_{\rm d}^{\rm warm}$|βLFIRSFRΣSFRMd
(kpc)(K)(K)(L)(M yr−1)(M yr−1 kpc−2)(M)
HS 0810+255425 ± 40.13 ± 0.040.57 ± 0.05|$39^{+4}_{-5}$||$135^{+25}_{-18}$|≡ 2|$1.3^{+1.0}_{-0.9}\times 10^{11}$||$40^{+30}_{-30}$||$400^{+300}_{-300}$||$1.1^{+0.4}_{-0.5}\times 10^{7}$|
RX J0911+055114.8 ± 0.20.51 ± 0.030.56 ± 0.04|$54^{+3}_{-3}$||$1.9^{+0.1}_{-0.1}$||$2.3^{+0.1}_{-0.1}\times 10^{12}$||$750^{+50}_{-50}$||$500^{+100}_{-100}$||$5.3^{+0.9}_{-0.8}\times 10^{6}$|
SDSS J0924+021915.1 ± 0.71.9 ± 0.21.2 ± 0.1|$38^{+8}_{-7}$||$1.5^{+0.6}_{-0.4}$||$1.9^{+0.7}_{-0.5}\times 10^{11}$||$60^{+20}_{-20}$||$3^{+1}_{-1}$||$3.9^{+1.5}_{-1.4}\times 10^{7}$|
PG 1115+08021.5 ± 0.40.14 ± 0.040.47 ± 0.01|$66^{+17}_{-21}$||$1.9^{+0.3}_{-0.3}$||$3.4^{+1.2}_{-1.0}\times 10^{11}$||$110^{+40}_{-30}$||$1000^{+400}_{-400}$||$2.5^{+1.5}_{-1.0}\times 10^{6}$|
H1413+11711.2 ± 0.20.8 ± 0.10.66 ± 0.07|$53^{+1}_{-1}$||$246^{+14}_{-24}$||$1.88^{+0.04}_{-0.04}$||$4.9^{+0.2}_{-0.2}\times 10^{12}$||$1600^{+60}_{-60}$||$370^{+80}_{-80}$||$1.2^{+0.1}_{-0.1}\times 10^{8}$|
WFI J2026−453619.6 ± 0.80.19 ± 0.020.61 ± 0.02|$63^{+4}_{-3}$||$1.8^{+0.1}_{-0.1}$||$3.1^{+1.7}_{-1.5}\times 10^{12}$||$1010^{+60}_{-50}$||$4500^{+1700}_{-1700}$||$3.9^{+0.1}_{0.1}\times 10^7$|
WFI J2033−472317.6 ± 0.92.5 ± 0.21.1 ± 0.2|$31^{+7}_{-5}$||$1.7^{+0.3}_{-0.3}$||$3.1^{+0.9}_{-0.6}\times 10^{11}$||$100^{+30}_{-20}$||$2.5^{+0.9}_{-0.7}$||$4.5^{+0.8}_{-0.7}\times 10^{7}$|
μdustRdustn|$T_{\rm d}^{\rm cold}$||$T_{\rm d}^{\rm warm}$|βLFIRSFRΣSFRMd
(kpc)(K)(K)(L)(M yr−1)(M yr−1 kpc−2)(M)
HS 0810+255425 ± 40.13 ± 0.040.57 ± 0.05|$39^{+4}_{-5}$||$135^{+25}_{-18}$|≡ 2|$1.3^{+1.0}_{-0.9}\times 10^{11}$||$40^{+30}_{-30}$||$400^{+300}_{-300}$||$1.1^{+0.4}_{-0.5}\times 10^{7}$|
RX J0911+055114.8 ± 0.20.51 ± 0.030.56 ± 0.04|$54^{+3}_{-3}$||$1.9^{+0.1}_{-0.1}$||$2.3^{+0.1}_{-0.1}\times 10^{12}$||$750^{+50}_{-50}$||$500^{+100}_{-100}$||$5.3^{+0.9}_{-0.8}\times 10^{6}$|
SDSS J0924+021915.1 ± 0.71.9 ± 0.21.2 ± 0.1|$38^{+8}_{-7}$||$1.5^{+0.6}_{-0.4}$||$1.9^{+0.7}_{-0.5}\times 10^{11}$||$60^{+20}_{-20}$||$3^{+1}_{-1}$||$3.9^{+1.5}_{-1.4}\times 10^{7}$|
PG 1115+08021.5 ± 0.40.14 ± 0.040.47 ± 0.01|$66^{+17}_{-21}$||$1.9^{+0.3}_{-0.3}$||$3.4^{+1.2}_{-1.0}\times 10^{11}$||$110^{+40}_{-30}$||$1000^{+400}_{-400}$||$2.5^{+1.5}_{-1.0}\times 10^{6}$|
H1413+11711.2 ± 0.20.8 ± 0.10.66 ± 0.07|$53^{+1}_{-1}$||$246^{+14}_{-24}$||$1.88^{+0.04}_{-0.04}$||$4.9^{+0.2}_{-0.2}\times 10^{12}$||$1600^{+60}_{-60}$||$370^{+80}_{-80}$||$1.2^{+0.1}_{-0.1}\times 10^{8}$|
WFI J2026−453619.6 ± 0.80.19 ± 0.020.61 ± 0.02|$63^{+4}_{-3}$||$1.8^{+0.1}_{-0.1}$||$3.1^{+1.7}_{-1.5}\times 10^{12}$||$1010^{+60}_{-50}$||$4500^{+1700}_{-1700}$||$3.9^{+0.1}_{0.1}\times 10^7$|
WFI J2033−472317.6 ± 0.92.5 ± 0.21.1 ± 0.2|$31^{+7}_{-5}$||$1.7^{+0.3}_{-0.3}$||$3.1^{+0.9}_{-0.6}\times 10^{11}$||$100^{+30}_{-20}$||$2.5^{+0.9}_{-0.7}$||$4.5^{+0.8}_{-0.7}\times 10^{7}$|
Table 4.

The properties of the reconstructed continuum emission, corrected for lensing magnification. For H1413+117, we give values after correcting the SED for photometric confusion (see Section 2.6). Note that for all except WFI J2033−4723 and PG 1115+080, the quoted sizes include an additional |$\pm 10\,\mathrm{ per\,cent}$| uncertainty due to empirical scatter in the slope of the mass profile (see Section 4.1 for details).

μdustRdustn|$T_{\rm d}^{\rm cold}$||$T_{\rm d}^{\rm warm}$|βLFIRSFRΣSFRMd
(kpc)(K)(K)(L)(M yr−1)(M yr−1 kpc−2)(M)
HS 0810+255425 ± 40.13 ± 0.040.57 ± 0.05|$39^{+4}_{-5}$||$135^{+25}_{-18}$|≡ 2|$1.3^{+1.0}_{-0.9}\times 10^{11}$||$40^{+30}_{-30}$||$400^{+300}_{-300}$||$1.1^{+0.4}_{-0.5}\times 10^{7}$|
RX J0911+055114.8 ± 0.20.51 ± 0.030.56 ± 0.04|$54^{+3}_{-3}$||$1.9^{+0.1}_{-0.1}$||$2.3^{+0.1}_{-0.1}\times 10^{12}$||$750^{+50}_{-50}$||$500^{+100}_{-100}$||$5.3^{+0.9}_{-0.8}\times 10^{6}$|
SDSS J0924+021915.1 ± 0.71.9 ± 0.21.2 ± 0.1|$38^{+8}_{-7}$||$1.5^{+0.6}_{-0.4}$||$1.9^{+0.7}_{-0.5}\times 10^{11}$||$60^{+20}_{-20}$||$3^{+1}_{-1}$||$3.9^{+1.5}_{-1.4}\times 10^{7}$|
PG 1115+08021.5 ± 0.40.14 ± 0.040.47 ± 0.01|$66^{+17}_{-21}$||$1.9^{+0.3}_{-0.3}$||$3.4^{+1.2}_{-1.0}\times 10^{11}$||$110^{+40}_{-30}$||$1000^{+400}_{-400}$||$2.5^{+1.5}_{-1.0}\times 10^{6}$|
H1413+11711.2 ± 0.20.8 ± 0.10.66 ± 0.07|$53^{+1}_{-1}$||$246^{+14}_{-24}$||$1.88^{+0.04}_{-0.04}$||$4.9^{+0.2}_{-0.2}\times 10^{12}$||$1600^{+60}_{-60}$||$370^{+80}_{-80}$||$1.2^{+0.1}_{-0.1}\times 10^{8}$|
WFI J2026−453619.6 ± 0.80.19 ± 0.020.61 ± 0.02|$63^{+4}_{-3}$||$1.8^{+0.1}_{-0.1}$||$3.1^{+1.7}_{-1.5}\times 10^{12}$||$1010^{+60}_{-50}$||$4500^{+1700}_{-1700}$||$3.9^{+0.1}_{0.1}\times 10^7$|
WFI J2033−472317.6 ± 0.92.5 ± 0.21.1 ± 0.2|$31^{+7}_{-5}$||$1.7^{+0.3}_{-0.3}$||$3.1^{+0.9}_{-0.6}\times 10^{11}$||$100^{+30}_{-20}$||$2.5^{+0.9}_{-0.7}$||$4.5^{+0.8}_{-0.7}\times 10^{7}$|
μdustRdustn|$T_{\rm d}^{\rm cold}$||$T_{\rm d}^{\rm warm}$|βLFIRSFRΣSFRMd
(kpc)(K)(K)(L)(M yr−1)(M yr−1 kpc−2)(M)
HS 0810+255425 ± 40.13 ± 0.040.57 ± 0.05|$39^{+4}_{-5}$||$135^{+25}_{-18}$|≡ 2|$1.3^{+1.0}_{-0.9}\times 10^{11}$||$40^{+30}_{-30}$||$400^{+300}_{-300}$||$1.1^{+0.4}_{-0.5}\times 10^{7}$|
RX J0911+055114.8 ± 0.20.51 ± 0.030.56 ± 0.04|$54^{+3}_{-3}$||$1.9^{+0.1}_{-0.1}$||$2.3^{+0.1}_{-0.1}\times 10^{12}$||$750^{+50}_{-50}$||$500^{+100}_{-100}$||$5.3^{+0.9}_{-0.8}\times 10^{6}$|
SDSS J0924+021915.1 ± 0.71.9 ± 0.21.2 ± 0.1|$38^{+8}_{-7}$||$1.5^{+0.6}_{-0.4}$||$1.9^{+0.7}_{-0.5}\times 10^{11}$||$60^{+20}_{-20}$||$3^{+1}_{-1}$||$3.9^{+1.5}_{-1.4}\times 10^{7}$|
PG 1115+08021.5 ± 0.40.14 ± 0.040.47 ± 0.01|$66^{+17}_{-21}$||$1.9^{+0.3}_{-0.3}$||$3.4^{+1.2}_{-1.0}\times 10^{11}$||$110^{+40}_{-30}$||$1000^{+400}_{-400}$||$2.5^{+1.5}_{-1.0}\times 10^{6}$|
H1413+11711.2 ± 0.20.8 ± 0.10.66 ± 0.07|$53^{+1}_{-1}$||$246^{+14}_{-24}$||$1.88^{+0.04}_{-0.04}$||$4.9^{+0.2}_{-0.2}\times 10^{12}$||$1600^{+60}_{-60}$||$370^{+80}_{-80}$||$1.2^{+0.1}_{-0.1}\times 10^{8}$|
WFI J2026−453619.6 ± 0.80.19 ± 0.020.61 ± 0.02|$63^{+4}_{-3}$||$1.8^{+0.1}_{-0.1}$||$3.1^{+1.7}_{-1.5}\times 10^{12}$||$1010^{+60}_{-50}$||$4500^{+1700}_{-1700}$||$3.9^{+0.1}_{0.1}\times 10^7$|
WFI J2033−472317.6 ± 0.92.5 ± 0.21.1 ± 0.2|$31^{+7}_{-5}$||$1.7^{+0.3}_{-0.3}$||$3.1^{+0.9}_{-0.6}\times 10^{11}$||$100^{+30}_{-20}$||$2.5^{+0.9}_{-0.7}$||$4.5^{+0.8}_{-0.7}\times 10^{7}$|
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