Table 5.
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Summary of our constraints on the dark matter mass fraction fsub (idealised CDM-only), the thermal relic particle mass mth, and the half-mode mass Mhm for different subsamples of lensed quasars.

Samplefsub (CDM-only)mthMhm
7 quasar lenses|$0.012 ^{+0.007}_{-0.004}$| (subs+LOS)|$0.023 ^{+0.018}_{-0.010}$| (subs-only)>5.58 keV (95 % CL)<107.80 M⊙ (95 % CL)
Exclude MG J0414+0534|$0.010 ^{+0.006}_{-0.004}$||$0.019 ^{+0.008}_{-0.009}$|>5.30 keV<107.89 M⊙
Exclude MG J0414+0534|$0.009 ^{+0.006}_{-0.004}$||$0.018 ^{+0.013}_{-0.008}$|>4.77 keV<108.03 M⊙
and CLASS B2045+265
Samplefsub (CDM-only)mthMhm
7 quasar lenses|$0.012 ^{+0.007}_{-0.004}$| (subs+LOS)|$0.023 ^{+0.018}_{-0.010}$| (subs-only)>5.58 keV (95 % CL)<107.80 M⊙ (95 % CL)
Exclude MG J0414+0534|$0.010 ^{+0.006}_{-0.004}$||$0.019 ^{+0.008}_{-0.009}$|>5.30 keV<107.89 M⊙
Exclude MG J0414+0534|$0.009 ^{+0.006}_{-0.004}$||$0.018 ^{+0.013}_{-0.008}$|>4.77 keV<108.03 M⊙
and CLASS B2045+265
Table 5.
Open in new tab

Summary of our constraints on the dark matter mass fraction fsub (idealised CDM-only), the thermal relic particle mass mth, and the half-mode mass Mhm for different subsamples of lensed quasars.

Samplefsub (CDM-only)mthMhm
7 quasar lenses|$0.012 ^{+0.007}_{-0.004}$| (subs+LOS)|$0.023 ^{+0.018}_{-0.010}$| (subs-only)>5.58 keV (95 % CL)<107.80 M⊙ (95 % CL)
Exclude MG J0414+0534|$0.010 ^{+0.006}_{-0.004}$||$0.019 ^{+0.008}_{-0.009}$|>5.30 keV<107.89 M⊙
Exclude MG J0414+0534|$0.009 ^{+0.006}_{-0.004}$||$0.018 ^{+0.013}_{-0.008}$|>4.77 keV<108.03 M⊙
and CLASS B2045+265
Samplefsub (CDM-only)mthMhm
7 quasar lenses|$0.012 ^{+0.007}_{-0.004}$| (subs+LOS)|$0.023 ^{+0.018}_{-0.010}$| (subs-only)>5.58 keV (95 % CL)<107.80 M⊙ (95 % CL)
Exclude MG J0414+0534|$0.010 ^{+0.006}_{-0.004}$||$0.019 ^{+0.008}_{-0.009}$|>5.30 keV<107.89 M⊙
Exclude MG J0414+0534|$0.009 ^{+0.006}_{-0.004}$||$0.018 ^{+0.013}_{-0.008}$|>4.77 keV<108.03 M⊙
and CLASS B2045+265
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