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Table 1.

Constraints on a cosmological measurement of G = λG2Gcodata for different data combination and cosmological models.

Model Data λG H0 (km s−1 Mpc−1) w0 wa Ωk
ΛCDM P20 TTTEEE + BAO SDSS 67.74 ± 0.41
ΛCDM P20 TTTEEE + BAO DESI 68.22 ± 0.39
λGΛCDM P20 TT 1 . 048 0.035 + 0.027 $ 1.048^{+0.027}_{-0.035} $ 74 . 4 5.2 + 3.7 $ 74.4^{+3.7}_{-5.2} $
λGΛCDM P18 TT + low E 0.998 ± 0.018 66.9 ± 2.00
λGΛCDM P18 TT + low E high- 0 . 969 0.058 + 0.052 $ 0.969^{+0.052}_{-0.058} $ 62 . 0 4.9 + 3.9 $ 62.0^{+3.9}_{-4.9} $
λGΛCDM P18 TT + low E low- 1 . 18 0.038 + 0.13 $ 1.18^{+0.13}_{-0.038} $ 80 . 9 4.4 + 8.5 $ 80.9^{+8.5}_{-4.4} $
λGΛCDM P20 EE 1 . 062 0.059 + 0.052 $ 1.062^{+0.052}_{-0.059} $ 74 . 7 6.2 + 5.4 $ 74.7^{+5.4}_{-6.2} $
λGΛCDM P20 TE 1.023 ± 0.047 70.5 ± 4.4
λGΛCDM P20 TTTEEE 1.007 ± 0.011 68.3 ± 1.1
λGΛCDM P20 TTTEEE + BAO DESI 1.010 ± 0.011 69.11 ± 0.98
λGΛCDM P20 TTTEEE + BAO DESI + BBN 1.0056 ± 0.0091 68.63 ± 0.87
λGw0CDM P20 TTTEEE + BAO DESI 1.008 ± 0.011 70 . 8 1.9 + 1.7 $ 70.8^{+1.7}_{-1.9} $ 1 . 070 0.055 + 0.062 $ -1.070^{+0.062}_{-0.055} $
λGw0waCDM P20 TTTEEE + BAO DESI 1.006 ± 0.011 64.9 ± 3.5 0 . 46 0.42 + 0.31 $ -0.46^{+0.31}_{-0.42} $ 1 . 67 0.79 + 1.2 $ -1.67^{+1.2}_{-0.79} $
λGΩkΛCDM P20 TTTEEE + BAO DESI 1.008 ± 0.011 69.3 ± 1.0 0.0016 ± 0.0015

Notes. The first two lines are obtained by fixing λG = 1 in our code, giving consistent results with the literature.

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