Table 2.
Maximum discrimination efficiency ℰmax with respect to ΛCDM attained for each MG model according to Map statistic, filtering scale ϑ, and source redshift zs.
| Model | ℰmax | Statistic | ϑ | zs |
|---|---|---|---|---|
| f4(R) [mν = 0 eV] | 100% 100% |
var. all others |
mult. mult. |
mult. mult. |
| f4(R) [mν = 0.3 eV] | 19% 38% |
var. p.c. (> 3σ) |
0.586′ 0.586′ |
2.0 2.0 |
| f5(R) [mν = 0 eV] | 99% 100% |
var. p.c. (mult.) |
1.17′ 0.586′ |
2.0 mult. |
| f5(R) [mν = 0.1 eV] | 76% 100% |
var. p.c. (mult.) |
1.17′ 0.586′ |
2.0 mult. |
| f5(R) [mν = 0.15 eV] | 17% 100% |
var. p.c. (mult.) |
1.17′ 0.586′ |
1.0 mult. |
| f6(R) [mν = 0 eV] | 12% 39% |
var. p.c. (> 5σ) |
1.17′ 18.8′ |
1.0 1.5 |
| f6(R) [mν = 0.06 eV] | 4.7% 41% |
var. p.c. (> 5σ) |
0.586′ 0.586′ |
1.5 2.0 |
| f6(R) [mν = 0.1 eV] | 12% 66% |
var. p.c. (> 5σ) |
2.34′ 0.586′ |
2.0 2.0 |
Notes. Results for the variance are shown first, along with the best available statistic underneath. For all models except f4(R) without neutrinos, the unique maximum discrimination efficiency is achieved with peak counts (p.c.), either above the 3σ or 5σ threshold. For f4(R) with mν = 0 eV, all of the statistics reach 100% discrimination efficiency for at least one combination of ϑ and zs.
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