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Table 4
Constraints on the cosmological parameters of the base ΛCDM model with the addition of a varying electron mass.
| Planck+WP | Planck+WP+highL | Planck+WP+BAO | Planck+WP+HST | Planck+WP+lensing | WMAP-9 | |
| Parameter | 68% limits | 68% limits | 68% limits | 68% limits | 68% limits | 68% limits |
|
|
||||||
| Ωbh2...... |
|
|
0.02216 ± 0.00027 | 0.02270 ± 0.00033 |
|
|
| Ωch2...... |
|
|
0.1201 ± 0.0036 | 0.1229 ± 0.0035 |
|
0.1154 ± 0.0083 |
| H0...... |
|
|
68.4 ± 1.7 | 73.5 ± 2.4 |
|
72 ± 10 |
| τ...... |
|
|
|
|
|
|
| me/me0...... |
|
|
1.004 ± 0.011 | 1.027 ± 0.012 | 0.969 ± 0.055 |
|
| ns...... | 0.9584 ± 0.0083 | 0.9565 ± 0.0077 | 0.9614 ± 0.0068 | 0.9628 ± 0.0072 | 0.9618 ± 0.0070 | 0.975 ± 0.014 |
| ln(1010As)... | 3.084 ± 0.027 |
|
3.091 ± 0.025 |
|
3.079 ± 0.025 | 3.097 ± 0.032 |
Notes. We quote ± 1σ errors here. We note that for WMAP there is a strong degeneracy between H0 and me, which is why the uncertainty on me/me0 is much larger than for Planck .
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