Table 2
The dependence on redshift z of the wavenumbers where the
ratios 
(at 
) and
(at 
)
reach 1%, 10%, and 50%.
| z | % |
|
|
|
|
|
||||
| 1% | 0.025 | 0.13 | ||
| 0 | 10% | 0.052 | 0.26 | 8 |
| 50% | 0.57 | |||
|
|
||||
| 1% | 0.03 | 0.3 | ||
| 1 | 10% | 0.064 | 0.63 | 18 |
| 50% | 1.3 | |||
|
|
||||
| 1% | 0.033 | 0.68 | ||
| 2 | 10% | 0.08 | 1.5 | 37 |
| 50% | 4 | |||
|
|
||||
| 1% | 0.043 | 1.3 | ||
| 3 | 10% | 0.1 | 3.2 | 72 |
| 50% | 9.8 | |||
Notes. The last column gives the last order
of
the “renormalized” perturbative expansion that is not fully below the
nonperturbative term. This table is the redshift-space counterpart of the real-space
Table 1, for longitudinal wavenumbers.
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