Dependency on the redshift of the k modes at which the |$\ell ^{-1}=3\, h\, {\rm Mpc}^{-1}$| simulation are converged at 1 and 2 per cent, respectively. For redshifts 0, 0.5, and 1 the |$k_{2\,\mathrm{ per\, cent}}$| values correspond to the highest k mode obtained from the simulations and hence should be understood as lower bounds.
. | |$k_{1\,\mathrm{ per\,cent}}\,\,[\, h\, {\rm Mpc}^{-1}]$| . | |$k_{2\,\mathrm{ per\,cent}}\,\,[\, h\, {\rm Mpc}^{-1}]$| . |
---|---|---|
z = 0 | 4.87 | ≥9.42 |
z = 0.5 | 4.36 | ≥9.42 |
z = 1 | 3.99 | ≥9.42 |
z = 2.76 | 1.97 | 3.57 |
z = 10 | 1.34 | 1.99 |
. | |$k_{1\,\mathrm{ per\,cent}}\,\,[\, h\, {\rm Mpc}^{-1}]$| . | |$k_{2\,\mathrm{ per\,cent}}\,\,[\, h\, {\rm Mpc}^{-1}]$| . |
---|---|---|
z = 0 | 4.87 | ≥9.42 |
z = 0.5 | 4.36 | ≥9.42 |
z = 1 | 3.99 | ≥9.42 |
z = 2.76 | 1.97 | 3.57 |
z = 10 | 1.34 | 1.99 |
Dependency on the redshift of the k modes at which the |$\ell ^{-1}=3\, h\, {\rm Mpc}^{-1}$| simulation are converged at 1 and 2 per cent, respectively. For redshifts 0, 0.5, and 1 the |$k_{2\,\mathrm{ per\, cent}}$| values correspond to the highest k mode obtained from the simulations and hence should be understood as lower bounds.
. | |$k_{1\,\mathrm{ per\,cent}}\,\,[\, h\, {\rm Mpc}^{-1}]$| . | |$k_{2\,\mathrm{ per\,cent}}\,\,[\, h\, {\rm Mpc}^{-1}]$| . |
---|---|---|
z = 0 | 4.87 | ≥9.42 |
z = 0.5 | 4.36 | ≥9.42 |
z = 1 | 3.99 | ≥9.42 |
z = 2.76 | 1.97 | 3.57 |
z = 10 | 1.34 | 1.99 |
. | |$k_{1\,\mathrm{ per\,cent}}\,\,[\, h\, {\rm Mpc}^{-1}]$| . | |$k_{2\,\mathrm{ per\,cent}}\,\,[\, h\, {\rm Mpc}^{-1}]$| . |
---|---|---|
z = 0 | 4.87 | ≥9.42 |
z = 0.5 | 4.36 | ≥9.42 |
z = 1 | 3.99 | ≥9.42 |
z = 2.76 | 1.97 | 3.57 |
z = 10 | 1.34 | 1.99 |
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