Table 1.

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 = 04.87≥9.42
z = 0.54.36≥9.42
z = 13.99≥9.42
z = 2.761.973.57
z = 101.341.99
|$k_{1\,\mathrm{ per\,cent}}\,\,[\, h\, {\rm Mpc}^{-1}]$||$k_{2\,\mathrm{ per\,cent}}\,\,[\, h\, {\rm Mpc}^{-1}]$|
z = 04.87≥9.42
z = 0.54.36≥9.42
z = 13.99≥9.42
z = 2.761.973.57
z = 101.341.99
Table 1.

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 = 04.87≥9.42
z = 0.54.36≥9.42
z = 13.99≥9.42
z = 2.761.973.57
z = 101.341.99
|$k_{1\,\mathrm{ per\,cent}}\,\,[\, h\, {\rm Mpc}^{-1}]$||$k_{2\,\mathrm{ per\,cent}}\,\,[\, h\, {\rm Mpc}^{-1}]$|
z = 04.87≥9.42
z = 0.54.36≥9.42
z = 13.99≥9.42
z = 2.761.973.57
z = 101.341.99
Close
This Feature Is Available To Subscribers Only

Sign In or Create an Account

Close

This PDF is available to Subscribers Only

View Article Abstract & Purchase Options

For full access to this pdf, sign in to an existing account, or purchase an annual subscription.

Close