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Fig. A.1.

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Matter power spectrum ratio between a 0.15 eV massive neutrinos simulation and a ΛCDM simulation with varying timestep, performed by ANUBIS. The simulation box has Lbox = 1024 h−1Mpc, Ncdm = Nν = 10243, and a fixed coarse base grid of 5123. The time step is calculated by the RAMSES algorithm for both runs, but for the ΛCDM case it is multiplied by a reduction factor, A. We see here that one way to compensate for the coarse base grid, especially at large scales, is to shorten the time step. This requires a longer run time for the ΛCDM simulation, but not more memory as would be the result of adopting a finer grid.

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