Table 2.

Simulation and cosmological parameters for the N-body simulations. Massara et al. (2015) use different names, which we list here.

NameReason for nameMassara et al. (2015)Box size (⁠|$h^{-1}\, {\rm Mpc}$|⁠)NcdmNνmν (eV)σ8109As
HZHigh σ8, zero ∑mνL010002563000.8342.13
LZLow σ8, zero ∑mνL0s810002563000.6931.473
LNLow σ8, non-zero ∑mνL601000256325630.60.6932.13
HZHRHigh σ8, zero ∑mν, high resolutionH05005123000.8342.13
LNHRLow σ8, zero ∑mν, high resolutionH60500512351230.60.6931.473
NameReason for nameMassara et al. (2015)Box size (⁠|$h^{-1}\, {\rm Mpc}$|⁠)NcdmNνmν (eV)σ8109As
HZHigh σ8, zero ∑mνL010002563000.8342.13
LZLow σ8, zero ∑mνL0s810002563000.6931.473
LNLow σ8, non-zero ∑mνL601000256325630.60.6932.13
HZHRHigh σ8, zero ∑mν, high resolutionH05005123000.8342.13
LNHRLow σ8, zero ∑mν, high resolutionH60500512351230.60.6931.473
Table 2.

Simulation and cosmological parameters for the N-body simulations. Massara et al. (2015) use different names, which we list here.

NameReason for nameMassara et al. (2015)Box size (⁠|$h^{-1}\, {\rm Mpc}$|⁠)NcdmNνmν (eV)σ8109As
HZHigh σ8, zero ∑mνL010002563000.8342.13
LZLow σ8, zero ∑mνL0s810002563000.6931.473
LNLow σ8, non-zero ∑mνL601000256325630.60.6932.13
HZHRHigh σ8, zero ∑mν, high resolutionH05005123000.8342.13
LNHRLow σ8, zero ∑mν, high resolutionH60500512351230.60.6931.473
NameReason for nameMassara et al. (2015)Box size (⁠|$h^{-1}\, {\rm Mpc}$|⁠)NcdmNνmν (eV)σ8109As
HZHigh σ8, zero ∑mνL010002563000.8342.13
LZLow σ8, zero ∑mνL0s810002563000.6931.473
LNLow σ8, non-zero ∑mνL601000256325630.60.6932.13
HZHRHigh σ8, zero ∑mν, high resolutionH05005123000.8342.13
LNHRLow σ8, zero ∑mν, high resolutionH60500512351230.60.6931.473
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