Estimating small angular scale CMB anisotropy with high resolution N-body simulations: weak lensing

We estimate the impact of weak lensing by strongly nonlinear cosmological structures on the cosmic microwave background. Accurate calculation of large \(\ell\) multipoles requires N-body simulations and ray-tracing schemes with both high spatial and temporal resolution. To this end we have developed...

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Veröffentlicht in:arXiv.org 2010-01
Hauptverfasser: Fullana, M J, Arnau, J V, Thacker, R J, Couchman, H M P, Sáez, D
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Sprache:eng
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Zusammenfassung:We estimate the impact of weak lensing by strongly nonlinear cosmological structures on the cosmic microwave background. Accurate calculation of large \(\ell\) multipoles requires N-body simulations and ray-tracing schemes with both high spatial and temporal resolution. To this end we have developed a new code that combines a gravitational Adaptive Particle-Particle, Particle-Mesh (AP3M) solver with a weak lensing evaluation routine. The lensing deviations are evaluated while structure evolves during the simulation so that all evolution steps--rather than just a few outputs--are used in the lensing computations. The new code also includes a ray-tracing procedure that avoids periodicity effects in a universe that is modeled as a 3-D torus in the standard way. Results from our new simulations are compared with previous ones based on Particle-Mesh simulations. We also systematically investigate the impact of box volume, resolution, and ray-tracing directions on the variance of the computed power spectra. We find that a box size of \(512 h^{-1}\) Mpc is sufficient to provide a robust estimate of the weak lensing angular power spectrum in the \(\ell\)-interval (2,000--7,000). For a reaslistic cosmological model the power \([\ell(\ell+1)C_{\ell}/2\pi]^{1/2}\) takes on values of a few \(\mu K\) in this interval, which suggests that a future detection is feasible and may explain the excess power at high \(\ell\) in the BIMA and CBI observations.
ISSN:2331-8422
DOI:10.48550/arxiv.1001.4991