Chebyshev interpolation in Einstein-Boltzmann codes
astro-ph.CO, astro-ph.IM, physics.comp-ph
Submitted: 2026-08-25
Updated: 2026-08-25
Comments: 8 pages, 7 figures, submitted to A&A, SymBoltz is available at https://github.com/hersle/SymBoltz.jl
Code: https://github.com/hersle/SymBoltz.jl
Project page: https://hersle.github.io/SymBoltz.jl
License: http://creativecommons.org/licenses/by/4.0/
The gist: Einstein-Boltzmann codes compute theoretical predictions of cosmological models and rely heavily on interpolation in their independent variables: time τ, wavenumber k and multipole.
Terminology
Abstract
Einstein-Boltzmann codes compute theoretical predictions of cosmological models and rely heavily on interpolation in their independent variables: time τ, wavenumber k and multipole. We give a practical summary of interpolation with Chebyshev polynomials, which converges rapidly for smooth functions and thus pairs naturally with approximation-free Einstein-Boltzmann codes. By solving the perturbations and line-of-sight integrals at Chebyshev nodes in k and, we show that Chebyshev polynomials interpolate to higher precision than traditional cubic splines from fewer explicit solutions. On a set of example spectra for matter and the cosmic microwave background (CMB), we find up to four orders of magnitude lower interpolation error using the same number of points. For a typical CMB temperature spectrum computed with interpolation in both k and, Chebyshev polynomials converge to 10-4 - 10-5 relative error with only 50-80 points per variable, while cubic splines approach 10-4 error with 200 points, translating to a 2.5 times - 4 times speedup. The exact improvement depends on the target function and is generally more dramatic at high precision levels. Standard Chebyshev-interpolation needs line-of-sight integrals generalized to non-integer, but we show a way to avoid this by rounding the nodes to integers. Chebyshev interpolation is implemented in SymBoltz, which is available at https://github.com/hersle/SymBoltz.jl.
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