A New Moment Method for Continuum Radiative Transfer in Cosmological Reionization

TL;DR

This paper presents a new moment-based radiative transfer code tailored for cosmological reionization, accurately modeling non-equilibrium ionization and photon conservation, with potential for benchmarking other methods.

Contribution

The paper introduces a novel moment method with an Eddington tensor computed via long characteristics, improving accuracy for cosmological reionization simulations.

Findings

Code conserves photons accurately

Reproduces analytic Stromgren sphere solutions

Handles cosmological effects effectively

Abstract

We introduce a new code for computing time-dependent continuum radiative transfer and non-equilibrium ionization states in static density fields with periodic boundaries. Our code solves the moments of the radiative transfer equation, closed by an Eddingtion tensor computed using a long characteristics method. We show that pure (i.e., not source-centered) short characteristics and the optically-thin approximation are inappropriate for computing Eddington factors for the problem of cosmological reionization. We evolve the non-equilibrium ionization field via an efficient and accurate (errors <1%) technique that switches between fully implicit or explicit finite-differencing depending on whether the local timescales are long or short compared to the timestep. We tailor our code for the problem of cosmological reionization. In tests, the code conserves photons, accurately treats cosmological effects, and reproduces analytic Stromgren sphere solutions. Its chief weakness is that the computation time for the long characteristics calculation scales relatively poorly compared to other techniques (t_{LC} \propto N_{cells}^1.5); however, we mitigate this by only recomputing the Eddington tensor when the radiation field changes substantially. Our technique makes almost no physical approximations, so it provides a way to benchmark faster but more approximate techniques. It can readily be extended to evolve multiple frequencies, though we do not do so here. Finally, we note that our method is generally applicable to any problem involving the transfer of continuum radiation through a periodic volume.