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The effect of large-scale power on simulated spectra of the Ly alpha forest

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出版社

OXFORD UNIV PRESS
DOI: 10.1111/j.1365-2966.2008.14196.x

关键词

methods: numerical; intergalactic medium; quasars: absorption lines; cosmology: observations

资金

  1. NSF [AST 0507717, 0808168]

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We explore the effects of size of the box that we use for simulations of the intergalactic medium (IGM) at redshift 2. We examine simulations from the hydrodynamic code ENZO that differ only in box size. We study the cold dark matter (CDM) distribution and many statistics of the Ly alpha forest absorption from the IGM. Larger boxes have fewer pixels with significant absorption (flux < 0.96), more pixels in longer stretches with little or no absorption, and they have wider Ly alpha lines. The larger boxes differ only because they include power from longer wavelength modes. These modes result in higher peak densities, higher velocities and hotter gas. Small simulations are too cold compared to larger ones. When we deliberately increase the heat we put into the IGM, we can approximate the Ly alpha forest in a simulation of twice the size. When we double the box size, the difference of most statistics from their value in our largest 76.8 Mpc box is reduced by approximately a factor of 2. When we enlarge the box from 38.4 to 76.8 Mpc, the mean Ly alpha absorption decreases 0.5 per cent, the frequency with which we encounter different common CDM densities changes by 2 per cent, typical Ly alpha linewidths, the frequency of flux values and the power spectrum of the flux all change by 4-7 per cent, and the column density distribution changes by up to 15 per cent. A 76.8 Mpc box is large enough to give errors of < 1 per cent for the mean flux, 5 per cent for the column density distribution and power spectrum and 5-10 per cent for the flux distribution. When we compare to the errors in data, we find that our 76.8 Mpc box is larger than we need for the mean flux, barely large enough for the flux distribution, column density distribution and the power spectrum of the flux, and too small for the linewidths. Cells of size 18.75 kpc are small enough to give errors of < 1 per cent for the mean flux, 1-5 per cent for linewidths, 5 per cent for the column densities and power and 5-10 per cent for the flux distribution. Compared to data, the simulated spectra in our largest box differ from data in all statistics, except, by design, the mean flux. The simulated spectra have too many Ly alpha lines with small HI column densities log N-HI < 14 cm(-2), and too few with larger log N-HI values. They have factors of 3-30 times too few lines with > 10(17) cm(-2). Decreasing the cell size from 75 to 18.75 kpc makes the difference larger at log N-HI < 14 cm(-2), and does not help with the higher columns. The Ly alpha lines in the simulated spectra from a very large box with 18.75 kpc cells would be too wide by 2.6 km s(-1). The simulated Ly alpha forest has 20 per cent too little power on small scales and 50 per cent too little large scales. A much larger box would increase the large-scale power only a few per cent. We confirm the Kim et al. (2007) and Bolton et al. (2008) finding that the simulated spectra also have different flux distributions than data. It is hard to see how our optically thin simulations using popular cosmological and astrophysical parameters can match the Ly alpha forest data at z = 2. Adding radiation transfer effects, especially shelf-shielding will reduce the temperature at high overdensities, possibly improving the match to linewidths, and it will help match the number of high column density lines. We could also decrease the linewidths with a softer ionizing spectrum, or by using sigma(8) > 0.9, which has the additional benefit of increasing the large-scale power.

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