Figure 11.
Gas density PDFs at the onset of sink particle formation (top panel) and 4 Myr later (bottom panel). We show PDFs from the 10−2 (red lines), 10−3 (green lines) and 10−4 Z⊙ (blue lines) runs. We separately plot PDFs computed using all gas within the virial radius of the halo (dashed lines) and only gas with T < 200 K and n > 100 cm−3 (solid lines). For the all gas PDFs, the average density is n0 ≈ 1 cm−3 at both times. In the bottom panel, we show lognormal fits to the 10−2 and 10−3 Z⊙ run cold gas PDFs which have widths of σ = 0.86 and 0.71, respectively. Power-law tails, evident in the top panel and in the 10−4 Z⊙ run in the bottom panel, are an anticipated outcome of self-gravity. In the 10−3 Z⊙ run, however, this power-law tail disappears within ∼2 Myr after the first sink particle formation as the sink particles deplete the cold, dense gas.

Gas density PDFs at the onset of sink particle formation (top panel) and 4 Myr later (bottom panel). We show PDFs from the 10−2 (red lines), 10−3 (green lines) and 10−4 Z (blue lines) runs. We separately plot PDFs computed using all gas within the virial radius of the halo (dashed lines) and only gas with T < 200 K and n > 100 cm−3 (solid lines). For the all gas PDFs, the average density is n0 ≈ 1 cm−3 at both times. In the bottom panel, we show lognormal fits to the 10−2 and 10−3 Z run cold gas PDFs which have widths of σ = 0.86 and 0.71, respectively. Power-law tails, evident in the top panel and in the 10−4 Z run in the bottom panel, are an anticipated outcome of self-gravity. In the 10−3 Z run, however, this power-law tail disappears within ∼2 Myr after the first sink particle formation as the sink particles deplete the cold, dense gas.

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