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Metallicity-Dependent quenching of Star Formation at High Redshift in Small Galaxies
Cosmology and Nongalactic Astrophysics · Submitted 1 Jun 2011
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Our model shows that including the effect of metallicity leads to suppression of star formation at redshift z>2 in dark halos with masses <~ 10^11 Msun, with the suppression becoming near total for halos below ~10^9.5-10 Msun.
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The abstract, sentence by sentence
[abridged] The star formation rates (SFR) of low-metallicity galaxies depend sensitively on the gas metallicity, because metals are crucial to mediating the transition from intermediate-temperature atomic gas to cold molecular gas, a necessary precursor to star formation. We study the impact of this effect on the star formation history of galaxies. We incorporate metallicity-dependent star formation and metal enrichment in a simple model that follows the evolution of a halo main progenitor. Our model shows that including the effect of metallicity leads to suppression of star formation at redshift z>2 in dark halos with masses <~ 10^11 Msun, with the suppression becoming near total for halos below ~10^9.5-10 Msun. We find that at high redshift the SFR cannot catch up with the gas inflow rate (IR), because the SFR is limited by the free-fall time, and because it is suppressed further by a lack of metals. As a result, in each galaxy the SFR is growing in time faster than the IR, and the integrated cosmic SFR density is rising with time. The suppressed in situ SFR at high z makes the growth of stellar mass dominated by ex situ SFR which implies that the specific SFR (sSFR) remains constant with time. The intensely accreted gas at high z is accumulating as an atomic gas reservoir. This provides additional fuel for star formation in 10^10 - 10^12 Msun halos at z ~ 1-3, which allows the SFR to exceed the instantaneous IR, and may enable an even higher outflow rate. At z<1, following the natural decline in IR with time due to the universal expansion, the SFR and sSFR are expected to drop. We specify the expected dependence of sSFR and metallicity on stellar mass and redshift. At a given z, and below a critical mass, these relations are predicted to be flat and rising respectively. Our model predictions qualitatively match some of the puzzling features in the observed star formation history.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | [abridged] The star formation rates (SFR) of low-metallicity galaxies depend sensitively on the gas metallicity, because metals are crucial to mediating the transition from intermediate-temperature atomic gas to cold molecular gas, a necessary precursor to star formation. | background 1.00 | 0.07 | 0.06 | asserted 1.00 |
| s1 | We study the impact of this effect on the star formation history of galaxies. | contribution 0.96 | 0.83 | 0.02 | unclear 0.77 |
| s2 | We incorporate metallicity-dependent star formation and metal enrichment in a simple model that follows the evolution of a halo main progenitor. | method 0.96 | 0.94 | 0.03 | asserted 0.81 |
| s3 | Our model shows that including the effect of metallicity leads to suppression of star formation at redshift z>2 in dark halos with masses <~ 10^11 Msun, with the suppression becoming near total for halos below ~10^9.5-10 Msun. | result 1.00 | 0.95 | 0.70 | asserted 1.00 |
| s4 | We find that at high redshift the SFR cannot catch up with the gas inflow rate (IR), because the SFR is limited by the free-fall time, and because it is suppressed further by a lack of metals. | result 0.84 | 0.88 | 0.13 | asserted 1.00 |
| s5 | As a result, in each galaxy the SFR is growing in time faster than the IR, and the integrated cosmic SFR density is rising with time. | result 0.79 | 0.85 | 0.13 | asserted 1.00 |
| s6 | The suppressed in situ SFR at high z makes the growth of stellar mass dominated by ex situ SFR which implies that the specific SFR (sSFR) remains constant with time. | interpretation 0.85 | 0.87 | 0.17 | asserted 0.99 |
| s7 | The intensely accreted gas at high z is accumulating as an atomic gas reservoir. | result 0.88 | 0.82 | 0.05 | asserted 1.00 |
| s8 | This provides additional fuel for star formation in 10^10 - 10^12 Msun halos at z ~ 1-3, which allows the SFR to exceed the instantaneous IR, and may enable an even higher outflow rate. | result 0.52 | 0.77 | 0.08 | hedged possibility 0.74 |
| s9 | At z<1, following the natural decline in IR with time due to the universal expansion, the SFR and sSFR are expected to drop. | result 0.65 | 0.42 | 0.07 | hedged possibility 0.84 |
| s10 | We specify the expected dependence of sSFR and metallicity on stellar mass and redshift. | contribution 0.61 | 0.85 | 0.06 | asserted 0.93 |
| s11 | At a given z, and below a critical mass, these relations are predicted to be flat and rising respectively. | result 0.98 | 0.77 | 0.11 | asserted 0.71 |
| s12 | Our model predictions qualitatively match some of the puzzling features in the observed star formation history. | result 0.52 | 0.85 | 0.11 | hedged possibility 0.62 |
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Original abstract
[abridged] The star formation rates (SFR) of low-metallicity galaxies depend sensitively on the gas metallicity, because metals are crucial to mediating the transition from intermediate-temperature atomic gas to cold molecular gas, a necessary precursor to star formation. We study the impact of this effect on the star formation history of galaxies. We incorporate metallicity-dependent star formation and metal enrichment in a simple model that follows the evolution of a halo main progenitor. Our model shows that including the effect of metallicity leads to suppression of star formation at redshift z>2 in dark halos with masses <~ 10^11 Msun, with the suppression becoming near total for halos below ~10^9.5-10 Msun. We find that at high redshift the SFR cannot catch up with the gas inflow rate (IR), because the SFR is limited by the free-fall time, and because it is suppressed further by a lack of metals. As a result, in each galaxy the SFR is growing in time faster than the IR, and the integrated cosmic SFR density is rising with time. The suppressed in situ SFR at high z makes the growth of stellar mass dominated by ex situ SFR which implies that the specific SFR (sSFR) remains constant with time. The intensely accreted gas at high z is accumulating as an atomic gas reservoir. This provides additional fuel for star formation in 10^10 - 10^12 Msun halos at z ~ 1-3, which allows the SFR to exceed the instantaneous IR, and may enable an even higher outflow rate. At z<1, following the natural decline in IR with time due to the universal expansion, the SFR and sSFR are expected to drop. We specify the expected dependence of sSFR and metallicity on stellar mass and redshift. At a given z, and below a critical mass, these relations are predicted to be flat and rising respectively. Our model predictions qualitatively match some of the puzzling features in the observed star formation history.
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References
How later papers used it
46 later papers cite it
2 later papers by other authors are listed below: 2 used its method or tool.
Uses its method or tool 2 of 4 papers with this label
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Computed neutral and molecular hydrogen from gas properties self-consistently, assuming self-shielding from another work and atomic/molecular separation based on this paper's subgrid model.
Hybrid analytic and machine-learned baryonic property insertion into galactic dark matter haloes (2020) · 1.00 · paraphrased: the licence does not allow quoting
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Since the quoted $Σ$ in these observations is inferred from the H$α$ luminosity by assuming a particular redshift-dependent molecular gas depletion time, but we use the [ref] star formation law (see Section [ref]), we use the quoted $Σ$ values to find the original estimated star formation rate surface density, then use the [ref] star formation law to infer $Σ$.
How Low Can Q Go? (2023) · Comparison to Data · 0.99
How the literature uses it
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For sizeable high-$z$ galaxies with $≈0.4-0.5$ [ref] and no outflows ($η=0$), we obtain $z_eq≈1.5-2.5$, in agreement with [ref] .
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We note that this scenario has also been referred to as a “reservoir" or “bath tub" model [ref] .
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A single pair-instability supernova from one of these stars pollutes its host halo up to a metallicity of $∼10^-3$ of solar [ref] .
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Another estimate based on SPH simulations [ref] gives similar values at high $z$ but somewhat smaller values, $ϵ_in ∼0.5$, at $z ∼2.5$.
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Cites as support 1 paper
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The distinction is important because it is not possible to produce Jeans masses as low as $∼M_⊙$ unless the gas can cool to $∼10$ K temperatures.] The subsequent numerical simulations of [ref] confirm this picture.
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Cites as background 1 paper
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Proposed mechanisms include photoionization by the UV background [ref] , and stellar feedback by supernovae [ref] or radiation pressure [ref] .
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