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The characteristic black hole mass resulting from direct collapse in the early universe
Cosmology and Nongalactic Astrophysics · Submitted 4 Sep 2013
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Our results show that the direct collapse model is clearly feasible as it provides the expected mass of the seed black holes.
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The abstract, sentence by sentence
Black holes of a billion solar masses are observed in the infant universe a few hundred million years after the Big Bang. The direct collapse of protogalactic gas clouds in primordial halos with $\rm T_{vir} \geq 10^{4} K$ provides the most promising way to assemble massive black holes. In this study, we aim to determine the characteristic mass scale of seed black holes and the time evolution of the accretion rates resulting from the direct collapse model. We explore the formation of supermassive black holes via cosmological large eddy simulations (LES) by employing sink particles and following their evolution for twenty thousand years after the formation of the first sink. As the resulting protostars were shown to have cool atmospheres in the presence of strong accretion, we assume here that UV feedback is negligible during this calculation. We confirm this result in a comparison run without sinks. Our findings show that black hole seeds with characteristic mass of $\rm 10^{5} M_{\odot}$ are formed in the presence of strong Lyman Werner flux which leads to an isothermal collapse. The characteristic mass is a about two times higher in LES compared to the implicit large eddy simulations (ILES). The accretion rates increase with time and reach a maximum value of 10 $\rm M_{\odot}/yr$ after $\rm 10^{4}$ years. Our results show that the direct collapse model is clearly feasible as it provides the expected mass of the seed black holes.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Black holes of a billion solar masses are observed in the infant universe a few hundred million years after the Big Bang. | background 1.00 | 0.08 | 0.03 | asserted 1.00 |
| s1 | The direct collapse of protogalactic gas clouds in primordial halos with $\rm T_{vir} \geq 10^{4} K$ provides the most promising way to assemble massive black holes. | background 0.99 | 0.07 | 0.05 | asserted 0.52 |
| s2 | In this study, we aim to determine the characteristic mass scale of seed black holes and the time evolution of the accretion rates resulting from the direct collapse model. | contribution 0.97 | 0.46 | 0.04 | unclear 0.63 |
| s3 | We explore the formation of supermassive black holes via cosmological large eddy simulations (LES) by employing sink particles and following their evolution for twenty thousand years after the formation of the first sink. | method 0.98 | 0.94 | 0.04 | asserted 0.88 |
| s4 | As the resulting protostars were shown to have cool atmospheres in the presence of strong accretion, we assume here that UV feedback is negligible during this calculation. | method 0.70 | 0.37 | 0.02 | asserted 0.98 |
| s5 | We confirm this result in a comparison run without sinks. | method 0.65 | 0.89 | 0.03 | asserted 1.00 |
| s6 | Our findings show that black hole seeds with characteristic mass of $\rm 10^{5} M_{\odot}$ are formed in the presence of strong Lyman Werner flux which leads to an isothermal collapse. | result 1.00 | 0.91 | 0.66 | asserted 1.00 |
| s7 | The characteristic mass is a about two times higher in LES compared to the implicit large eddy simulations (ILES). | result 1.00 | 0.86 | 0.10 | asserted 1.00 |
| s8 | The accretion rates increase with time and reach a maximum value of 10 $\rm M_{\odot}/yr$ after $\rm 10^{4}$ years. | result 1.00 | 0.93 | 0.09 | asserted 1.00 |
| s9 | Our results show that the direct collapse model is clearly feasible as it provides the expected mass of the seed black holes. | interpretation 0.97 | 0.87 | 0.78 | asserted 1.00 |
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The paper
Original abstract
Black holes of a billion solar masses are observed in the infant universe a few hundred million years after the Big Bang. The direct collapse of protogalactic gas clouds in primordial halos with $\rm T_{vir} \geq 10^{4} K$ provides the most promising way to assemble massive black holes. In this study, we aim to determine the characteristic mass scale of seed black holes and the time evolution of the accretion rates resulting from the direct collapse model. We explore the formation of supermassive black holes via cosmological large eddy simulations (LES) by employing sink particles and following their evolution for twenty thousand years after the formation of the first sink. As the resulting protostars were shown to have cool atmospheres in the presence of strong accretion, we assume here that UV feedback is negligible during this calculation. We confirm this result in a comparison run without sinks. Our findings show that black hole seeds with characteristic mass of $\rm 10^{5} M_{\odot}$ are formed in the presence of strong Lyman Werner flux which leads to an isothermal collapse. The characteristic mass is a about two times higher in LES compared to the implicit large eddy simulations (ILES). The accretion rates increase with time and reach a maximum value of 10 $\rm M_{\odot}/yr$ after $\rm 10^{4}$ years. Our results show that the direct collapse model is clearly feasible as it provides the expected mass of the seed black holes.
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References
How later papers used it
68 later papers cite it
1 paper by the same authors is listed below: 1 compared its own results with it.
Compares with it 1 of 4 papers with this label · 1 by the same authors
By the same authors
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We compared the results of the pressure floor method with sink particles in [ref] and [ref] and found that both methods yield similar results.
Role of magnetic fields in the formation of direct collapse black holes (2022) (same authors) · Conclusions and Discussion · 0.86
How the literature uses it
11 arXiv papers cite this in 12 sentences
Papers citing it · 5 sentences without a confident label
Uses its method or tool 1 paper
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This method is applied in [ref] to follow the accretion history of protostars in atomic cooling halos.
Large Eddy Simulations in Astrophysics · Gravitational collapse of gas in primordial halos · 0.84
Cites it as background 6 papers
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In this scenario, primordial gas collapses at temperatures of $∼10^4$K, suppressing fragmentation and enabling large gas inflow rates [ref] .
Abundant Heavy Black Hole Seeds from Moderate Lyman-Werner Radiation · Introduction · 0.86
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Possible scenarios to produce such massive seed BHs have been studied, e.g., through collapses of massive stars/gas clouds, or through mergers of massive stars/ black holes [ref] .
Cosmological 21cm line observations to test scenarios of super-Eddington accretion on to black holes being seeds of high-redshifted supermassive black holes · Introduction · 0.92
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The third are "heavy" seeds, commonly referred to as direct collapse black holes (DCBHs), with masses of $M_∙ ≳10^4 M_⊙$, which form from the collapsed cores of supermassive stars (SMSs) [ref] ; we will focus on this formation channel for the remainder of this paper.
Identification of Candidate Halos Hosting Massive Black Hole Seeds in the $\textit{Renaissance}$ Simulations with Support Vector Machines · Introduction · 0.96
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