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Mass Accretion Rates and Histories of Dark Matter Haloes

Cosmology and Nongalactic Astrophysics · Submitted 23 Feb 2009

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim We find only about 25% of the haloes to have MAHs that are well described by a 1-parameter exponential form.

how it is stated · asserted 1.00 read the record →

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arXiv ID0902.3659 (version 2)
Pith ID7UGIX6V4, Pith's permanent record of this paper and its review
CitationChung-Pei Ma, James McBride, Onsi Fakhouri. "Mass Accretion Rates and Histories of Dark Matter Haloes." arXiv:0902.3659 (2009). https://pith.science/paper/7UGIX6V4
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The compiled record

The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 8,556 input tokens, $0.0004 reported.

What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.42 · human participants 0.01 · controlled comparison 0.14 · randomized assignment 0.01 · states quantitative result 0.99 · compares with prior results 0.42 · mentions code or data availability 0.03.

The abstract, sentence by sentence

arXiv listing abstract v2. Results and the main claim are underlined; .

We use the extensive catalog of dark matter haloes from the Millennium simulation to investigate the statistics of the mass accretion histories (MAHs) and accretion rates of ~500,000 haloes from redshift z=0 to 6. We find only about 25% of the haloes to have MAHs that are well described by a 1-parameter exponential form. For the rest of the haloes, between 20% (Milky-Way mass) to 50% (cluster mass) experience late-time growth that is steeper than an exponential, whereas the remaining haloes show plateau-ed late-time growth that is shallower than an exponential. The haloes with slower late-time growth tend to reside in denser environments, suggesting that either tidal stripping or the "hotter" dynamics are suppressing the accretion rate of dark matter onto these haloes. These deviations from exponential growth are well fit by introducing a second parameter: M(z) \propto (1+z)^beta exp(-gamma z). The full distribution of beta and gamma as a function of halo mass is provided. From the analytic form of M(z), we obtain a simple formula for the mean accretion rate of dark matter, dM/dt, as a function of redshift and mass. At z=0, this rate is 42 Msun/yr for 1e12 Msun haloes, which corresponds to a mean baryon accretion rate of dMbaryon/dt=7 Msun/yr. This mean rate increases approximately as (1+z)^1.5 at low z and (1+z)^2.5 at high z, reaching dMbaryon/dt = 27, 69, and 140 Msun/yr at z=1, 2, and 3. The specific rate depends on halo mass weakly: dlogM/dt \propto M^0.127. Results for the broad distributions about the mean rates are also discussed.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 We use the extensive catalog of dark matter haloes from the Millennium simulation to investigate the statistics of the mass accretion histories (MAHs) and accretion rates of ~500,000 haloes from redshift z=0 to 6. method 0.68 0.95 0.04 asserted 0.92
s1 We find only about 25% of the haloes to have MAHs that are well described by a 1-parameter exponential form. result 1.00 0.97 0.21 asserted 1.00
s2 For the rest of the haloes, between 20% (Milky-Way mass) to 50% (cluster mass) experience late-time growth that is steeper than an exponential, whereas the remaining haloes show plateau-ed late-time growth that is shallower than an exponential. result 1.00 0.95 0.24 asserted 1.00
s3 The haloes with slower late-time growth tend to reside in denser environments, suggesting that either tidal stripping or the "hotter" dynamics are suppressing the accretion rate of dark matter onto these haloes. interpretation 0.97 0.85 0.10 hedged possibility 0.99
s4 These deviations from exponential growth are well fit by introducing a second parameter: M(z) \propto (1+z)^beta exp(-gamma z). result 0.74 0.92 0.21 asserted 1.00
s5 The full distribution of beta and gamma as a function of halo mass is provided. result 0.77 0.94 0.08 asserted 0.97
s6 From the analytic form of M(z), we obtain a simple formula for the mean accretion rate of dark matter, dM/dt, as a function of redshift and mass. result 0.50 0.95 0.11 asserted 1.00
s7 At z=0, this rate is 42 Msun/yr for 1e12 Msun haloes, which corresponds to a mean baryon accretion rate of dMbaryon/dt=7 Msun/yr. result 1.00 0.92 0.09 asserted 1.00
s8 This mean rate increases approximately as (1+z)^1.5 at low z and (1+z)^2.5 at high z, reaching dMbaryon/dt = 27, 69, and 140 Msun/yr at z=1, 2, and 3. result 1.00 0.94 0.09 asserted 0.99
s9 The specific rate depends on halo mass weakly: dlogM/dt \propto M^0.127. result 1.00 0.93 0.06 asserted 1.00
s10 Results for the broad distributions about the mean rates are also discussed. result 0.70 0.85 0.03 unclear 0.64

What kind of paper the classifier reports this is: simulation study 1.00 · evidence from simulation or computation 0.77.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

We use the extensive catalog of dark matter haloes from the Millennium simulation to investigate the statistics of the mass accretion histories (MAHs) and accretion rates of ~500,000 haloes from redshift z=0 to 6. We find only about 25% of the haloes to have MAHs that are well described by a 1-parameter exponential form. For the rest of the haloes, between 20% (Milky-Way mass) to 50% (cluster mass) experience late-time growth that is steeper than an exponential, whereas the remaining haloes show plateau-ed late-time growth that is shallower than an exponential. The haloes with slower late-time growth tend to reside in denser environments, suggesting that either tidal stripping or the "hotter" dynamics are suppressing the accretion rate of dark matter onto these haloes. These deviations from exponential growth are well fit by introducing a second parameter: M(z) \propto (1+z)^beta exp(-gamma z). The full distribution of beta and gamma as a function of halo mass is provided. From the analytic form of M(z), we obtain a simple formula for the mean accretion rate of dark matter, dM/dt, as a function of redshift and mass. At z=0, this rate is 42 Msun/yr for 1e12 Msun haloes, which corresponds to a mean baryon accretion rate of dMbaryon/dt=7 Msun/yr. This mean rate increases approximately as (1+z)^1.5 at low z and (1+z)^2.5 at high z, reaching dMbaryon/dt = 27, 69, and 140 Msun/yr at z=1, 2, and 3. The specific rate depends on halo mass weakly: dlogM/dt \propto M^0.127. Results for the broad distributions about the mean rates are also discussed.

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References
How later papers used it

66 later papers cite it

Evidence: substantial. 65 of the citing papers share no author with it, and 21 of those carry a confident label from Pith's citation classifier.

Pith read 22 of the 104 citing sentences, choosing only those whose citation markers point at this paper alone, and wrote the paraphrases from them. The summary, the counts, the evidence level, the links and the quotes come from code; the summary counts the papers listed below. A later paper is listed under a label when Pith's citation classifier gives one of its sentences that label at probability 0.8 or more (0.95 for support), Pith's reading finds that the citing paper itself did it, and a second check confirms the paraphrase against the sentence. This section lists uses only. It does not list criticism or disagreement, so their absence here says nothing about how the paper has been received. Papers that share an author with this one are listed apart, under "By the same authors". A quote is the citing authors' own sentence, shown when their paper's licence is CC BY, CC BY-SA or CC0. JSON

Uses its method or tool 3 of 10 papers with this label
Uses its data or values 2 of 6 papers with this label
Compares with it 1 of 5 papers with this label
  • Compared its own median mass accretion history of the Auriga suite with this paper's curve, finding it coincident for z<1 and roughly following it for z>2.

    The Hestia project: simulations of the Local Group (2020) · 0.85 · paraphrased: the licence does not allow quoting

How the literature uses it

7 arXiv papers cite this in 11 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 7 sentences without a confident label

Uses its data or values 1 paper
  • We begin with the dark matter accretion rate from [ref] and [ref] , which quantified the mass accretion histories of all dark matter halos with masses above $∼10^10$ M$_⊙$ in the two Millennium simulations of a $Λ$CDM universe [ref] .

    The Gas Consumption History to z ~ 4 · Comparing $d/dt$ to Dark Matter Accretion Rate · 0.98

Compares with it 1 paper
Cites it as support 1 paper
Cites it as background 1 paper
  • A more stringent test is to consider the mass accretion history[for a discussion of the statistical properties of mass accretion histories, see [ref] .] for each Aquarius halo and to compare results from the Aquarius resimulations and from the .

    Resolving Cosmic Structure Formation with the Millennium-II Simulation · Comparing Aquarius and Millennium-II halos · 0.96

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