The Formation of Direct Collapse Black Holes at Cosmic Dawn and 21 cm Global Spectrum

Abstract JWST reveals numerous high- z galaxies and supermassive black holes (SMBHs), suggesting that stars and SMBH seeds formation at z ≳ 10 may be more efficient than previously derived. One popular SMBH seed scenario is the direct collapse black holes (DCBHs) formed in pristine atomic-cooling halos irradiated by nearby galaxies. Therefore, the efficient star formation likely facilitates the formation of DCBH. We calculate the first critical <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msub> <mml:mi>k</mml:mi> <mml:msub> <mml:mi mathvariant="normal">H</mml:mi> <mml:mn>2</mml:mn> </mml:msub> </mml:msub> <mml:mo>‒</mml:mo> <mml:msub> <mml:mi>k</mml:mi> <mml:msup> <mml:mi mathvariant="normal">H</mml:mi> <mml:mo>−</mml:mo> </mml:msup> </mml:msub> </mml:math> curves for DCBH formation under the influence of X-ray radiation using the one-zone model. We then build the UV luminosity function consistent with JWST observations and incorporate it into the model that calculates the DCBH-triggering probability. We confirm that enhanced star formation promotes the DCBH formation. However, the DCBH abundance n DCBH is significantly influenced by the X-ray radiation that is also related to star formation. Since the 21 cm global spectrum is also X-ray dependent, the 21 cm absorption depth <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>δ</mml:mi> <mml:msubsup> <mml:mrow> <mml:mi>T</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>b</mml:mi> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">trough</mml:mi> </mml:mrow> </mml:msubsup> </mml:math> at Cosmic Dawn encodes the DCBH abundance information. We provide a tentative trend in the n DCBH – <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>δ</mml:mi> <mml:msubsup> <mml:mrow> <mml:mi>T</mml:mi> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">b</mml:mi> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">trough</mml:mi> </mml:mrow> </mml:msubsup> </mml:math> relation, which could be a useful guide. In our fiducial model, if <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>δ</mml:mi> <mml:msubsup> <mml:mrow> <mml:mi>T</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>b</mml:mi> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">trough</mml:mi> </mml:mrow> </mml:msubsup> <mml:mo>≳</mml:mo> <mml:mo>−</mml:mo> <mml:mn>100</mml:mn> </mml:math> mK, then the DCBH is rather rare; if <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mo>−</mml:mo> <mml:mn>150</mml:mn> <mml:mspace width="0.25em"/> <mml:mi>mK</mml:mi> <mml:mo>≲</mml:mo> <mml:mi>δ</mml:mi> <mml:msubsup> <mml:mi>T</mml:mi> <mml:mi>b</mml:mi> <mml:mi>trough</mml:mi> </mml:msubsup> <mml:mo>≲</mml:mo> <mml:mo>−</mml:mo> <mml:mn>100</mml:mn> </mml:math> mK, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msub> <mml:mrow> <mml:mi>n</mml:mi> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">DCBH</mml:mi> </mml:mrow> </mml:msub> <mml:mo>∼</mml:mo> <mml:mi class="MJX-tex-calligraphic" mathvariant="script">O</mml:mi> <mml:mo stretchy="false">(</mml:mo> <mml:mn>1</mml:mn> <mml:msup> <mml:mrow> <mml:mn>0</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>2</mml:mn> </mml:mrow> </mml:msup> <mml:mo>−</mml:mo> <mml:mn>1</mml:mn> <mml:msup> <mml:mrow> <mml:mn>0</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>3</mml:mn> </mml:mrow> </mml:msup> <mml:mo stretchy="false">)</mml:mo> </mml:math> cMpc −3 (comoving Mpc −3 ), consistent with the HST/JWST observed SMBHs abundance at z ≳ 6; if <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>δ</mml:mi> <mml:msubsup> <mml:mrow> <mml:mi>T</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>b</mml:mi> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">trough</mml:mi> </mml:mrow> </mml:msubsup> <mml:mo>≲</mml:mo> <mml:mo>−</mml:mo> <mml:mn>150</mml:mn> </mml:math> mK, n DCBH can largely exceed <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi class="MJX-tex-calligraphic" mathvariant="script">O</mml:mi> <mml:mo stretchy="false">(</mml:mo> <mml:mn>1</mml:mn> <mml:msup> <mml:mrow> <mml:mn>0</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>2</mml:mn> </mml:mrow> </mml:msup> <mml:mo stretchy="false">)</mml:mo> </mml:math> cMpc −3 . The 21 cm global spectrum observations will help to constrain the DCBH abundance.

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Publication Details

Journal
The Astrophysical Journal
Published
2025-05-02
DOI
https://doi.org/10.3847/1538-4357/adc730
Citations
2
Primary Topic
Radio Astronomy Observations and Technology
Type
article
Field-Weighted Citation Impact
2.31

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article

The Formation of Direct Collapse Black Holes at Cosmic Dawn and 21 cm Global Spectrum

Yidong Xu, Andrea Ferrara, Bin Yue, Meng Zhang
2 citations
The Astrophysical Journal
Radio Astronomy Observations and Technology
2.31
article

The Formation of Direct Collapse Black Holes at Cosmic Dawn and 21 cm Global Spectrum

Yidong Xu, Andrea Ferrara, Bin Yue, Meng Zhang
article en
2 citations

Abstract

Abstract JWST reveals numerous high- z galaxies and supermassive black holes (SMBHs), suggesting that stars and SMBH seeds formation at z ≳ 10 may be more efficient than previously derived. One popular SMBH seed scenario is the direct collapse black holes (DCBHs) formed in pristine atomic-cooling halos irradiated by nearby galaxies. Therefore, the efficient star formation likely facilitates the formation of DCBH. We calculate the first critical <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msub> <mml:mi>k</mml:mi> <mml:msub> <mml:mi mathvariant="normal">H</mml:mi> <mml:mn>2</mml:mn> </mml:msub> </mml:msub> <mml:mo>‒</mml:mo> <mml:msub> <mml:mi>k</mml:mi> <mml:msup> <mml:mi mathvariant="normal">H</mml:mi> <mml:mo>−</mml:mo> </mml:msup> </mml:msub> </mml:math> curves for DCBH formation under the influence of X-ray radiation using the one-zone model. We then build the UV luminosity function consistent with JWST observations and incorporate it into the model that calculates the DCBH-triggering probability. We confirm that enhanced star formation promotes the DCBH formation. However, the DCBH abundance n DCBH is significantly influenced by the X-ray radiation that is also related to star formation. Since the 21 cm global spectrum is also X-ray dependent, the 21 cm absorption depth <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>δ</mml:mi> <mml:msubsup> <mml:mrow> <mml:mi>T</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>b</mml:mi> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">trough</mml:mi> </mml:mrow> </mml:msubsup> </mml:math> at Cosmic Dawn encodes the DCBH abundance information. We provide a tentative trend in the n DCBH – <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>δ</mml:mi> <mml:msubsup> <mml:mrow> <mml:mi>T</mml:mi> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">b</mml:mi> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">trough</mml:mi> </mml:mrow> </mml:msubsup> </mml:math> relation, which could be a useful guide. In our fiducial model, if <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>δ</mml:mi> <mml:msubsup> <mml:mrow> <mml:mi>T</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>b</mml:mi> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">trough</mml:mi> </mml:mrow> </mml:msubsup> <mml:mo>≳</mml:mo> <mml:mo>−</mml:mo> <mml:mn>100</mml:mn> </mml:math> mK, then the DCBH is rather rare; if <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mo>−</mml:mo> <mml:mn>150</mml:mn> <mml:mspace width="0.25em"/> <mml:mi>mK</mml:mi> <mml:mo>≲</mml:mo> <mml:mi>δ</mml:mi> <mml:msubsup> <mml:mi>T</mml:mi> <mml:mi>b</mml:mi> <mml:mi>trough</mml:mi> </mml:msubsup> <mml:mo>≲</mml:mo> <mml:mo>−</mml:mo> <mml:mn>100</mml:mn> </mml:math> mK, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msub> <mml:mrow> <mml:mi>n</mml:mi> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">DCBH</mml:mi> </mml:mrow> </mml:msub> <mml:mo>∼</mml:mo> <mml:mi class="MJX-tex-calligraphic" mathvariant="script">O</mml:mi> <mml:mo stretchy="false">(</mml:mo> <mml:mn>1</mml:mn> <mml:msup> <mml:mrow> <mml:mn>0</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>2</mml:mn> </mml:mrow> </mml:msup> <mml:mo>−</mml:mo> <mml:mn>1</mml:mn> <mml:msup> <mml:mrow> <mml:mn>0</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>3</mml:mn> </mml:mrow> </mml:msup> <mml:mo stretchy="false">)</mml:mo> </mml:math> cMpc −3 (comoving Mpc −3 ), consistent with the HST/JWST observed SMBHs abundance at z ≳ 6; if <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>δ</mml:mi> <mml:msubsup> <mml:mrow> <mml:mi>T</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>b</mml:mi> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">trough</mml:mi> </mml:mrow> </mml:msubsup> <mml:mo>≲</mml:mo> <mml:mo>−</mml:mo> <mml:mn>150</mml:mn> </mml:math> mK, n DCBH can largely exceed <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi class="MJX-tex-calligraphic" mathvariant="script">O</mml:mi> <mml:mo stretchy="false">(</mml:mo> <mml:mn>1</mml:mn> <mml:msup> <mml:mrow> <mml:mn>0</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>2</mml:mn> </mml:mrow> </mml:msup> <mml:mo stretchy="false">)</mml:mo> </mml:math> cMpc −3 . The 21 cm global spectrum observations will help to constrain the DCBH abundance.

The Astrophysical JournalVol. 984(2)
National Natural Science Foundation of China
Openalex Percentile: Top 12%
Radio Astronomy Observations and Technology
2.31
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