Early formation of supermassive black holes from the collapse of strongly self-interacting dark matter
arXiv:2410.17480 · doi:10.1088/1475-7516/2025/01/060
Abstract
Evidence for high-redshift supermassive black holes challenges standard scenarios for how such objects form in the early universe. Here, we entertain the possibility that a fraction of the cosmological dark matter could be ultra-strongly self interacting. This would imply that gravothermal collapse occur at early times in the cores of dark matter halos, followed by accretion. We study under which conditions on the abundance and interaction strength and structure of such ultra self-interacting dark matter the black holes resulting from the end-point of gravothermal core collapse can seed the observed, early-forming supermassive black holes. We find, depending on the velocity dependence of the self-interaction cross section, a bimodal structure in the favored parameter space, where data points to either a small collapsing dark matter fraction with a large cross section, or a large fraction and a relatively small cross section. While self-interaction cross sections with different velocity dependence can explain observations, we find that the best, self-consistent results correspond to a Rutherford-like self-interaction, typical of long-range dark-sector forces with light mediators. We discuss complementary observational probes if this scenario is realized in nature, focusing especially on the expected intermediate mass black holes predicted to exist in smaller galaxies.
arXiv comment28 pages, 6 Figures; matches published version in JCAP, includes a few additional references
References in corpus (97)
- emcee: The MCMC Hammer
- Planck 2015 results. XIII. Cosmological parameters
- A Universal Density Profile from Hierarchical Clustering
- Planck 2013 results. XVI. Cosmological parameters
- Observational evidence for self-interacting cold dark matter
- The James Webb Space Telescope
- A Catalog of Quasar Properties from SDSS DR7
- Too big to fail? The puzzling darkness of massive Milky Way subhaloes
- Determining Central Black Hole Masses in Distant Active Galaxies and Quasars. II. Improved Optical and UV Scaling Relationships
- Simulating galaxy formation with black hole driven thermal and kinetic feedback
- Dark Matter Self-interactions and Small Scale Structure
- The First Stars
- Formation of Supermassive Black Holes by Direct Collapse in Pregalactic Halos
- Formation of the First Supermassive Black Holes
- Observational and Theoretical Constraints on Singular Dark Matter Halos
- Formation of Supermassive Black Holes
- The Milky Way's bright satellites as an apparent failure of LCDM
- The Assembly of the First Massive Black Holes
- The cosmological evolution of quasar black-hole masses
- Dwarf Galaxies with Optical Signatures of Active Massive Black Holes
- Beyond Collisionless Dark Matter: Particle Physics Dynamics for Dark Matter Halo Structure
- How Do Massive Black Holes Get Their Gas?
- COLOSSUS: A python toolkit for cosmology, large-scale structure, and dark matter halos
- The unexpected diversity of dwarf galaxy rotation curves
- Supermassive black holes and their feedback effects in the IllustrisTNG simulation
- Dark Matter Scaling Relations
- Hidden Charged Dark Matter
- Halo Properties in Cosmological Simulations of Self-Interacting Cold Dark Matter
- Cores in Dwarf Galaxies from Dark Matter with a Yukawa Potential
- The SIMPlest Miracle
- Nuclear Star Clusters
- Collapse of Primordial Gas Clouds and the Formation of Quasar Black Holes
- Rapid growth of high redshift black holes
- Core Formation in Dwarf Halos with Self Interacting Dark Matter: No Fine-Tuning Necessary
- Formation of the first nuclear clusters and massive black holes at high redshift
- Fragmentation of star-forming clouds enriched with the first dust
- Observational evidence for intermediate-mass black holes
- Weakly Self-Interacting Dark Matter and the Structure of Dark Halos
- Accretion onto the First Stellar Mass Black Holes
- The Assembly of Supermassive Black Holes at High Redshifts
- How the Self-Interacting Dark Matter Model Explains the Diverse Galactic Rotation Curves
- An accurate physical model for halo concentrations
- Super-Critical Growth of Massive Black Holes from Stellar-Mass Seeds
- Self-Interacting Dark Matter Halos and the Gravothermal Catastrophe
- A 400 solar mass black hole in the Ultraluminous X-ray source M82 X-1 accreting close to its Eddington limit
- Evidence for non-evolving FeII/MgII ratios in rapidly accreting z~6 QSOs
- A ~50,000 solar mass black hole in the nucleus of RGG 118
- An intermediate-mass black hole in the centre of the globular cluster 47 Tucanae
- Collapse of a Rotating Supermassive Star to a Supermassive Black Hole: Fully Relativistic Simulations
- The case for super-critical accretion onto massive black holes at high redshift
- The aftermath of the first stars: massive black holes
- Accretion onto Seed Black Holes in the First Galaxies
- The Formation Rates of Population III Stars and Chemical Enrichment of Halos during the Reionization Era
- Gravothermal collapse of isolated self-interacting dark matter haloes: N-body simulation versus the fluid model
- Active galactic nuclei at z~1.5: II. Black Hole Mass estimation by means of broad emission lines
- Supermassive Black Holes from Ultra-Strongly Self-Interacting Dark Matter
- The erratic dynamical life of black hole seeds in high-redshift galaxies
- Super-Eddington growth of the first black holes
- A Quantitative Study of Interacting Dark Matter in Halos
- Constraining Dissipative Dark Matter Self-Interactions
- Structure and Subhalo Population of Halos in a Self-Interacting Dark Matter Cosmology
- Constraining Velocity-dependent Self-Interacting Dark Matter with the Milky Way's dwarf spheroidal galaxies
- Reconciling the Diversity and Uniformity of Galactic Rotation Curves with Self-Interacting Dark Matter
- Accelerated core collapse in tidally stripped self-interacting dark matter halos
- Velocity-dependent Self-interacting Dark Matter from Groups and Clusters of Galaxies
- The X-shooter/ALMA Sample of Quasars in the Epoch of Reionization. II. Black Hole Masses, Eddington Ratios, and the Formation of the First Quasars
- Formation of the Black Holes in the Highest Redshift Quasars
- Metallicity Evolution in the Early Universe
- Core Formation in Galactic Nuclei Due to Recoiling Black Holes
- The Growth of Black Holes from Population III Remnants in the Renaissance Simulations
- Gravothermal Collapse of Self-Interacting Dark Matter Halos and the Origin of Massive Black Holes
- Fast-moving stars around an intermediate-mass black hole in Omega Centauri
- XQR-30: the ultimate XSHOOTER quasar sample at the reionization epoch
- Cosmic abundances of SIMP dark matter
- Diversity in density profiles of self-interacting dark matter satellite halos
- The impact of baryonic discs on the shapes and profiles of self-interacting dark matter halos
- Seeding Supermassive Black Holes with Self-Interacting Dark Matter: A Unified Scenario with Baryons
- The diverse dark matter density at sub-kiloparsec scales in Milky Way satellites:implications for the nature of dark matter
- The Onset of Gravothermal Core Collapse in Velocity Dependent Self-Interacting Dark Matter Subhaloes
- Velocity Dependence from Resonant Self-Interacting Dark Matter
- Dense gas formation and destruction in a simulated Perseus-like galaxy cluster with spin-driven black hole feedback
- Early formation of supermassive black holes via dark matter self-interactions
- Mass estimates from stellar proper motions: The mass of Centauri
- Universal gravothermal evolution of isolated self-interacting dark matter halos for velocity-dependent cross sections
- Motivations for a Large Self-Interacting Dark Matter Cross Section from Milky Way Satellites
- A Practical and Consistent Parametrization of Dark Matter Self-Interactions
- Black hole mass estimates in quasars - A comparative analysis of high- and low-ionization lines
- Production of dark-matter bound states in the early universe by three-body recombination
- SMBH Seeds from Dissipative Dark Matter
- Demographics of z ~ 6 Quasars in the Black Hole Mass-Luminosity Plane
- Hyper-Eddington Black Hole Growth in Star-Forming Molecular Clouds and Galactic Nuclei: Can It Happen?
- Direct-collapse supermassive black holes from relic particle decay
- The most massive Population III stars
- Feeding plankton to whales: high-redshift supermassive black holes from tiny black hole explosions
- Gravothermal Catastrophe in Resonant Self-interacting Dark Matter Models
- Physical Pathways for JWST-Observed Supermassive Black Holes in the Early Universe
- The First Stellar Cluster