JWST SMBH Seeds (Z=10, 10^9 M_SUN)

The detection of supermassive black holes of ~10⁹ solar masses at z ∼ 10 — only ~500 million years after the Big Bang — is simply irreconcilable with ΛCDM unless one invokes continuous super-Eddington accretion from stellar-mass seeds for the entire available time with negligible feedback, a scenario that is both physically implausible and observationally unsupported. Successive Collision Theory eliminates the problem at its root by recognizing that the most massive early SMBHs were never stellar-mass seeds. The post-collision plasma was a superhot pre-baryonic fluid whose temperature was initially above the electroweak scale. As it cooled, the angular momentum gradients inherited from the collision geometry produced regions of dramatically different density. In the overdense swirling nodes, gravitational focusing concentrated plasma energy until the enclosed stress-energy exceeded the Schwarzschild threshold — before the plasma had cooled enough for quarks to confine, before hadrons existed, before the fine structure constant governed electromagnetic interactions. Those regions collapsed directly into black holes from the pre-baryonic plasma. A 10⁹ solar mass object at z ∼ 10 is not the product of 500 million years of accretion; it is a remnant of a direct-collapse event that occurred during the thermalization cooling epoch, potentially within the first millions of years after the collision.

The quark degeneracy pressure mechanism in SCT is directly relevant here: as the most overdense plasma nodes collapsed, the QCD-derived lower boundary on GR's domain prevented a true singularity from forming, establishing instead a finite-density polyquark core. The result is a stable, massive compact object whose interior is supported by quark degeneracy pressure rather than terminated at a mathematical singularity — a physically self-consistent outcome that standard GR without the SCT QCD modification cannot produce for pre-baryonic collapse events. The mass of the resulting object is set by the mass-energy of the plasma within the Schwarzschild radius at the moment of crossing, which for the densest collision geometry nodes is naturally in the range of 10⁸ to 10¹⁰ solar mass equivalents.

The gravitational superposition from overlapping nested comoving frames further enhances the effective gravitational depth of the highest-density plasma nodes during the cooling epoch. The superposition term adds effective gravitational influence above what the plasma mass alone provides, accelerating the crossing of the Schwarzschild threshold in the densest regions and setting a higher effective floor on the minimum mass of direct-collapse objects. This means that the SCT direct-collapse channel preferentially produces high-mass compact objects — naturally explaining why the JWST-observed early SMBHs are already at 10⁸ to 10⁹ solar masses rather than showing the broad mass distribution expected from stellar seed accretion. These are not grown objects; they are the direct fossil record of the collision's most overdense angular momentum nodes, preserved as massive black holes at the centers of the earliest galaxies.