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We then analyze the continuum limit of the quadratic coefficient and show that it separates into a Gaussian contribution, a \(D\)-channel, and a \(\beta\)-channel. The naive Gaussian term becomes trivial, while the exact holonomy kernel generates finite continuum contributions through singular dependence on the endpoint Gaussian width and anisotropic coupling.
We then study the geometry of the holonomy potential and show that its relevant saddle is a constrained boundary saddle on the aligned branch, rather than an unconstrained critical point. The associated transverse expansion captures the local saddle geometry, but any finite polynomial truncation has a trivial continuum limit. Finally, we introduce a non-polynomial toy model based on \(V_{\rm toy}(B)=-\log\cosh B\), which provides a completion of the transverse expansion and reproduces exactly the continuum \(D\)-channel contribution \(-2d\). This prepares the geometric interpretation of the \(D\)-channel as a Wishart--Stiefel entropy associated with an emergent four-dimensional geometry embedded \(\mathbb R^d\) in the endpoint formulation.
| Comments: | BFSS/BMN Matrix Quantum Mechanics IV |
| Subjects: | High Energy Physics - Theory (hep-th); General Relativity and Quantum Cosmology (gr-qc); High Energy Physics - Lattice (hep-lat); High Energy Physics - Phenomenology (hep-ph); Mathematical Physics (math-ph) |
| Cite as: | arXiv:2605.25647 [hep-th] |
| (or arXiv:2605.25647v1 [hep-th] for this version) | |
| https://doi.org/10.48550/arXiv.2605.25647 arXiv-issued DOI via DataCite (pending registration) |
From: Badis Ydri [view email]
[v1]
Mon, 25 May 2026 09:53:14 UTC (270 KB)
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