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arXiv:2601.13764

Quantum Entanglement Geometry on Severi-Brauer Schemes: Subsystem Reductions of Azumaya Algebras

Kazuki Ikeda

math.AGhep-thmath-phmath.RAquant-phSubmitted Jan 20, 2026• Announced Jan 21, 2026• 0 citations• Revised Aug 5, 2026 (v3)
v1 · Jan 20, 2026v2 · Jan 26, 2026v3 · Aug 5, 2026
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Abstract

Quantum entanglement is a basic resource of quantum theory, but its usual definition assumes a fixed decomposition into subsystems. We develop an algebro--geometric framework to address quantum entanglement. For the Severi--Brauer scheme $SB(\mathcal{A})\to X$ of an Azumaya algebra and a factorization type $\mathbf{d}$, we prove that a global locus of product states exists exactly when the associated torsor under $\mathrm{PGL}_n$ reduces to the stabilizer $G_{\mathbf d}$ of the Segre variety. Thus entanglement in families is measured by a geometric obstruction to global subsystem structure. Beyond this reduction criterion, we identify the cohomology that carries computable entangling obstructions. After determinant and incidence data $L\subset R\subset K$ are chosen, the relevant classes lie in the mapping cone relative cohomology $E^\bullet(BL\to BR)$. Their absolute images on $X$, modulo classes induced from $BK$, give determinant entangling obstructions beyond the Brauer class. We construct the moduli of subsystem structures as the quotient $P/G_{\mathbf d}$ and realize it as a locally closed locus in the relative Hilbert scheme, with a compactification by degenerations of product state loci. In the bipartite case, a chosen subsystem structure globalizes the Schmidt rank stratification to a flat filtration with base change compatible resolutions and fiberwise constant numerical invariants. Examples show that reducibility can depend on the underlying torsor, not only on the Brauer class, with an interpretation by entangling monodromy.

Comments
An introductory note to this article is provided in arXiv:2601.19111. Concrete applications to physics studies can be found in arXiv:2608.03634 and arXiv:2604.11596

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Quantum entanglement is a basic resource of quantum theory, but its usual definition assumes a fixed decomposition into subsystems. We develop an algebro--geometric framework to address quantum entanglement. For the Severi--Brauer scheme SB(A)→XSB(\mathcal{A})\to XSB(A)→X of an Azumaya algebra and a factorization type d\mathbf{d}d, we prove that a global locus of product states exists exactly when the associated torsor under PGLn\mathrm{PGL}_nPGLn​ reduces to the stabilizer GdG_{\mathbf d}Gd​ of the Segre variety. Thus entanglement in families is measured by a geometric obstruction to global subsystem structure.
Beyond this reduction criterion, we identify the cohomology that carries computable entangling obstructions. After determinant and incidence data L⊂R⊂KL\subset R\subset KL⊂R⊂K are chosen, the relevant classes lie in the mapping cone relative cohomology E∙(BL→BR)E^\bullet(BL\to BR)E∙(BL→BR). Their absolute images on XXX, modulo classes induced from BKBKBK, give determinant entangling obstructions beyond the Brauer class. We construct the moduli of subsystem structures as the quotient P/GdP/G_{\mathbf d}P/Gd​ and realize it as a locally closed locus in the relative Hilbert scheme, with a compactification by degenerations of product state loci. In the bipartite case, a chosen subsystem structure globalizes the Schmidt rank stratification to a flat filtration with base change compatible resolutions and fiberwise constant numerical invariants. Examples show that reducibility can depend on the underlying torsor, not only on the Brauer class, with an interpretation by entangling monodromy.
This article is an expository account aimed at viewing entanglement in finite-dimensional quantum many-body systems as a phenomenon of global geometry. While the mathematics of general quantum states has been studied extensively, this article focuses specifically on their entanglement. When a quantum system varies over a classical parameter space, each fiber may look like the same Hilbert space, yet there may be no global identification because of twisting in the gluing data. Describing this situation by an Azumaya algebra, one always obtains the family of pure-state spaces as a Severi-Brauer scheme. The main focus is to characterize the condition under which the subsystem decomposition required to define entanglement exists globally and compatibly, by a reduction to the stabilizer subgroup of the Segre variety, and to explain that the obstruction appears in the Brauer class. As a consequence, quantum states yield a natural filtration dictated by entanglement on the Severi-Brauer scheme. Using a spin system on a torus as an example, we show concretely that the holonomy of the gluing can produce an entangling quantum gate, and can appear as an obstruction class distinct from the usual Berry numbers or Chern numbers. For instance, even for quantum systems that have traditionally been regarded as having no topological band structure, the entanglement of their eigenstates can be related to global geometric universal quantities, reflecting the background geometry.
We recast quantum entanglement as a cohomological obstruction to reconstructing a global quantum state from locally compatible information. We address this by considering presheaf cohomologies of states and entanglement witnesses. Sheafification erases the global-from-local signature while leaving within-patch multipartite structure, captured by local entanglement groups introduced here. For smooth parameter families, the obstruction admits a differential-geometric representative obtained by pairing an appropriate witness field with the curvature of a natural unitary connection on the associated bundle of amplitudes. We also introduce a Quantum Entanglement Index (QEI) as an index-theoretic invariant of entangled states and explain its behavior. Finally, we outline a theoretical physics approach to probe these ideas in quantum many-body systems and suggest a possible entanglement-induced correction as an experimental validation. Detailed numerical implementations for concrete quantum many-body models are presented in the companion paper \cite{2026arXiv260113467I}.
Abstract We introduce a geometric framework for representing quantum entanglementthrough reduced entanglement coordinates derived from the Schmidt decompo-sition. For pure two-qubit states, the framework yields an entanglement conein which separability corresponds to geometric collapse to the cone apex. Thisconstruction extends naturally to higher-rank bipartitions through Schmidt-simplex geometries associated with Schmidt-rank reduction. For multipartitesystems, we introduce entanglement-graph coordinates that use pairwise bipar-tite reductions as geometric probes of global quantum states. The resultingrepresentation defines a local-unitary-invariant reduced geometry whose dimen-sion scales quadratically with subsystem number, compared with the exponentialscaling of the underlying pure-state space. Although not a complete invariantof multipartite entanglement, the graph geometry preserves important rela-tional and connectivity structure while remaining computationally tractable.Building on this representation, we develop a geometric interpretation of vari-ational quantum dynamics in which optimization trajectories evolve throughstructured regions of entanglement-graph space. We introduce Hamiltonian-selected entanglement-graph sectors, establish exact and perturbative sectorconstructions, derive local graph-distance energy relations near nondegenerateoptima, and develop learned geometric diagnostics for variational optimization.Numerical experiments on molecular and spin-chain Hamiltonians support thehypothesis that low-energy states concentrate near Hamiltonian-dependent graphsectors and demonstrate predictive information in the resulting geometric rep-resentations. Together, these results provide a unified geometric framework foranalyzing entanglement structure, quantum dynamics, and variational quantumoptimization.
This work explores the interplay between quantum information theory, algebraic geometry, and number theory, with a particular focus on multiqubit systems, their entanglement structure, and their classification via geometric embeddings. The Segre embedding, a fundamental construction in algebraic geometry, provides an algebraic framework to distinguish separable and entangled states, encoding quantum correlations in projective geometry. We develop a systematic study of qubit moduli spaces, illustrating the geometric structure of entanglement through hypercube constructions and Coxeter chamber decompositions. We establish a bijection between the Segre embeddings of tensor products of projective spaces and binary words of length n−1n-1n−1, structured as an (n−1)(n-1)(n−1)-dimensional hypercube, where adjacency corresponds to a single Segre operation. This reveals a combinatorial structure underlying the hierarchy of embeddings, with direct implications for quantum error correction schemes. The symmetry of the Segre variety under the Coxeter group of type AAA allows us to analyze quantum states and errors through the lens of reflection groups, viewing separable states as lying in distinct Coxeter chambers on a Segre variety. The transitive action of the permutation group on these chambers provides a natural method for tracking errors in quantum states and potentially reversing them. Beyond foundational aspects, we highlight relations between Segre varieties and Dixon elliptic curves, drawing connections between entanglement and number theory.
Quantum Entanglement is one of the key manifestations of quantum mechanics that separate the quantum realm from the classical one. Characterization of entanglement as a physical resource for quantum technology became of uppermost importance. While the entanglement of bipartite systems is already well understood, the ultimate goal to cope with the properties of entanglement of multipartite systems is still far from being realized. This paper covers characterization of multipartite entanglement using algebraic-geometric tools. First, we establish an algorithm to classify multipartite entanglement by [Formula: see text]-secant varieties of the Segre variety and [Formula: see text]-multilinear ranks that are invariant under Stochastic Local Operations with Classical Communication (SLOCC). We present a fine-structure classification of multiqubit and tripartite entanglement based on this algorithm. Another fundamental problem in quantum information theory is entanglement transformation that is quite challenging regarding to multipartite systems. It is captivating that the proposed entanglement classification by algebraic geometry can be considered as a reference to study SLOCC and asymptotic SLOCC interconversions among different resources based on tensor rank and border rank, respectively. In this regard, we also introduce a new class of tensors that we call persistent tensors and construct a lower bound for their tensor rank. We further cover SLOCC convertibility of multipartite systems considering several families of persistent tensors.