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This paper resolves a long-standing open problem in quantum information theory by establishing the exact minimum cardinality of unextendible product bases (UPBs) for all multipartite systems with at least three parties. By proving a stabilization theorem that settles cases previously obstructed by parity constraints, the authors provide a complete characterization of these extremal structures using a unified graph-theoretic framework. This advancement deepens the theoretical understanding of quantum entanglement and nonlocal phenomena, which are foundational to quantum communication protocols and complexity theory.
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Minimum Cardinalities of Multipartite Unextendible Product Bases

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arXiv:2609.05657v1 Announce Type: new Abstract: In quantum information theory, the state space of a multipartite quantum system is modeled by a tensor product. In the tensor-product space $\mathbb C^{d_1}\otimes\cdots\otimes\mathbb C^{d_p}$, a nonzero vector is a \emph{product state} if it can be written as $\lvert \varphi_1\rangle\otimes\cdots\otimes\lvert \varphi_p\rangle$ with $\lvert \varphi_j\rangle\in\mathbb C^{d_j}\setminus\{0\}$. An \emph{unextendible product basis} (UPB) is a finite family of pairwise orthogonal product states such that no nonzero product state is orthogonal to all of them. UPBs play a key role in investigating quantum entanglement and nonlocal phenomena. Finding a smallest UPB is a natural extremal problem: it asks how few pairwise orthogonal product states suffice to prevent any further product state from being added. The general minimum-size problem for UPBs has been studied for over two decades since the seminal work of Alon and Lov\'asz. For local dimensions $d_1,\ldots,d_p\ge2$, let $f_m(d_1,\ldots,d_p)$ be the minimum cardinality of a UPB and let $f_{LB}(d_1,\ldots,d_p)=1+\sum_{j=1}^{p}(d_j-1)$ be the natural lower bound. Alon and Lov\'asz determined exactly when $f_m$ attains the lower bound $f_{LB}$, but the obstructed multipartite cases remained open in general. We prove a stabilization theorem: for every non-all-qubit system with $p\ge3$, whenever parity prevents the natural lower bound $f_{LB}$ from being attained, the true minimum is exactly $f_{LB}+1$. Equivalently, if the number of even local dimensions is positive and even, and at least one local dimension is greater than two, then $f_m(d_1,\ldots,d_p)=f_{LB}(d_1,\ldots,d_p)+1$. The proof is built on a unified graph-theoretic framework. Our result, together with earlier work, settles the minimum-cardinality problem for UPBs in all finite quantum systems.

Abstract:In quantum information theory, the state space of a multipartite quantum system is modeled by a tensor product. In the tensor-product space $\mathbb C^{d_1}\otimes\cdots\otimes\mathbb C^{d_p}$, a nonzero vector is a \emph{product state} if it can be written as $\lvert \varphi_1\rangle\otimes\cdots\otimes\lvert \varphi_p\rangle$ with $\lvert \varphi_j\rangle\in\mathbb C^{d_j}\setminus\{0\}$. An \emph{unextendible product basis} (UPB) is a finite family of pairwise orthogonal product states such that no nonzero product state is orthogonal to all of them. UPBs play a key role in investigating quantum entanglement and nonlocal phenomena. Finding a smallest UPB is a natural extremal problem: it asks how few pairwise orthogonal product states suffice to prevent any further product state from being added. The general minimum-size problem for UPBs has been studied for over two decades since the seminal work of Alon and Lovász. For local dimensions $d_1,\ldots,d_p\ge2$, let $f_m(d_1,\ldots,d_p)$ be the minimum cardinality of a UPB and let $f_{LB}(d_1,\ldots,d_p)=1+\sum_{j=1}^{p}(d_j-1)$ be the natural lower bound. Alon and Lovász determined exactly when $f_m$ attains the lower bound $f_{LB}$, but the obstructed multipartite cases remained open in general. We prove a stabilization theorem: for every non-all-qubit system with $p\ge3$, whenever parity prevents the natural lower bound $f_{LB}$ from being attained, the true minimum is exactly $f_{LB}+1$. Equivalently, if the number of even local dimensions is positive and even, and at least one local dimension is greater than two, then $f_m(d_1,\ldots,d_p)=f_{LB}(d_1,\ldots,d_p)+1$. The proof is built on a unified graph-theoretic framework. Our result, together with earlier work, settles the minimum-cardinality problem for UPBs in all finite quantum systems.

Quantum Physics (quant-ph); Combinatorics (math.CO)

arXiv:2609.05657 [quant-ph]

(or arXiv:2609.05657v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2609.05657 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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