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Weak Typicality of von Neumann Entanglement Entropy in Gaussian Boson Sampling

Published 18 Aug 2026 in quant-ph | (2608.17274v1)

Abstract: We study the von Neumann entanglement entropy generated by a Haar distributed passive interferometer acting on nn equally squeezed input modes with fixed nonzero squeezing strength ss. Previous work established proportional weak typicality for integer R'enyi orders α2α\geq 2 and stated a sublinear von Neumann result, while the proportional von Neumann case remained open. For a subsystem of knk_n modes satisfying kn/nr(0,1)k_n/n\to r\in(0,1), we prove that, for every $\varepsilon&gt;0$ and all sufficiently large nn, P(S1,nES1,n1ε)2exp[cs,rε<sup>2n<sup>2log<sup>2(en)].\mathbb{P}\left(\left|\frac{S_{1,n}}{\mathbb{E}S_{1,n}}-1\right|\geq\varepsilon\right)\leq2\exp\left[-\frac{c_{s,r}\varepsilon<sup>2n<sup>2}{\log<sup>2(en)}\right]. The proof represents the entropy as a singular value statistic of a principal block of UU<sup></sup>TUU<sup>{\mathsf</sup> T}, where UU denotes the unitary interferometer. It regularizes the logarithmic singularity at the endpoint corresponding to a pure Gaussian mode and applies concentration on the unitary group. The result establishes proportional von Neumann weak typicality and further implies almost sure convergence of S1,n/ES1,nS_{1,n}/\mathbb{E}S_{1,n} to $1$, a typical volume law, and the variance bound Var(S1,n)=Os(log<sup>2</sup>n)\mathrm{Var}(S_{1,n})=O_s(\log<sup>2</sup> n). An accompanying Lean 4 development verifies the proof chain.

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Summary

  • The paper proves proportional weak typicality for von Neumann entanglement entropy, with relative deviations bounded by 2 exp[-c ε²n²/log²(en)] for Haar-random interferometers and proportional subsystems.
  • The proof combines an exact singular-value representation, endpoint regularization, an extensive mean lower bound, and Haar concentration to establish a typical volume law, Page-curve convergence, and Var(S₁,ₙ) = Oₛ(log²(en)).
  • The paper shows strong typicality fails for every proportional cut except that the balanced case remains unresolved, while unequal squeezing, optical loss, and nonintegrable endpoint singularities remain important open challenges.

Setting and problem

Gaussian boson sampling (GBS) prepares squeezed vacuum inputs, mixes them through a passive linear optical interferometer, and measures photon counts. Before measurement, the output is a pure bosonic Gaussian state whose entanglement across a bipartition of the modes is the von Neumann entropy S1,nS_{1,n} of either reduced state. The paper studies this entropy for a Haar distributed interferometer UU(n)U \in U(n) acting on nn equally squeezed inputs with fixed nonzero squeezing strength ss, and a subsystem of knk_n modes with kn/nr(0,1)k_n/n \to r \in (0,1).

Prior work left a specific gap. Iosue et al. proved proportional weak typicality for Rényi order 2 and stated von Neumann weak typicality only for sublinear subsystems; Youm et al. extended proportional weak typicality to every integer Rényi order α2\alpha \ge 2 and derived the asymptotically exact mean Page curve, but explicitly left proportional von Neumann typicality open. The obstruction is analytic: the one-mode entropy profile has a derivative that diverges logarithmically as a reduced symplectic eigenvalue approaches its pure value ν=1\nu = 1. The paper closes this gap with a quantitative relative tail bound and an accompanying Lean 4 formalization.

Main result

The central theorem establishes weak typicality in the proportional regime. For fixed s0s \neq 0 and any sequence kn/nr(0,1)k_n/n \to r \in (0,1), there exists UU(n)U \in U(n)0 such that for all sufficiently large UU(n)U \in U(n)1,

UU(n)U \in U(n)2

The right-hand side is summable in UU(n)U \in U(n)3, so by Borel–Cantelli the convergence holds almost surely for every coupling whose size-UU(n)U \in U(n)4 marginal is Haar on UU(n)U \in U(n)5; no independence across dimensions is required. Three corollaries follow directly:

  • Typical volume law: for any UU(n)U \in U(n)6, the probability that UU(n)U \in U(n)7 tends to one, so UU(n)U \in U(n)8. Purity sharpens the deterministic upper bound to UU(n)U \in U(n)9.
  • Typical Page curve value: combined with the published mean limit nn0 of Youm et al., the entropy density converges in probability (and almost surely) to the Page curve density at each fixed ratio nn1. This is pointwise in nn2; it does not assert simultaneous concentration over all ratios or mode subsets.
  • Variance bound: nn3, with deviations below every polynomial scale almost surely, i.e. nn4.

A notable negative companion result: strong typicality (nn5 in probability) fails at every proportional ratio nn6, proved via the Jacobi linear statistics CLT applied to the squared singular values, which form a real nn7-Jacobi ensemble with nondegenerate limiting Gaussian fluctuations.

Proof structure

The argument proceeds in four steps.

Exact spectral reduction. For equal squeezing, the reduced covariance matrix is nn8, where nn9, ss0, and ss1 is built from the leading ss2 principal block ss3 of ss4, which is complex symmetric and COE distributed. Anticommutation with the symplectic form yields the exact finite-ss5 identity

ss6

where ss7 are the singular values of ss8 and ss9 is the one-mode entropy function. This reduces the entropy to a singular value statistic of a principal COE block.

Endpoint regularization. The function knk_n0 is continuous but its derivative diverges logarithmically at knk_n1: knk_n2. Truncating within knk_n3 of the endpoint defines knk_n4 with Lipschitz constant knk_n5 while the uniform approximation error satisfies knk_n6. The cost–benefit ratio is favorable because the cutoff error scales as knk_n7 while the Lipschitz penalty grows only as knk_n8; choosing knk_n9 makes the former vanish without degrading concentration. A direct variance calculation is thereby avoided entirely.

Extensive mean lower bound. Concentration must be compared against the mean scale. Using kn/nr(0,1)k_n/n \to r \in (0,1)0, a chord bound on the logarithm, and an elementary self-contained derivation of the COE second moment kn/nr(0,1)k_n/n \to r \in (0,1)1 — obtained by congruence symmetries rather than Weingarten calculus — the paper proves

kn/nr(0,1)k_n/n \to r \in (0,1)2

which is kn/nr(0,1)k_n/n \to r \in (0,1)3 in the proportional regime.

Haar concentration. Applying the Meckes–Meckes log-Sobolev concentration inequality on kn/nr(0,1)k_n/n \to r \in (0,1)4 to the Lipschitz statistic kn/nr(0,1)k_n/n \to r \in (0,1)5, and transferring back through the uniform approximation, yields the main tail. The variance bound follows by integrating the same tail.

Formal verification

A Lean 4 development (pinned toolchain and Mathlib commit, archived on Zenodo) kernel-checks the core proof chain. Its scope is explicitly bounded: full unitary Haar concentration, Mirsky's singular value inequality, and the Gaussian covariance/normal-form results are represented as explicit theorem assumptions rather than re-proved; the published hypergeometric Page curve computation is likewise assumed for the transfer corollary. The formalization transcribes but does not construct Fock space, trace-class operators, or partial traces, identifying them with the abstract spectral model only through the stated Gaussian interface. The strong-typicality failure result lies outside the formalization scope.

Limitations and open questions

The paper states its boundaries plainly. Strong typicality at the balanced cut kn/nr(0,1)k_n/n \to r \in (0,1)6 remains undetermined: there the limiting Jacobi support reaches the logarithmically singular endpoint, so the kn/nr(0,1)k_n/n \to r \in (0,1)7 CLT used elsewhere does not apply, though weak typicality still holds. Equal squeezing is essential to the reduction to a single principal COE block; with unequal squeezing profiles the reduction is lost, and extending weak typicality to that experimentally relevant case is identified as the natural next problem. The result concerns the ideal lossless premeasurement state — with loss the global state is mixed and kn/nr(0,1)k_n/n \to r \in (0,1)8 no longer isolates entanglement — and it makes no claim about sampling hardness or anticoncentration of output probabilities. The method's reliance on integrable endpoint singularities also means it would not transfer unchanged to observables with power-law singularities, where cutoff error and Lipschitz cost compete at the extensive scale.

Conclusion

The paper proves proportional weak typicality of the von Neumann entanglement entropy for Haar random passive interferometers acting on equally squeezed vacuum inputs, closing the cell left open in prior work. The proof combines an exact singular-value representation, a vanishing logarithmic endpoint cutoff, a self-contained extensive mean lower bound, and Haar concentration, yielding a summable relative tail, a typical volume law, logarithmic tightness, and kn/nr(0,1)k_n/n \to r \in (0,1)9. Together with the known mean Page curve, it promotes the average Page curve value at each fixed proportional bipartition to a statement about typical samples, while proving that additive (strong) typicality fails away from the balanced cut.

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