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Semicircular law with a few independent entries in a random matrix

Published 18 Aug 2026 in math.PR, math-ph, and math.ST | (2608.17648v1)

Abstract: It is well known in random matrix literature that the limiting spectral distribution of a Wigner matrix is the semi circular law while the limiting spectral distributions of other patterned matrices like Toeplitz, Hankel, symmetric circulant and reverse circulant matrices have unbounded supports. One fundamental difference between the Wigner matrices and the other matrices mentioned above is that the Wigner matrices have O(n<sup>2)O(n<sup>2) independent random variables while the others have O(n)O(n) independent random variables. In this paper, we show that this is not true in general. In particular, we form matrices with O(n)O(n) independent random variables whose empirical spectral distributions are arbitrary close to the semi circular law.

Summary

  • The paper constructs a symmetric random matrix using exactly n independent variables and proves that its empirical spectral distribution converges in probability to the standard semicircular law on [-2,2].
  • The authors use moment bounds, matched-partition estimates, and permutation-induced weak dependence to verify sufficient conditions for semicircular convergence, including conditional convergence for almost every permutation pattern.
  • The result shows that repetition geometry, rather than the number of independent entries, determines whether a patterned matrix has bounded semicircular or unbounded limiting spectral behavior.

The paper addresses a long-standing heuristic in the theory of patterned random matrices: that matrices built from only O(n)O(n) independent random variables, such as Toeplitz, Hankel, symmetric circulant, and reverse circulant ensembles, necessarily have limiting spectral distributions (LSDs) with unbounded support, in contrast to Wigner matrices whose O(n2)O(n^2) independent entries yield the semicircular law on [2,2][-2,2]. The authors show this dichotomy is not a consequence of the number of independent variables per se. They construct an explicit family of symmetric random matrices with only nn independent inputs whose empirical spectral distributions (ESDs) converge to the standard semicircular law (2608.17648).

The model

Let ξ1,,ξn\xi_1,\ldots,\xi_n be independent, centered, unit-variance random variables with uniformly bounded moments, i.e., Mr:=supiEξir<M_r := \sup_i E|\xi_i|^r < \infty for each fixed rr. Let Φ1,,Φn\Phi_1,\ldots,\Phi_n be i.i.d. uniform random permutations of [n][n], and set Yij:=ξΦi(j)Y_{ij} := \xi_{\Phi_i(j)}. The matrix of interest is the symmetrization

O(n2)O(n^2)0

Each row O(n2)O(n^2)1 draws its entries from a fresh random permutation of the same pool O(n2)O(n^2)2, so the entire ensemble depends on only O(n2)O(n^2)3 independent random variables. The permutation structure induces weak dependence: O(n2)O(n^2)4 when O(n2)O(n^2)5 and zero otherwise. After symmetrization, off-diagonal variances are O(n2)O(n^2)6 and diagonal variances are O(n2)O(n^2)7, giving O(n2)O(n^2)8, which fixes the correct scaling.

Main result

Theorem. If all moments of O(n2)O(n^2)9 are finite, then the ESD of [2,2][-2,2]0 converges weakly in probability to the standard semicircular law with density [2,2][-2,2]1 on [2,2][-2,2]2.

Equivalently, [2,2][-2,2]3 in probability under the bounded-Lipschitz metric. The corollary that carries the conceptual weight of the paper is a conditional LSD statement: for every [2,2][-2,2]4 there exist sets [2,2][-2,2]5 with [2,2][-2,2]6 such that, conditioned on any realization [2,2][-2,2]7 of the permutations, the conditional probability that the ESD deviates from the semicircle by more than [2,2][-2,2]8 is at most [2,2][-2,2]9. In other words, for almost all fixed choices of permutations — deterministic patterns of entry repetition — the resulting matrix still has a semicircular LSD. This directly answers the question posed by Arup Bose: it is not the count of independent variables but the structure of the repetitions (diagonal-parallel lines in Toeplitz matrices, cross-diagonal lines in Hankel matrices) that inflates the moments and produces unbounded support. Destroying that structure via random permutations restores Wigner-type behavior while retaining only nn0 randomness.

Proof technique

The proof reduces the problem, via Theorem 5 of Hochstättler et al., to verifying two moment conditions on distinct index sets: mixed moments of order nn1 satisfy nn2, and nn3. The key observation is that a product of the nn4's has nonzero expectation only if the multiset of indices nn5 is matched (each value appearing with multiplicity at least two). A union bound over the at most nn6 matched partitions, combined with the fact that equality events among nn7 values carry probability nn8 per constraint, yields the nn9 decay; the counting hinges on the bound ξ1,,ξn\xi_1,\ldots,\xi_n0, where ξ1,,ξn\xi_1,\ldots,\xi_n1 counts blocks containing no ξ1,,ξn\xi_1,\ldots,\xi_n2-indices. The second condition follows from Hölder's inequality together with ξ1,,ξn\xi_1,\ldots,\xi_n3, giving convergence at rate ξ1,,ξn\xi_1,\ldots,\xi_n4. The conditional corollary is then a direct Markov inequality argument.

A simulation with ξ1,,ξn\xi_1,\ldots,\xi_n5 and Gaussian ξ1,,ξn\xi_1,\ldots,\xi_n6 shows the eigenvalue histogram matching the semicircular density closely, consistent with the theorem.

Limitations and open questions

Several points are left open. The result is convergence in probability of the ESD, not almost sure convergence, and no rate of convergence in ξ1,,ξn\xi_1,\ldots,\xi_n7 is established beyond what the proof implicitly suggests. The moment method verifies the two sufficient conditions but does not provide fluctuation results, local statistics, or operator norm bounds for ξ1,,ξn\xi_1,\ldots,\xi_n8. It also remains open whether analogous constructions can reproduce other classical LSDs (e.g., Marchenko–Pastur-type behavior) using ξ1,,ξn\xi_1,\ldots,\xi_n9 independent variables, and whether the requirement of finite moments of all orders can be relaxed to a Lindeberg-type condition as in the Wigner setting. Finally, the paper does not quantify how "structured" a deterministic pattern must be before the LSD departs from the semicircle; the conditional corollary asserts typicality over permutations but gives no characterization of the exceptional set Mr:=supiEξir<M_r := \sup_i E|\xi_i|^r < \infty0.

Conclusion

This paper refutes the folk belief that Mr:=supiEξir<M_r := \sup_i E|\xi_i|^r < \infty1 independent entries force unbounded-limiting-support behavior in patterned random matrices. By randomly permuting a single pool of Mr:=supiEξir<M_r := \sup_i E|\xi_i|^r < \infty2 variables across rows, the authors obtain a symmetric ensemble with exactly Mr:=supiEξir<M_r := \sup_i E|\xi_i|^r < \infty3 independent inputs whose ESD converges in probability to the semicircular law, and which does so conditionally on almost every realization of the permutation pattern. The result cleanly isolates repetition geometry, rather than independence count, as the determinant of the LSD in patterned ensembles.

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