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PreprintCC BY 4.0arXiv

Quenched Growth of Normal Matrices and Harmonic Measure

Abstract

The eigenvalues of a large normal random matrix form a two-dimensional Coulomb gas. At fixed weight, the spectral droplet grows with the matrix rank, and its semiclassical density increment is harmonic measure. We freeze an N-eigenvalue configuration and sample M further eigenvalues using the projection onto polynomials of degree less than N+M that vanish at the frozen points. Their conditional law is an exact polynomial ensemble in the potential of the frozen charges. For a regular analytic droplet, we prove that the spatial distribution of the new eigenvalues converges to harmonic measure on the old boundary when M/log N→∞ and M/N→0. This convergence holds conditionally on the frozen spectrum, outside a set of frozen configurations whose probability tends to zero. The equilibrium process formed from orthogonal polynomials of degrees N,…,N+M−1 has the same limit. An exact finite-rank identity relates polynomial moments of the conditional mean to fluctuations of the frozen spectrum, with a remainder from polynomial modes of degree N+M and above.

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BibTeX
@misc{alekseev2026quenched,
  title = {{Quenched Growth of Normal Matrices and Harmonic Measure}},
  author = {Oleg Alekseev},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.03912},
  eprint = {2610.03912},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.03912},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Quenched Growth of Normal Matrices and Harmonic Measure
AU  - Oleg Alekseev
PY  - 2026
DA  - 2026/10/02
PB  - arXiv
DO  - 10.48550/arxiv.2610.03912
UR  - https://arxiv.org/abs/2610.03912
AB  - The eigenvalues of a large normal random matrix form a two-dimensional Coulomb gas. At fixed weight, the spectral droplet grows with the matrix rank, and its semiclassical density increment is harmonic measure. We freeze an N-eigenvalue configuration and sample M further eigenvalues using the projection onto polynomials of degree less than N+M that vanish at the frozen points. Their conditional law is an exact polynomial ensemble in the potential of the frozen charges. For a regular analytic droplet, we prove that the spatial distribution of the new eigenvalues converges to harmonic measure on the old boundary when M/log N→∞ and M/N→0. This convergence holds conditionally on the frozen spectrum, outside a set of frozen configurations whose probability tends to zero. The equilibrium process formed from orthogonal polynomials of degrees N,…,N+M−1 has the same limit. An exact finite-rank identity relates polynomial moments of the conditional mean to fluctuations of the frozen spectrum, with a remainder from polynomial modes of degree N+M and above.
ER  -