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Orthogonal polynomials in the spherical ensemble with two insertions

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arxiv 2503.15732 v2 pith:E55MEACR submitted 2025-03-19 math.CA math-phmath.MP

classification math.CAmath-phmath.MP
keywords asymptoticspolynomialsmeasureorthogonalorthogonalityplanarproblemrelies
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abstract

We consider asymptotics of planar orthogonal polynomials $P_{n,N}$ (where $\mathrm{deg}P_{n,N}=n$) with respect to the weight $$\frac{|z-w|^{2NQ_1}}{(1+|z|^2)^{N(1+Q_0+Q_1)+1}}, \quad(Q_0,Q_1 > 0)$$ in the whole complex plane. With $n, N\rightarrow\infty$ and $N-n$ fixed, we obtain the strong asymptotics of the polynomials, asymptotics for the weighted $L^2$ norm and the limiting zero counting measure. These results apply to the pre-critical phase of the underlying two-dimensional Coulomb gas system, when the support of the equilibrium measure is simply connected. Our method relies on specifying the mother body of the two-dimensional potential problem. It relies too on the fact that the planar orthogonality can be rewritten as a non-Hermitian contour orthogonality. This allows us to perform the Deift-Zhou steepest descent analysis of the associated $2\times 2$ Riemann-Hilbert problem.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Asymptotics of the real eigenvalue distribution for the real spherical ensemble

    math-ph 2025-08 conditional novelty 6.0 of 10

    For the real spherical ensemble, asymptotic formulas are derived for the probability of M real eigenvalues when M ~ N, M ~ sqrt(N), and M near the mean, with cross-regime matching and the leading p_{N,0} ~ e^{-sqrt(pi...

  2. Partition function of 2D Coulomb gases with radially symmetric potentials and a hard wall

    math.PR 2025-06 conditional novelty 6.0 of 10

    For radially symmetric potentials at beta = 2, the log N coefficient in the hard-wall partition function is -1/4 for an annulus and -1/3 for a disk when the wall lies strictly inside the droplet, instead of the usual -1/12.

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