Abstract

We study the statistics of the condition number κ=λmax/λminκ=λ_{\mathrm{max}}/λ_{\mathrm{min}} (the ratio between largest and smallest squared singular values) of N×MN\times M Gaussian random matrices. Using a Coulomb fluid technique, we derive analytically and for large NN the cumulative P[κ<x]\mathcal{P}[κ<x] and tail-cumulative P[κ>x]\mathcal{P}[κ>x] distributions of κκ. We find that these distributions decay as P[κ<x]≈exp⁡(−βN2Φ−(x))\mathcal{P}[κ<x]\approx\exp\left(-βN^2 Φ_{-}(x)\right) and P[κ>x]≈exp⁡(−βNΦ+(x))\mathcal{P}[κ>x]\approx\exp\left(-βN Φ_{+}(x)\right), where ββ is the Dyson index of the ensemble. The left and right rate functions Φ±(x)Φ_{\pm}(x) are independent of ββ and calculated exactly for any choice of the rectangularity parameter α=M/N−1>0α=M/N-1>0. Interestingly, they show a weak non-analytic behavior at their minimum ⟨κ⟩\langleκ\rangle (corresponding to the average condition number), a direct consequence of a phase transition in the associated Coulomb fluid problem. Matching the behavior of the rate functions around ⟨κ⟩\langleκ\rangle, we determine exactly the scale of typical fluctuations ∼O(N−2/3)\sim\mathcal{O}(N^{-2/3}) and the tails of the limiting distribution of κκ. The analytical results are in excellent agreement with numerical simulations.

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