numerical computation with random data

The research direction is to determine how broadly universality of computation times extends across numerical algorithms on random data. For input size nn, let XnX_n have input law En\mathcal E_n, let AA be an algorithm, and let Tϵ,n,A,En(Xn)T_{\epsilon,n,A,\mathcal E_n}(X_n) denote the elapsed time or iteration count until its prescribed halting criterion is met at tolerance ϵ\epsilon. Given a sample of such inputs, write ⟨T⟩\langle T\rangle and σT\sigma_T for the sample mean and sample standard deviation, and standardize the observed times by

τϵ,n,A,En(Xn)=Tϵ,n,A,En(Xn)−⟨Tϵ,n,A,En⟩σϵ,n,A,En.\tau_{\epsilon,n,A,\mathcal E_n}(X_n)=\frac{T_{\epsilon,n,A,\mathcal E_n}(X_n)-\langle T_{\epsilon,n,A,\mathcal E_n}\rangle}{\sigma_{\epsilon,n,A,\mathcal E_n}}.

The question is whether, for a fixed algorithm and suitable size and tolerance regimes, the distributions of these normalized times become independent of the input law, and how widely this behavior occurs across computations. This is a research direction rather than a single limit theorem: the reported limiting or empirical laws may depend on the algorithm. Universality in Numerical Computations with Random Data. Case Studies

Background

The motivation combines two uses of random models: Wigner’s random-matrix work in the 1950s and the use of random ensembles in scientific computing, also traced to work of von Neumann and Goldstine in that decade. In eigenvalue computation, algorithms such as QR evolve a matrix through isospectral transformations: the eigenvalues remain fixed while the matrix approaches a form from which they can be read off. Thus computation on random matrices can be viewed as deterministic evolution of random input data. The Toda lattice, introduced by M. Toda in 1967, provides a particularly direct link between integrable dynamics and eigenvalue computation. Universality in Numerical Computations with Random Data. Case Studies Universality for the Toda algorithm to compute the largest eigenvalue of a random matrix

Known results

The case studies report empirical two-component universality: after centering halting times by their sample mean and scaling by their sample standard deviation, histograms from different input ensembles were observed to collapse as dimension increased. The scope includes QR on Hermitian ensembles and Jacobi on real symmetric matrices with independent entries; these are distinct settings, not a claim that Jacobi was tested on the Hermitian ensembles. Other reported examples include conjugate gradient and GMRES for random linear systems, as well as a genetic algorithm and computations involving random PDEs. These observations are evidence from computations, not general convergence theorems, and the observed law can differ between algorithms. Universality in Numerical Computations with Random Data. Case Studies

For the Toda algorithm, a theorem gives a more specific limiting law. Along the isospectral flow, let X(t)X(t) start at an N×NN\times N real symmetric or complex Hermitian random matrix HH, and set

E(t)=∑j=2N∣X1j(t)∣2,T(1)(H)=inf⁡{t:E(t)≤ϵ2}.E(t)=\sum_{j=2}^{N}|X_{1j}(t)|^2,\qquad T^{(1)}(H)=\inf\{t:E(t)\leq\epsilon^2\}.

This is the first-row deflation time, not the time to deflate the entire matrix. Let λN≥λN−1\lambda_N\geq\lambda_{N-1} be the two largest eigenvalues. For the real (β=1\beta=1) and complex (β=2\beta=2) invariant or Wigner ensembles in the theorem, the top-gap distribution is

Fβgap(t)=lim⁡N→∞P ⁣(1cV2/32−2/3N2/3(λN−λN−1)≤t),t≥0,F^{\mathrm{gap}}_{\beta}(t)=\lim_{N\to\infty}\mathbb P\!\left(\frac{1}{c_V^{2/3}2^{-2/3}N^{2/3}(\lambda_N-\lambda_{N-1})}\leq t\right),\qquad t\geq0,

where cVc_V depends on the ensemble. For fixed 0<σ<10<\sigma<1, if the size and tolerance satisfy log⁡(ϵ−1)/log⁡N≥5/3+σ/2\log(\epsilon^{-1})/\log N\geq 5/3+\sigma/2, the theorem identifies the rescaled deflation-time law with this gap law:

lim⁡N→∞P ⁣(T(1)cV2/32−2/3N2/3(log⁡ϵ−1−23log⁡N)≤t)=Fβgap(t).\lim_{N\to\infty}\mathbb P\!\left(\frac{T^{(1)}}{c_V^{2/3}2^{-2/3}N^{2/3}(\log\epsilon^{-1}-\tfrac23\log N)}\leq t\right)=F^{\mathrm{gap}}_{\beta}(t).

In this regime, the mechanism is that the first deflation time is controlled asymptotically by the spacing of the two largest eigenvalues; it is a rigorous result for this particular algorithm and stopping rule, not a theorem establishing universality for numerical computation in general. Universality for the Toda algorithm to compute the largest eigenvalue of a random matrix

References

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