Explicit Expansion and Bounds of Spectral Projector in ESPRIT Analysis

Written by algorithmicbias | Published 2025/05/16
Tech Story Tags: esprit-analysis | perturbation-theory | spectral-projector | signal-processing | schur-polynomial | error-bounds | mathematical-proofs | schur-polynomials

TLDRThis section details the explicit formulas for higher-order terms in the perturbation expansion of the spectral projector, along with their boundsvia the TL;DR App

Table of Links

Abstract and 1 Introduction

1.1 ESPRIT algorithm and central limit error scaling

1.2 Contribution

1.3 Related work

1.4 Technical overview and 1.5 Organization

2 Proof of the central limit error scaling

3 Proof of the optimal error scaling

4 Second-order eigenvector perturbation theory

5 Strong eigenvector comparison

5.1 Construction of the “good” P

5.2 Taylor expansion with respect to the error terms

5.3 Error cancellation in the Taylor expansion

5.4 Proof of Theorem 5.1

A Preliminaries

B Vandermonde matrice

C Deferred proofs for Section 2

D Deferred proofs for Section 4

E Deferred proofs for Section 5

F Lower bound for spectral estimation

References

D Deferred proofs for Section 4

This section provides supplementary proofs for Section 4. In Appendix D.1, we develop explicit formulas for the higher-order terms in the perturbation expansion result, Proposition 4.2. In Appendix D.2, we show how to bound the terms appearing in this expression. We conclude by proving Lemma 4.3 in Appendix D.3.

D.1 Expansion of spectral projector: explicit formulas

After deriving the explicit expansion, we need to employ the following two properties of the Schur polynomial [Mac15] to constrain the higher-order terms in Appendix D.2:

We also need to use the standard cofactor expansion for the determinant calculation.

Fact D.3 (Cofactor expansion of determinant). For any n-by-n matrix A, the cofactor expansion of the determinant along the first row is

where the second step follows from

We recognize the numerator of this expression of a cofactor expansion of a determinant (Fact D.3), obtaining

where the second step follows from the definition of the Schur polynomial (Definition D.1). Substituting this expression back in Eq. (D.4) yields the stated result.

Theorem D.7 (Expansion of spectral projector, explicit form). It holds that

Thus, we obtain that

The theorem then follows by Proposition 4.2.

D.2 Expansion of spectral projector: bounds on terms

In this section, we bound the terms appearing in the expansion of the spectral projector, Theorem D.7. Our result is as follows:

Proof. For ease of reading, we break the proof into steps.

Proof of (b). Using Eq. (D.12) and Eq. (D.9) to bound every term in Eq. (D.8), we conclude that

where the second step follows from Corollary B.3, Lemma C.1, and Eq. (D.11).

For the second term, we have

D.3 Proof of Lemma 4.3

Lemma 4.3 (Expansion of spectral projector, simplified). It holds that

Proof. Begin with the explicit expansion of the spectral projector (Theorem D.7)

where the last step follows from C ∈ (0, 3/8).

The lemma is then proved.

This paper is available on arxiv under CC BY 4.0 DEED license.

Authors:

(1) Zhiyan Ding, Department of Mathematics, University of California, Berkeley;

(2) Ethan N. Epperly, Department of Computing and Mathematical Sciences, California Institute of Technology, Pasadena, CA, USA;

(3) Lin Lin, Department of Mathematics, University of California, Berkeley, Applied Mathematics and Computational Research Division, Lawrence Berkeley National Laboratory, and Challenge Institute for Quantum Computation, University of California, Berkeley;

(4) Ruizhe Zhang, Simons Institute for the Theory of Computing.


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Published by HackerNoon on 2025/05/16