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With a Hermitian matrix, Arnoldi collapses to the Lanczos three-term recurrence and a real symmetric tridiagonal projection

Statement

Let A be Hermitian, and run Arnoldi on (A,b) through step m without breakdown. Write

AQm=Qm+1Hˉm,Qm=[q1qm].

Then there exist real numbers α1,,αm and nonnegative real numbers β1,,βm such that

Aqj=βj1qj1+αjqj+βjqj+1(1jm, q0:=0, β0:=0).

Moreover, Tm:=QmAQm is a real symmetric tridiagonal matrix.

Facts & Assumptions

Given: A Hermitian matrix A and an Arnoldi run through step m without breakdown.

[F1]

The Lanczos process is Arnoldi specialized to a Hermitian matrix, with the phase chosen so that the subdiagonal coefficients are real and nonnegative (The Lanczos process as Arnoldi specialized to a Hermitian matrix, with the usual real-subdiagonal phase convention).

[L1]

Arnoldi yields an orthonormal basis and an upper-Hessenberg factorization AQm=Qm+1Hˉm, with column relations Aqj=i=1j+1hijqi (Before breakdown, Arnoldi produces an orthonormal Krylov basis and a rectangular upper-Hessenberg factorization).

[L2]

An upper-Hessenberg matrix has hij=0 for i>j+1, and a real symmetric tridiagonal matrix has zeros whenever ij>1 (Upper Hessenberg matrices and real symmetric tridiagonal matrices).

Proof

technique · direct
1.1

Fix j and let ij2. By [L1], Aqi lies in span{q1,,qi+1}, which is orthogonal to qj. Since A is Hermitian, hij=qiAqj=(Aqi)qj=0. Together with the upper-Hessenberg zero pattern from [L2], this shows that the only possibly nonzero coefficients in column j are hj1,j, hjj, and hj+1,j. Therefore each Arnoldi column relation collapses to a three-term recurrence.

L1L2algebra
2.1

Hermitian symmetry also gives hj,j1=hj1,j. Under the phase convention in [F1], the subdiagonal coefficients hj+1,j are real and nonnegative; write βj:=hj+1,j and αj:=hjj. Since hjj=qjAqj equals its own complex conjugate, each αj is real. Hence Aqj=βj1qj1+αjqj+βjqj+1, which is the Lanczos recurrence.

F1step 1.1algebra
3.1

The projected matrix is Tm=QmAQm=(qiAqj)i,j=(hij)1i,jm. Step 1.1 shows hij=0 for ij>1, and Hermitian symmetry together with the reality from step 2.1 shows hij=hjiR on the remaining bands. Thus Tm is a real symmetric tridiagonal matrix in the sense of [L2].

L2step 1.1step 2.1

Depends on

Used by

Cited to discharge well-definedness by The Lanczos process as Arnoldi specialized to a Hermitian matrix, with the usual real-subdiagonal phase convention.

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