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TheoremStatement: AI-adaptedProof: AI-generatedprecheck passjudge pass (gpt-5.6-terra)audited 2026-09-01
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Symmetric positive-definite preconditioning preserves a Hermitian positive-definite CG problem, and the CG bound uses the transformed condition number

Statement

Let AMn(C) be Hermitian positive definite, let x solve Ax=b, and let M be Hermitian positive definite. Write M=CC, and define

A~:=C1AC,b~:=C1b,y:=Cx,y:=Cx.

Then A~ is Hermitian positive definite, the transformed system

A~y=b~

is equivalent to Ax=b, and

yyA~=xxA.

Consequently, if

κ:=λmax(A~)λmin(A~),

then exact-arithmetic CG on the transformed system obeys

yymA~2(κ1κ+1)myy0A~,

which is the preconditioned CG bound.

Facts & Assumptions

Given: A Hermitian positive-definite matrix A, a Hermitian positive-definite preconditioner M, and the symmetric transform A~=C1AC.

[F1]

Symmetric preconditioning uses the variable change y=Cx coming from a Cholesky factorization M=CC (Left preconditioning, right preconditioning, and symmetric preconditioning of a linear system).

[L1]

Equivalent preconditioned systems have the transformed residual and error maps recorded explicitly (Invertible preconditioners give equivalent linear systems, with the transformed residuals and errors written explicitly).

[L2]

A Hermitian positive-definite matrix has a Cholesky factorization M=CC with invertible C (A matrix admits a Cholesky factorisation with positive diagonal exactly when it is Hermitian positive definite, and that factor is unique).

[L3]

CG obeys the Chebyshev A-norm bound with the spectral condition number of its Hermitian positive-definite coefficient matrix (CG obeys the Chebyshev A-norm bound in terms of the spectral condition number κ2(A)).

Proof

technique · direct
1.1

By [L2], the preconditioner has a factorization M=CC with invertible C. For any nonzero z, zA~z=(Cz)A(Cz)>0, because Cz0 and A is Hermitian positive definite. Also A~=(C1AC)=C1AC=C1AC=A~. So A~ is Hermitian positive definite.

L2algebra
2.1

By [F1] and [L1], the transformed system A~y=b~ is equivalent to Ax=b, and its transformed error is esym=yy=C(xx). Therefore yyA~2=(yy)A~(yy)=(xx)A(xx)=xxA2. Hence the energy norms agree under the symmetric change of variables.

F1L1step 1.1algebra
3.1

Since step 1.1 shows that A~ is Hermitian positive definite, [L3] applies to the transformed system and gives yymA~2(κ1κ+1)myy0A~, where κ=λmax(A~)/λmin(A~) is the spectral ratio from the Statement. By step 2.1, this is exactly the preconditioned CG estimate expressed in the original variables. The bound depends on the transformed operator A~, not on κ2(A) by itself.

L3step 1.1step 2.1

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