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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 be Hermitian positive definite, let solve , and let be Hermitian positive definite. Write , and define
Then is Hermitian positive definite, the transformed system
is equivalent to , and
Consequently, if
then exact-arithmetic CG on the transformed system obeys
which is the preconditioned CG bound.
Facts & Assumptions
Given: A Hermitian positive-definite matrix , a Hermitian positive-definite preconditioner , and the symmetric transform .
Symmetric preconditioning uses the variable change coming from a Cholesky factorization (Left preconditioning, right preconditioning, and symmetric preconditioning of a linear system).
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).
A Hermitian positive-definite matrix has a Cholesky factorization with invertible (A matrix admits a Cholesky factorisation with positive diagonal exactly when it is Hermitian positive definite, and that factor is unique).
CG obeys the Chebyshev -norm bound with the spectral condition number of its Hermitian positive-definite coefficient matrix (CG obeys the Chebyshev -norm bound in terms of the spectral condition number ).
Proof
By [L2], the preconditioner has a factorization with invertible . For any nonzero , because and is Hermitian positive definite. Also So is Hermitian positive definite.
By [F1] and [L1], the transformed system is equivalent to , and its transformed error is . Therefore Hence the energy norms agree under the symmetric change of variables.
Since step 1.1 shows that is Hermitian positive definite, [L3] applies to the transformed system and gives where 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 , not on by itself.
Depends on
- Left preconditioning, right preconditioning, and symmetric preconditioning of a linear system
- Invertible preconditioners give equivalent linear systems, with the transformed residuals and errors written explicitly
- A matrix admits a Cholesky factorisation with positive diagonal exactly when it is Hermitian positive definite, and that factor is unique
- CG obeys the Chebyshev $A$-norm bound in terms of the spectral condition number $\kappa_2(A)$
Used by
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Sources
- Jonathan Richard Shewchuk, An Introduction to the Conjugate Gradient Method Without the Agonizing Pain (standard reference, not scraped)
- Richard Barrett et al., Templates for the Solution of Linear Systems: Building Blocks for Iterative Methods (standard reference, not scraped)