Generalized minimal residual method

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In mathematics, the generalized minimal residual method (usually abbreviated GMRES) is an iterative method for the numerical solution of a nonsymmetric system of linear equations. The method approximates the solution by the vector in a Krylov subspace with minimal residual. The Arnoldi iteration is used to find this vector.

The GMRES method was developed by Yousef Saad and Martin H. Schultz in 1986.[1] GMRES is a generalization of the MINRES method developed by Chris Paige and Michael Saunders in 1975. GMRES also is a special case of the DIIS method developed by Peter Pulay in 1980. DIIS is also applicable to non-linear systems.

The method[edit]

Denote the Euclidean norm of any vector v by \|v\|. Denote the system of linear equations to be solved by

 Ax = b. \,

The matrix A is assumed to be invertible of size m-by-m. Furthermore, it is assumed that b is normalized, i.e., that \|b\| = 1.

The n-th Krylov subspace for this problem is

 K_n = K_n(A,b) = \operatorname{span} \, \{ b, Ab, A^2b, \ldots, A^{n-1}b \}. \,

GMRES approximates the exact solution of Ax = b by the vector x_n \in K_n that minimizes the Euclidean norm of the residual r_n= Ax_n-b.

The vectors b,Ab,\ldots A^{n-1}b might be almost linearly dependent, so instead of this basis, the Arnoldi iteration is used to find orthonormal vectors

 q_1, q_2, \ldots, q_n \,

which form a basis for K_n. Hence, the vector x_n \in K_n can be written as x_n = Q_n y_n with  y_n \in \mathbb{R}^n , where  Q_n is the  m -by- n matrix formed by  q_1,\ldots,q_n

The Arnoldi process also produces an (n+1)-by-n upper Hessenberg matrix \tilde{H}_n with

 AQ_n = Q_{n+1} \tilde{H}_n. \,

Because columns of Q_n are orthogonal, we have

 \| Ax_n - b \| = \| \tilde{H}_ny_n - \beta e_1 \|, \,


 e_1 = (1,0,0,\ldots,0)^T \,

is the first vector in the standard basis of \mathbb{R}^{n+1} , and

 \beta = \|b-Ax_0\| \, ,

x_0 being the first trial vector (usually zero). Hence, x_n can be found by minimizing the Euclidean norm of the residual

 r_n = \tilde{H}_n y_n - \beta e_1.

This is a linear least squares problem of size n.

This yields the GMRES method. On the n-th iteration:

  1. calculate  q_n with the Arnoldi method;
  2. find the  y_n which minimizes \|r_n\|;
  3. compute  x_n = Q_n y_n ;
  4. repeat if the residual is not yet small enough.

At every iteration, a matrix-vector product A q_n must be computed. This costs about 2m^2 floating-point operations for general dense matrices of size m, but the cost can decrease to O(m) for sparse matrices. In addition to the matrix-vector product, O(nm) floating-point operations must be computed at the n-th iteration.


The nth iterate minimizes the residual in the Krylov subspace Kn. Since every subspace is contained in the next subspace, the residual decreases monotonically. After m iterations, where m is the size of the matrix A, the Krylov space Km is the whole of Rm and hence the GMRES method arrives at the exact solution. However, the idea is that after a small number of iterations (relative to m), the vector xn is already a good approximation to the exact solution.

This does not happen in general. Indeed, a theorem of Greenbaum, Pták and Strakoš states that for every monotonically decreasing sequence a1, …, am−1, am = 0, one can find a matrix A such that the ||rn|| = an for all n, where rn is the residual defined above. In particular, it is possible to find a matrix for which the residual stays constant for m − 1 iterations, and only drops to zero at the last iteration.

In practice, though, GMRES often performs well. This can be proven in specific situations. If A is positive definite, then

 \|r_n\| \leq \left( 1-\frac{\lambda_{\mathrm{min}}^2(1/2(A^T + A))}{ \lambda_{\mathrm{max}}(A^T A)} \right)^{n/2} \|r_0\|,

where \lambda_{\mathrm{min}}(M) and \lambda_{\mathrm{max}}(M) denote the smallest and largest eigenvalue of the matrix M, respectively. [2]

If A is symmetric and positive definite, then we even have

 \|r_n\| \leq \left( \frac{\kappa_2^2(A)-1}{\kappa_2^2(A)} \right)^{n/2} \|r_0\|.

where \kappa_2(A) denotes the condition number of A in the Euclidean norm.

In the general case, where A is not positive definite, we have

 \|r_n\| \le \inf_{p \in P_n} \|p(A)\| \le \kappa_2(V) \inf_{p \in P_n} \max_{\lambda \in \sigma(A)} |p(\lambda)| \|r_0\|, \,

where Pn denotes the set of polynomials of degree at most n with p(0) = 1, V is the matrix appearing in the spectral decomposition of A, and σ(A) is the spectrum of A. Roughly speaking, this says that fast convergence occurs when the eigenvalues of A are clustered away from the origin and A is not too far from normality.[3]

All these inequalities bound only the residuals instead of the actual error, that is, the distance between the current iterate xn and the exact solution.

Extensions of the method[edit]

Like other iterative methods, GMRES is usually combined with a preconditioning method in order to speed up convergence.

The cost of the iterations grow as O(n2), where n is the iteration number. Therefore, the method is sometimes restarted after a number, say k, of iterations, with xk as initial guess. The resulting method is called GMRES(k) or Restarted GMRES. This methods suffers from stagnation in convergence as the restarted subspace is often close to the earlier subspace.

The shortcomings of GMRES and restarted GMRES are addressed by the recycling of Krylov subspace in the GCRO type methods such as GCROT and GCRODR.[4]

Comparison with other solvers[edit]

The Arnoldi iteration reduces to the Lanczos iteration for symmetric matrices. The corresponding Krylov subspace method is the minimal residual method (MinRes) of Paige and Saunders. Unlike the unsymmetric case, the MinRes method is given by a three-term recurrence relation. It can be shown that there is no Krylov subspace method for general matrices, which is given by a short recurrence relation and yet minimizes the norms of the residuals, as GMRES does.

Another class of methods builds on the unsymmetric Lanczos iteration, in particular the BiCG method. These use a three-term recurrence relation, but they do not attain the minimum residual, and hence the residual does not decrease monotonically for these methods. Convergence is not even guaranteed.

The third class is formed by methods like CGS and BiCGSTAB. These also work with a three-term recurrence relation (hence, without optimality) and they can even terminate prematurely without achieving convergence. The idea behind these methods is to choose the generating polynomials of the iteration sequence suitably.

None of these three classes is the best for all matrices; there are always examples in which one class outperforms the other. Therefore, multiple solvers are tried in practice to see which one is the best for a given problem.

Solving the least squares problem[edit]

One part of the GMRES method is to find the vector y_n which minimizes

 \| \tilde{H}_n y_n - \beta e_1 \|. \,

Note that \tilde{H}_n is an (n+1)-by-n matrix, hence it gives an over-constrained linear system of n+1 equations for n unknowns.

The minimum can be computed using a QR decomposition: find an (n+1)-by-(n+1) orthogonal matrix Ωn and an (n+1)-by-n upper triangular matrix \tilde{R}_n such that

 \Omega_n \tilde{H}_n = \tilde{R}_n.

The triangular matrix has one more row than it has columns, so its bottom row consists of zero. Hence, it can be decomposed as

 \tilde{R}_n = \begin{bmatrix} R_n \\ 0 \end{bmatrix},

where R_n is an n-by-n (thus square) triangular matrix.

The QR decomposition can be updated cheaply from one iteration to the next, because the Hessenberg matrices differ only by a row of zeros and a column:

\tilde{H}_{n+1} = \begin{bmatrix} \tilde{H}_n & h_{n+1} \\ 0 & h_{n+2,n+1} \end{bmatrix},

where hn+1 = (h1,n+1, …, hn+1,n+1)T. This implies that premultiplying the Hessenberg matrix with Ωn, augmented with zeroes and a row with multiplicative identity, yields almost a triangular matrix:

 \begin{bmatrix} \Omega_n & 0 \\ 0 & 1 \end{bmatrix} \tilde{H}_{n+1} = \begin{bmatrix} R_n & r_{n+1} \\ 0 & \rho \\ 0 & \sigma \end{bmatrix}

This would be triangular if σ is zero. To remedy this, one needs the Givens rotation

 G_n = \begin{bmatrix} I_{n} & 0 & 0 \\ 0 & c_n & s_n \\ 0 & -s_n & c_n \end{bmatrix}


 c_n = \frac{\rho}{\sqrt{\rho^2+\sigma^2}} \quad\mbox{and}\quad s_n = \frac{\sigma}{\sqrt{\rho^2+\sigma^2}}.

With this Givens rotation, we form

 \Omega_{n+1} = G_n \begin{bmatrix} \Omega_n & 0 \\ 0 & 1 \end{bmatrix}.


 \Omega_{n+1} \tilde{H}_{n+1} = \begin{bmatrix} R_n & r_{n+1} \\ 0 & r_{n+1,n+1} \\ 0 & 0 \end{bmatrix} \quad\text{with}\quad r_{n+1,n+1} = \sqrt{\rho^2+\sigma^2}

is a triangular matrix.

Given the QR decomposition, the minimization problem is easily solved by noting that

 \| \tilde{H}_n y_n - \beta e_1 \| = \| \Omega_n (\tilde{H}_n y_n - \beta e_1) \| = \| \tilde{R}_n y_n - \beta \Omega_n e_1 \|.

Denoting the vector \beta\Omega_ne_1 by

 \tilde{g}_n = \begin{bmatrix} g_n \\ \gamma_n \end{bmatrix}

with gnRn and γnR, this is

 \| \tilde{H}_n y_n - \beta e_1 \| = \| \tilde{R}_n y_n - \beta \Omega_n e_1 \| = \left\| \begin{bmatrix} R_n \\ 0 \end{bmatrix} y_n - \begin{bmatrix} g_n \\ \gamma_n \end{bmatrix} \right\|.

The vector y that minimizes this expression is given by

 y_n = R_n^{-1} g_n.

Again, the vectors g_n are easy to update.[5]

See also[edit]


  1. ^ Saad and Schultz
  2. ^ Eisenstat, Elman & Schultz, Thm 3.3. NB all results for GCR also hold for GMRES, cf. Saad & Schultz
  3. ^ Trefethen & Bau, Thm 35.2
  4. ^ Amritkar, Amit; de Sturler, Eric; Świrydowicz, Katarzyna; Tafti, Danesh; Ahuja, Kapil (2015). "Recycling Krylov subspaces for CFD applications and a new hybrid recycling solver". Journal of Computational Physics 303: 222. doi:10.1016/ 
  5. ^ Stoer and Bulirsch, §8.7.2


  • A. Meister, Numerik linearer Gleichungssysteme, 2nd edition, Vieweg 2005, ISBN 978-3-528-13135-7.
  • Y. Saad, Iterative Methods for Sparse Linear Systems, 2nd edition, Society for Industrial and Applied Mathematics, 2003. ISBN 978-0-89871-534-7.
  • Y. Saad and M.H. Schultz, "GMRES: A generalized minimal residual algorithm for solving nonsymmetric linear systems", SIAM J. Sci. Stat. Comput., 7:856-869, 1986. doi:10.1137/0907058.
  • S. C. Eisenstat, H.C. Elman and M.H. Schultz, "Variational iterative methods for nonsymmetric systems of linear equations", SIAM Journal on Numerical Analysis, 20(2), 345-357, 1983.
  • J. Stoer and R. Bulirsch, Introduction to numerical analysis, 3rd edition, Springer, New York, 2002. ISBN 978-0-387-95452-3.
  • Lloyd N. Trefethen and David Bau, III, Numerical Linear Algebra, Society for Industrial and Applied Mathematics, 1997. ISBN 978-0-89871-361-9.
  • Dongarra et al. , Templates for the Solution of Linear Systems: Building Blocks for Iterative Methods, 2nd Edition, SIAM, Philadelphia, 1994
  • Amritkar, Amit; de Sturler, Eric; Świrydowicz, Katarzyna; Tafti, Danesh; Ahuja, Kapil (2015). "Recycling Krylov subspaces for CFD applications and a new hybrid recycling solver". Journal of Computational Physics 303: 222. doi:10.1016/