************************************************************************** SSMFE_EXPERT - Sparse Symmetric Matrix-Free Eigensolver (Expert interface) ************************************************************************** .. code-block:: C #include /* or for all packages */ ======= Purpose ======= This package computes extreme (leftmost and/or rightmost) eigenpairs :math:`\{\lambda_i, x_i\}` of the following eigenvalue problems: - the standard eigenvalue problem .. math:: A x = \lambda x, - the generalized eigenvalue problem .. math:: A x = \lambda B x, - the buckling problem .. math:: B x = \lambda A x, where :math:`A` and :math:`B` are **real symmetric** (or **Hermitian**) matrices and :math:`B` is **positive definite**. The package :doc:`SSMFE ` provides a more user-friendly wrapper around this code. Conversely, :doc:`SSMFE_CORE ` provides a lower level implementation of the core solver, which this package provides a wrapper for. Major version history --------------------- 2014-11-20 Version 1.0.0 Initial release [for detail please see ChangeLog] ============== Usage overview ============== The eigensolver subroutines behind this package implement a block iterative algorithm. The block nature of this algorithm allows the user to benefit from highly optimized linear algebra subroutines and from the ubiquitous multicore architecture of modern computers. It also makes this algorithm more reliable than Krylov-based algorithms employed e.g. by ARPACK in the presence of clustered eigenvalues. However, convergence of the iterations may be slow if the density of the spectrum is high. Thus, good performance (in terms of speed) is contingent on the following two factors: i. the number of desired eigenpairs must be substantial (e.g. not fewer than the number of CPU cores), and ii. the employment of a convergence acceleration technique. The acceleration techniques that can be used are shift-and-invert and preconditioning. The former requires the direct solution of linear systems with the matrix :math:`A` or its linear combination with :math:`B`, for which a sparse symmetric indefinite solver (such as HSL_MA97 or SPRAL_SSIDS) can be employed. The latter applies to the case of positive definite :math:`A` and requires a matrix or an operator :math:`T`, called *a preconditioner*, such that the vector :math:`v = T f` is an approximation to the solution :math:`u` of the system :math:`A u = f` (see the simple :ref:`example below `). Note: This technique is only recommended for experienced users. In this expert interface, the user must handle storage of all vectors, facilitating advanced memory handling techniques required for parallel, hybrid and/or out-of-core execution. If there is no requirement to store these vectors, consider using the simplified interface of :doc:`SSMFE ` instead. =========== Subroutines =========== To use the solver procedures, the user must maintain a workspace of `(kw+1)` blocks each containing `m` vectors of size `n`. For notational convienience we refer to this workspace as a C array ``W[kw+1][m][n]``, but the user is free to store it as they wish. The following table provides minimum values of `kw` for each setup: +-------------------+------------+------------+------------+------------+ | | minAprod=T | minAprod=F | +-------------------+------------+------------+------------+------------+ | Problem | minBprod=T | minBprod=F | minBprod=T | minBprod=F | +===================+============+============+============+============+ | standard | 7 | 5 | 3 | 3 | +-------------------+------------+------------+------------+------------+ | standard_shift | 7 | 5 | N/A | N/A | +-------------------+------------+------------+------------+------------+ | generalized | 7 | 5 | 5 | 3 | +-------------------+------------+------------+------------+------------+ | generalized_shift | 7 | 7 | N/A | N/A | +-------------------+------------+------------+------------+------------+ | buckling | 7 | 7 | N/A | N/A | +-------------------+------------+------------+------------+------------+ Further, the user must also store the converged eigenvectors :math:`X`, and (for generalised problems) their :math:`B`-images :math:`BX` using separate storage, e.g. ``X[mep][n], BX[mep][n]``. For convienence of notation we use the convention that ``x[i:j]`` denotes indices `i` through `j` (inclusive) of the vector `x[]`. In addition to being output, the routine may need to reorthagonalise against these from time to time. .. c:function:: void spral_ssmfe_default_options(struct spral_ssmfe_options *options) Intialises members of options structure to default values. :param options: Structure to be initialised. .. c:function:: void spral_ssmfe_expert_standard_double(struct spral_ssmfe_rcid *rci, int left, int mep, double *lambda, int m, double *rr, int *ind, void **keep, const struct spral_ssmfe_options *options, struct spral_ssmfe_inform *inform) Computes the left-most eigenpairs of the standard eigenvalue problem .. math:: Ax = \lambda x Optionally uses preconditioning. Uses reverse-communication. Upon return the user must perform a task specified by the `rci` parameter and recall the routine. Possible values of `rci` and associated tasks are: +----------+---------------------------------------------------------------+ | `rci.job`| Task to be performed | +==========+===============================================================+ | -3 | None. Fatal error, see :c:member:`inform.flag | | | `. | +----------+---------------------------------------------------------------+ | -2 | Failed to converge, see | | | :c:member:`inform.flag `. | +----------+---------------------------------------------------------------+ | -1 | None. Computation complete. | +----------+---------------------------------------------------------------+ |  1 | Calculate :math:`\bar{V} = AU`. | +----------+---------------------------------------------------------------+ | 2 | Apply preconditioner :math:`\bar{V} = TU`. (Copy if T=I). | +----------+---------------------------------------------------------------+ | 5 | Copy converged eigenvectors :math:`X` to user storage: | | | | | | * If `rci.i>0`: ``W[rci.kx][rci.jx:rci.jx+rci.nx-1][:]``. | | | * Else: ``W[rci.kx][rci.jx-rci.nx+1:rci.jx][:]``. | +----------+---------------------------------------------------------------+ | 11 | If `rci.i.eq.0`, copy :math:`\bar{V} = U`. | | | | | | Otherwise, reorder columns of block `rci.kx` such that column | | | `ind[j]` becomes the new column `j` for `j=1, ..., rci.nx` | | | | | | Note: if ``rci.kx==rci.ky``, only reorder once. | +----------+---------------------------------------------------------------+ | 12 | Compute the dot products | | | | | | .. math:: r_{ii} = U_i \cdot \bar{V}_i | +----------+---------------------------------------------------------------+ | 13 | Perform the scalings | | | | | | .. math:: U_i = U_i/\sqrt{(U_i\cdot \bar{V}_i)} | | | | | | and | | | | | | .. math:: \bar{V}_i = \bar{V}_i/\sqrt{(U_i\cdot \bar{V}_i)} | | | | | | for each column :math:`U_i` and :math:`\bar{V}_i` of :math:`U`| | | and :math:`\bar{V}`. | | | | | | Note: if ``rci.kx == rci.ky``, only scale once. | +----------+---------------------------------------------------------------+ | 14 | Perform the updates | | | | | | .. math:: \bar{V}_i = \bar{V}_i + r_{ii} U_i | | | | | | for each column :math:`\bar{V}_i` of :math:`\bar{V}` | +----------+---------------------------------------------------------------+ | 15 | Perform the update | | | | | | .. math:: R = \alpha U^T V + \beta R | +----------+---------------------------------------------------------------+ | 16 | Perform the update | | | | | | .. math:: V = \alpha U R + \beta V | +----------+---------------------------------------------------------------+ | 17 | Perform the update | | | | | | .. math:: U = \alpha U R | | | | | | Note: :math:`V` may be used as a workspace | +----------+---------------------------------------------------------------+ | 21 | Orthogonalize columns of :math:`V` to all vectors :math:`X` | | | by solving | | | | | | .. math:: (X^TX) Q = X^T \bar{V} | | | | | | for :math:`Q` and updating | | | | | | .. math:: U = U - XQ | +----------+---------------------------------------------------------------+ | 22 | Orthogonalize columns of :math:`U` to all vectors :math:`X` | | | by solving | | | | | | .. math:: (X^TX) Q = X^T U | | | | | | for :math:`Q` and updating | | | | | | .. math:: U = U - XQ | +----------+---------------------------------------------------------------+ | 999 | Restart: | | | | | | If `rci.k>0`: Restart suggested with block size | | | `m >= rci.nx + rci.i + rci.j`, adjusting workspace size | | | to match. Set `rci.i=0` and `rci.j=0` and recall the routine. | | | If a restart is not desirable, routine may be recalled with | | | no change to parameters. | | | | | | If `rci.k=0`: Restart required with the same block size. | | | | | | In both cases, the first block ``W[0][:][:]`` should retain | | | vectors ``rci.jx:rci.jx+rci.nx-1``, filling remaining vectors | | | randomly such that the entire set of columns is linearly | | | independent from each other and also from the converged | | | eigenvectors. | +----------+---------------------------------------------------------------+ The matrices are defined as follows: * :math:`U` = ``W[rci.kx][rci.jx:rci.jx+rci.nx-1][:]`` * :math:`V` = ``W[rci.ky][rci.jy:rci.jy+rci.ny-1][:]`` * :math:`\bar{V}` = ``W[rci.ky][rci.jy:rci.jy+rci.nx-1][:]`` * :math:`R` = ``rr[rci.k][rci.j:rci.j+rci.ny-1][rci.i:rci.i+rci.nx-1]`` and :math:`\alpha` and :math:`\beta` are given by ``rci.alpha`` and ``rci.beta`` respectively. We use the notation :math:`r_{ii}` to refer to the :math:`i`-th diagonal element of :math:`R`, being ``rr[rci.k][rci.j+i-1][rci.i+i-1]``. :param rci: Reverse communication type. :c:member:`rci.job ` must be set to `0` before the first call. :param left: Number of left eigenpairs to find. :param mep: Number of working eigenpairs. See :ref:`method section ` for guidance on selecting a good value. Must be at least `left`. :param lambda[mep]: Current eigenvalue estimates in ascending order. :param m: Block size of workspace `W`. Must be at least `2`. :param rr[3][2*m][2*m]: reverse communication workspace. :param ind[m]: reverse communication workspace. :param keep: Internal workspace used by routine. :param options: specifies algorithm options to be used. :param inform: returns information about the exection of the routine. .. c:function:: void spral_ssmfe_expert_standard_double_complex(struct spral_ssmfe_rciz *rci, int left, int mep, double *lambda, int m, double complex *rr, int *ind, void **keep, const struct spral_ssmfe_options *options, struct spral_ssmfe_inform *inform) As :c:func:`spral_ssmfe_expert_standard_double()`, but types of ``rci``, and ``rr`` changed to support type ``double complex``. .. c:function:: void spral_ssmfe_expert_standard_shift_double(struct spral_ssmfe_rcid *rci, double sigma, int left, int right, int mep, double *lambda, int m, double *rr, int *ind, void **keep, const struct spral_ssmfe_options *options, struct spral_ssmfe_inform *inform) Computes eigenpairs of the standard eigenvalue problem .. math:: Ax = \lambda x in the vicinity of a given value :math:`sigma`. Uses reverse-communication. Upon return the user must perform a task specified by the `rci` parameter and recall the routine. Possible values of `rci` and associated tasks are: +----------+---------------------------------------------------------------+ | `rci.job`| Task to be performed | +==========+===============================================================+ | -3 | None. Fatal error, see :c:member:`inform.flag | | | `. | +----------+---------------------------------------------------------------+ | -2 | Failed to converge, see | | | :c:member:`inform.flag `. | +----------+---------------------------------------------------------------+ | -1 | None. Computation complete. | +----------+---------------------------------------------------------------+ | 2 | Apply preconditioner :math:`\bar{V} = TU`. (Copy if T=I). | +----------+---------------------------------------------------------------+ | 5 | Copy converged eigenvectors :math:`X` to user storage: | | | | | | * If `rci.i>0`: ``W[rci.kx][rci.jx:rci.jx+rci.nx-1][:]``. | | | * Else: ``W[rci.kx][rci.jx-rci.nx+1:rci.jx][:]``. | +----------+---------------------------------------------------------------+ | 9 | Compute :math:`V = (A-\sigma I)^{-1} U` | +----------+---------------------------------------------------------------+ | 11 | If `rci.i == 0`, copy :math:`\bar{V} = U`. | | | | | | Otherwise, reorder columns of block `rci.kx` such that column | | | `ind[j]` becomes the new column `j` for `j=0, ..., rci.nx-1` | | | | | | Note: if ``rci.kx == rci.ky``, only reorder once. | +----------+---------------------------------------------------------------+ | 12 | Compute the dot products | | | | | | .. math:: r_{ii} = U_i \cdot \bar{V}_i | +----------+---------------------------------------------------------------+ | 13 | Perform the scalings | | | | | | .. math:: U_i = U_i/\sqrt{(U_i\cdot \bar{V}_i)} | | | | | | and | | | | | | .. math:: \bar{V}_i = \bar{V}_i/\sqrt{(U_i\cdot \bar{V}_i)} | | | | | | for each column :math:`U_i` and :math:`\bar{V}_i` of :math:`U`| | | and :math:`\bar{V}`. | | | | | | Note: if ``rci.kx == rci.ky``, only scale once. | +----------+---------------------------------------------------------------+ | 14 | Perform the updates | | | | | | .. math:: \bar{V}_i = \bar{V}_i + r_{ii} U_i | | | | | | for each column :math:`\bar{V}_i` of :math:`\bar{V}` | +----------+---------------------------------------------------------------+ | 15 | Perform the update | | | | | | .. math:: R = \alpha U^T V + \beta R | +----------+---------------------------------------------------------------+ | 16 | Perform the update | | | | | | .. math:: V = \alpha U R + \beta V | +----------+---------------------------------------------------------------+ | 17 | Perform the update | | | | | | .. math:: U = \alpha U R | | | | | | Note: :math:`V` may be used as a workspace | +----------+---------------------------------------------------------------+ | 21 | Orthogonalize columns of :math:`V` to all vectors :math:`X` | | | by solving | | | | | | .. math:: (X^TX) Q = X^T \bar{V} | | | | | | for :math:`Q` and updating | | | | | | .. math:: U = U - XQ | +----------+---------------------------------------------------------------+ | 22 | Orthogonalize columns of :math:`U` to all vectors :math:`X` | | | by solving | | | | | | .. math:: (X^TX) Q = X^T U | | | | | | for :math:`Q` and updating | | | | | | .. math:: U = U - XQ | +----------+---------------------------------------------------------------+ | 999 | Restart: | | | | | | If `rci.k>0`: Restart suggested with block size | | | `m >= rci.nx + rci.i + rci.j`, adjusting workspace size | | | to match. Set `rci.i=0` and `rci.j=0` and recall the routine. | | | If a restart is not desirable, routine may be recalled with | | | no change to parameters. | | | | | | If `rci.k=0`: Restart required with the same block size. | | | | | | In both cases, the first block ``W[0][:][:]`` should retain | | | vectors ``rci.jx:rci.jx+rci.nx-1``, filling remaining vectors | | | randomly such that the entire set of columns is linearly | | | independent from each other and also from the converged | | | eigenvectors. | +----------+---------------------------------------------------------------+ The matrices are defined as follows: * :math:`U` = ``W[rci.kx][rci.jx:rci.jx+rci.nx-1][:]`` * :math:`V` = ``W[rci.ky][rci.jy:rci.jy+rci.ny-1][:]`` * :math:`\bar{V}` = ``W[rci.ky][rci.jy:rci.jy+rci.nx-1][:]`` * :math:`R` = ``rr[rci.k][rci.j:rci.j+rci.ny-1][rci.i:rci.i+rci.nx-1]`` and :math:`\alpha` and :math:`\beta` are given by ``rci.alpha`` and ``rci.beta`` respectively. We use the notation :math:`r_{ii}` to refer to the :math:`i`-th diagonal element of :math:`R`, being ``rr[rci.k][rci.j+i-1][rci.i+i-1]``. :param rci: Reverse communication type. :c:member:`rci.job ` must be set to `0` before the first call. :param sigma: Shift value :math:`sigma`. :param left: Number of left eigenpairs to find. :param right: Number of right eigenpairs to find. :param mep: Number of working eigenpairs. See :ref:`method section ` for guidance on selecting a good value. Must be at least `left+right`. :param lambda[mep]: Current eigenvalue estimates in ascending order. :param m: Block size of workspace `W`. Must be at least `2`. :param rr[3][2*m][2*m]: reverse communication workspace. :param ind[m]: reverse communication workspace. :param keep: Internal workspace used by routine. :param options: specifies algorithm options to be used. :param inform: returns information about the exection of the routine. .. c:function:: void spral_ssmfe_expert_standard_shift_double_complex(struct spral_ssmfe_rciz *rci, double sigma, int left, int right, int mep, double *lambda, int m, double complex *rr, int *ind, void **keep, const struct spral_ssmfe_options *options, struct spral_ssmfe_inform *inform) As :c:func:`spral_ssmfe_expert_standard_shift_double()`, but types of ``rci``, and ``rr`` changed to support type ``double complex``. .. c:function:: void spral_ssmfe_expert_generalized_double(struct spral_ssmfe_rcid *rci, int left, int mep, double *lambda, int m, double *rr, int *ind, void **keep, const struct spral_ssmfe_options *options, struct spral_ssmfe_inform *inform) Computes the left-most eigenpairs of the generalized eigenvalue problem .. math:: Ax = \lambda B x Optionally uses preconditioning. Uses reverse-communication. Upon return the user must perform a task specified by the `rci` parameter and recall the routine. Possible values of `rci` and associated tasks are: +----------+---------------------------------------------------------------+ | `rci.job`| Task to be performed | +==========+===============================================================+ | -3 | None. Fatal error, see :c:member:`inform.flag | | | `. | +----------+---------------------------------------------------------------+ | -2 | Failed to converge, see | | | :c:member:`inform.flag `. | +----------+---------------------------------------------------------------+ | -1 | None. Computation complete. | +----------+---------------------------------------------------------------+ |  1 | Calculate :math:`\bar{V} = AU`. | +----------+---------------------------------------------------------------+ | 2 | Apply preconditioner :math:`\bar{V} = TU`. (Copy if T=I). | +----------+---------------------------------------------------------------+ | 3 | Compute :math:`\bar{V} = BU` | +----------+---------------------------------------------------------------+ | 5 | Copy converged eigenvectors :math:`X` to user storage: | | | | | | * If `rci.i>0`: ``W[rci.kx][rci.jx:rci.jx+rci.nx-1][:]``. | | | * Else: ``W[rci.kx][rci.jx-rci.nx+1:rci.jx][:]``. | | | | | | Optionally save their :math:`B`-images: | | | | | | * If `rci.i>0`: ``W[rci.ky][rci.jx:rci.jx+rci.nx-1][:]``. | | | * Else: ``W[rci.ky][rci.jx-rci.nx+1:rci.jx][:]``. | +----------+---------------------------------------------------------------+ | 11 | If `rci.i == 0`, copy :math:`\bar{V} = U`. | | | | | | Otherwise, reorder columns of block `rci.kx` such that column | | | `ind[j]` becomes the new column `j` for `j=0, ..., rci.nx-1` | | | | | | Note: if ``rci.kx == rci.ky``, only reorder once. | +----------+---------------------------------------------------------------+ | 12 | Compute the dot products | | | | | | .. math:: r_{ii} = U_i \cdot \bar{V}_i | +----------+---------------------------------------------------------------+ | 13 | Perform the scalings | | | | | | .. math:: U_i = U_i/\sqrt{(U_i\cdot \bar{V}_i)} | | | | | | and | | | | | | .. math:: \bar{V}_i = \bar{V}_i/\sqrt{(U_i\cdot \bar{V}_i)} | | | | | | for each column :math:`U_i` and :math:`\bar{V}_i` of :math:`U`| | | and :math:`\bar{V}`. | | | | | | Note: if ``rci.kx == rci.ky``, only scale once. | +----------+---------------------------------------------------------------+ | 14 | Perform the updates | | | | | | .. math:: \bar{V}_i = \bar{V}_i + r_{ii} U_i | | | | | | for each column :math:`\bar{V}_i` of :math:`\bar{V}` | +----------+---------------------------------------------------------------+ | 15 | Perform the update | | | | | | .. math:: R = \alpha U^T V + \beta R | +----------+---------------------------------------------------------------+ | 16 | Perform the update | | | | | | .. math:: V = \alpha U R + \beta V | +----------+---------------------------------------------------------------+ | 17 | Perform the update | | | | | | .. math:: U = \alpha U R | | | | | | Note: :math:`V` may be used as a workspace | +----------+---------------------------------------------------------------+ | 21 | :math:`B`-orthogonalize columns of :math:`V` to all vectors | | | :math:`X` by solving | | | | | | .. math:: (X^TBX) Q = X^T \bar{V} | | | | | | for :math:`Q` and updating | | | | | | .. math:: | | | | | | U & = & U - XQ \\ | | | \bar{V} & = & \bar{V} - BXQ | | | | | | The update of :math:`\bar{V}` may be replaced by | | | | | | .. math:: \bar{V} = BU | +----------+---------------------------------------------------------------+ | 22 | :math:`B`-orthogonalize columns of :math:`U` to all vectors | | | :math:`X` by solving | | | | | | .. math:: (X^TBX) Q = X^T U | | | | | | for :math:`Q` and updating | | | | | | .. math:: U = U - BXQ | +----------+---------------------------------------------------------------+ | 999 | Restart: | | | | | | If `rci.k>0`: Restart suggested with block size | | | `m >= rci.nx + rci.i + rci.j`, adjusting workspace size | | | to match. Set `rci.i=0` and `rci.j=0` and recall the routine. | | | If a restart is not desirable, routine may be recalled with | | | no change to parameters. | | | | | | If `rci.k=0`: Restart required with the same block size. | | | | | | In both cases, the first block ``W[0][:][:]`` should retain | | | vectors ``rci.jx:rci.jx+rci.nx-1``, filling remaining vectors | | | randomly such that the entire set of columns is linearly | | | independent from each other and also from the converged | | | eigenvectors. | +----------+---------------------------------------------------------------+ The matrices are defined as follows: * :math:`U` = ``W[rci.kx][rci.jx:rci.jx+rci.nx-1][:]`` * :math:`V` = ``W[rci.ky][rci.jy:rci.jy+rci.ny-1][:]`` * :math:`\bar{V}` = ``W[rci.ky][rci.jy:rci.jy+rci.nx-1][:]`` * :math:`R` = ``rr[rci.k][rci.j:rci.j+rci.ny-1][rci.i:rci.i+rci.nx-1]`` and :math:`\alpha` and :math:`\beta` are given by ``rci.alpha`` and ``rci.beta`` respectively. We use the notation :math:`r_{ii}` to refer to the :math:`i`-th diagonal element of :math:`R`, being ``rr[rci.k][rci.j+i-1][rci.i+i-1]``. :param rci: Reverse communication type. :c:member:`rci.job ` must be set to `0` before the first call. :param left: Number of left eigenpairs to find. :param mep: Number of working eigenpairs. See :ref:`method section ` for guidance on selecting a good value. Must be at least `left`. :param lambda[mep]: Current eigenvalue estimates in ascending order. :param m: Block size of workspace `W`. Must be at least `2`. :param rr[3][2*m][2*m]: reverse communication workspace. :param ind[m]: reverse communication workspace. :param keep: Internal workspace used by routine. :param options: specifies algorithm options to be used. :param inform: returns information about the exection of the routine. .. c:function:: void spral_ssmfe_expert_generalized_double_complex(struct spral_ssmfe_rciz *rci, int left, int mep, double *lambda, int m, double complex *rr, int *ind, void **keep, const struct spral_ssmfe_options *options, struct spral_ssmfe_inform *inform) As :c:func:`spral_ssmfe_expert_generalized_double()`, but types of ``rci`` and ``rr`` changed to support type ``double complex``. .. c:function:: void spral_ssmfe_expert_generalized_shift_double(struct spral_ssmfe_rcid *rci, double sigma, int left, int right, int mep, double *lambda, int m, double *rr, int *ind, void **keep, const struct spral_ssmfe_options *options, struct spral_ssmfe_inform *inform) Computes eigenpairs of the generalized eigenvalue problem .. math:: Ax = \lambda B x in the vicinity of a given value :math:`\sigma`. Uses reverse-communication. Upon return the user must perform a task specified by the `rci` parameter and recall the routine. Possible values of `rci` and associated tasks are: +----------+---------------------------------------------------------------+ | `rci.job`| Task to be performed | +==========+===============================================================+ | -3 | None. Fatal error, see :c:member:`inform.flag | | | `. | +----------+---------------------------------------------------------------+ | -2 | Failed to converge, see | | | :c:member:`inform.flag `. | +----------+---------------------------------------------------------------+ | -1 | None. Computation complete. | +----------+---------------------------------------------------------------+ | 3 | Compute :math:`\bar{V} = BU` | +----------+---------------------------------------------------------------+ | 5 | Copy converged eigenvectors :math:`X` to user storage: | | | | | | * If `rci.i>0`: ``W[rci.kx][rci.jx:rci.jx+rci.nx-1][:]``. | | | * Else: ``W[rci.kx][rci.jx-rci.nx+1:rci.jx][:]``. | | | | | | Optionally save their :math:`B`-images: | | | | | | * If `rci.i>0`: ``W[rci.ky][rci.jx:rci.jx+rci.nx-1][:]``. | | | * Else: ``W[rci.ky][rci.jx-rci.nx+1:rci.jx][:]``. | +----------+---------------------------------------------------------------+ | 9 | Compute :math:`V = (A-\sigma B)^{-1} U` | +----------+---------------------------------------------------------------+ | 11 | If `rci.i == 0`, copy :math:`\bar{V} = U`. | | | | | | Otherwise, reorder columns of block `rci.kx` such that column | | | `ind[j]` becomes the new column `j` for `j=0, ..., rci.nx-1` | | | | | | Note: if ``rci.kx == rci.ky``, only reorder once. | +----------+---------------------------------------------------------------+ | 12 | Compute the dot products | | | | | | .. math:: r_{ii} = U_i \cdot \bar{V}_i | +----------+---------------------------------------------------------------+ | 13 | Perform the scalings | | | | | | .. math:: U_i = U_i/\sqrt{(U_i\cdot \bar{V}_i)} | | | | | | and | | | | | | .. math:: \bar{V}_i = \bar{V}_i/\sqrt{(U_i\cdot \bar{V}_i)} | | | | | | for each column :math:`U_i` and :math:`\bar{V}_i` of :math:`U`| | | and :math:`\bar{V}`. | | | | | | Note: if ``rci.kx == rci.ky``, only scale once. | +----------+---------------------------------------------------------------+ | 14 | Perform the updates | | | | | | .. math:: \bar{V}_i = \bar{V}_i + r_{ii} U_i | | | | | | for each column :math:`\bar{V}_i` of :math:`\bar{V}` | +----------+---------------------------------------------------------------+ | 15 | Perform the update | | | | | | .. math:: R = \alpha U^T V + \beta R | +----------+---------------------------------------------------------------+ | 16 | Perform the update | | | | | | .. math:: V = \alpha U R + \beta V | +----------+---------------------------------------------------------------+ | 17 | Perform the update | | | | | | .. math:: U = \alpha U R | | | | | | Note: :math:`V` may be used as a workspace | +----------+---------------------------------------------------------------+ | 21 | :math:`B`-orthogonalize columns of :math:`V` to all vectors | | | :math:`X` by solving | | | | | | .. math:: (X^TBX) Q = X^T \bar{V} | | | | | | for :math:`Q` and updating | | | | | | .. math:: | | | | | | U & = & U - XQ \\ | | | \bar{V} & = & \bar{V} - BXQ | | | | | | The update of :math:`\bar{V}` may be replaced by | | | | | | .. math:: \bar{V} = BU | +----------+---------------------------------------------------------------+ | 22 | :math:`B`-orthogonalize columns of :math:`U` to all vectors | | | :math:`X` by solving | | | | | | .. math:: (X^TBX) Q = X^T U | | | | | | for :math:`Q` and updating | | | | | | .. math:: U = U - BXQ | +----------+---------------------------------------------------------------+ | 999 | Restart: | | | | | | If `rci.k>0`: Restart suggested with block size | | | `m >= rci.nx + rci.i + rci.j`, adjusting workspace size | | | to match. Set `rci.i=0` and `rci.j=0` and recall the routine. | | | If a restart is not desirable, routine may be recalled with | | | no change to parameters. | | | | | | If `rci.k=0`: Restart required with the same block size. | | | | | | In both cases, the first block ``W[0][:][:]`` should retain | | | vectors ``rci.jx:rci.jx+rci.nx-1``, filling remaining vectors | | | randomly such that the entire set of columns is linearly | | | independent from each other and also from the converged | | | eigenvectors. | +----------+---------------------------------------------------------------+ The matrices are defined as follows: * :math:`U` = ``W[rci.kx][rci.jx:rci.jx+rci.nx-1][:]`` * :math:`V` = ``W[rci.ky][rci.jy:rci.jy+rci.ny-1][:]`` * :math:`\bar{V}` = ``W[rci.ky][rci.jy:rci.jy+rci.nx-1][:]`` * :math:`R` = ``rr[rci.k][rci.j:rci.j+rci.ny-1][rci.i:rci.i+rci.nx-1]`` and :math:`\alpha` and :math:`\beta` are given by ``rci.alpha`` and ``rci.beta`` respectively. We use the notation :math:`r_{ii}` to refer to the :math:`i`-th diagonal element of :math:`R`, being ``rr[rci.k][rci.j+i-1][rci.i+i-1]``. :param rci: Reverse communication type. :c:member:`rci.job ` must be set to `0` before the first call. :param sigma: Shift value :math:`sigma`. :param left: Number of left eigenpairs to find. :param right: Number of right eigenpairs to find. :param mep: Number of working eigenpairs. See :ref:`method section ` for guidance on selecting a good value. Must be at least `left+right`. :param lambda[mep]: Current eigenvalue estimates in ascending order. :param m: Block size of workspace `W`. Must be at least `2`. :param rr[3][2*m][2*m]: reverse communication workspace. :param ind[m]: reverse communication workspace. :param keep: Internal workspace used by routine. :param options: specifies algorithm options to be used. :param inform: returns information about the exection of the routine. .. c:function:: void spral_ssmfe_expert_generalized_shift_double_complex(struct spral_ssmfe_rciz *rci, double sigma, int left, int right, int mep, double *lambda, int m, double complex *rr, int *ind, void **keep, const struct spral_ssmfe_options *options, struct spral_ssmfe_inform *inform) As :c:func:`spral_ssmfe_expert_generalized_shift_double()`, but types of ``rci``, and ``rr`` changed to support type ``double complex``. .. c:function:: void spral_ssmfe_expert_buckling_double(struct spral_ssmfe_rcid *rci, double sigma, int left, int right, int mep, double *lambda, int m, double *rr, int *ind, void **keep, const struct spral_ssmfe_options *options, struct spral_ssmfe_inform *inform) Computes the eigenpairs of the buckling problem .. math:: Bx = \lambda A x in the vicinity of a given value :math:`\sigma`. Uses reverse-communication. Upon return the user must perform a task specified by the `rci` parameter and recall the routine. Possible values of `rci` and associated tasks are: +----------+---------------------------------------------------------------+ | `rci.job`| Task to be performed | +==========+===============================================================+ | -3 | None. Fatal error, see :c:member:`inform.flag | | | `. | +----------+---------------------------------------------------------------+ | -2 | Failed to converge, see | | | :c:member:`inform.flag `. | +----------+---------------------------------------------------------------+ | -1 | None. Computation complete. | +----------+---------------------------------------------------------------+ | 3 | Compute :math:`\bar{V} = BU` | +----------+---------------------------------------------------------------+ | 5 | Copy converged eigenvectors :math:`X` to user storage: | | | | | | * If `rci.i>0`: ``W[rci.kx][rci.jx:rci.jx+rci.nx-1][:]``. | | | * Else: ``W[rci.kx][rci.jx-rci.nx+1:rci.jx][:]``. | | | | | | Optionally save their :math:`B`-images: | | | | | | * If `rci.i>0`: ``W[rci.ky][rci.jx:rci.jx+rci.nx-1][:]``. | | | * Else: ``W[rci.ky][rci.jx-rci.nx+1:rci.jx][:]``. | +----------+---------------------------------------------------------------+ | 9 | Compute :math:`V = (B-\sigma A)^{-1} U` | +----------+---------------------------------------------------------------+ | 11 | If `rci.i == 0`, copy :math:`\bar{V} = U`. | | | | | | Otherwise, reorder columns of block `rci.kx` such that column | | | `ind[j]` becomes the new column `j` for `j=0, ..., rci.nx-1` | | | | | | Note: if ``rci.kx == rci.ky``, only reorder once. | +----------+---------------------------------------------------------------+ | 12 | Compute the dot products | | | | | | .. math:: r_{ii} = U_i \cdot \bar{V}_i | +----------+---------------------------------------------------------------+ | 13 | Perform the scalings | | | | | | .. math:: U_i = U_i/\sqrt{(U_i\cdot \bar{V}_i)} | | | | | | and | | | | | | .. math:: \bar{V}_i = \bar{V}_i/\sqrt{(U_i\cdot \bar{V}_i)} | | | | | | for each column :math:`U_i` and :math:`\bar{V}_i` of :math:`U`| | | and :math:`\bar{V}`. | | | | | | Note: if ``rci.kx == rci.ky``, only scale once. | +----------+---------------------------------------------------------------+ | 14 | Perform the updates | | | | | | .. math:: \bar{V}_i = \bar{V}_i + r_{ii} U_i | | | | | | for each column :math:`\bar{V}_i` of :math:`\bar{V}` | +----------+---------------------------------------------------------------+ | 15 | Perform the update | | | | | | .. math:: R = \alpha U^T V + \beta R | +----------+---------------------------------------------------------------+ | 16 | Perform the update | | | | | | .. math:: V = \alpha U R + \beta V | +----------+---------------------------------------------------------------+ | 17 | Perform the update | | | | | | .. math:: U = \alpha U R | | | | | | Note: :math:`V` may be used as a workspace | +----------+---------------------------------------------------------------+ | 21 | :math:`B`-orthogonalize columns of :math:`V` to all vectors | | | :math:`X` by solving | | | | | | .. math:: (X^TBX) Q = X^T \bar{V} | | | | | | for :math:`Q` and updating | | | | | | .. math:: | | | | | | U & = & U - XQ \\ | | | \bar{V} & = & \bar{V} - BXQ | | | | | | The update of :math:`\bar{V}` may be replaced by | | | | | | .. math:: \bar{V} = BU | +----------+---------------------------------------------------------------+ | 22 | :math:`B`-orthogonalize columns of :math:`U` to all vectors | | | :math:`X` by solving | | | | | | .. math:: (X^TBX) Q = X^T U | | | | | | for :math:`Q` and updating | | | | | | .. math:: U = U - BXQ | +----------+---------------------------------------------------------------+ | 999 | Restart: | | | | | | If `rci.k>0`: Restart suggested with block size | | | `m >= rci.nx + rci.i + rci.j`, adjusting workspace size | | | to match. Set `rci.i=0` and `rci.j=0` and recall the routine. | | | If a restart is not desirable, routine may be recalled with | | | no change to parameters. | | | | | | If `rci.k=0`: Restart required with the same block size. | | | | | | In both cases, the first block ``W[0][:][:]`` should retain | | | vectors ``rci.jx:rci.jx+rci.nx-1``, filling remaining vectors | | | randomly such that the entire set of columns is linearly | | | independent from each other and also from the converged | | | eigenvectors. | +----------+---------------------------------------------------------------+ The matrices are defined as follows: * :math:`U` = ``W[rci.kx][rci.jx:rci.jx+rci.nx-1][:]`` * :math:`V` = ``W[rci.ky][rci.jy:rci.jy+rci.ny-1][:]`` * :math:`\bar{V}` = ``W[rci.ky][rci.jy:rci.jy+rci.nx-1][:]`` * :math:`R` = ``rr[rci.k][rci.j:rci.j+rci.ny-1][rci.i:rci.i+rci.nx-1]`` and :math:`\alpha` and :math:`\beta` are given by ``rci.alpha`` and ``rci.beta`` respectively. We use the notation :math:`r_{ii}` to refer to the :math:`i`-th diagonal element of :math:`R`, being ``rr[rci.k][rci.j+i-1][rci.i+i-1]``. :param rci: Reverse communication type. :c:member:`rci.job ` must be set to `0` before the first call. :param sigma: Shift value :math:`sigma`. :param left: Number of left eigenpairs to find. :param right: Number of right eigenpairs to find. :param mep: Number of working eigenpairs. See :ref:`method section ` for guidance on selecting a good value. Must be at least `left+right`. :param lambda[mep]: Current eigenvalue estimates in ascending order. :param m: Block size of workspace `W`. Must be at least `2`. :param rr[3][2*m][2*m]: reverse communication workspace. :param ind[m]: reverse communication workspace. :param keep: Internal workspace used by routine. :param options: specifies algorithm options to be used. :param inform: returns information about the exection of the routine. .. c:function:: void spral_ssmfe_expert_buckling_double_complex(struct spral_ssmfe_rciz *rci, double sigma, int left, int right, int mep, double *lambda, int m, double complex *rr, int *ind, void **keep, const struct spral_ssmfe_options *options, struct spral_ssmfe_inform *inform) As :c:func:`spral_ssmfe_expert_buckling_double()`, but types of ``rci``, and ``rr`` changed to support type ``double complex``. .. c:function:: void spral_ssmfe_expert_free(void **keep, struct spral_ssmfe_inform *inform) Free memory allocated in `keep` and `inform`. :param keep: Workspace to be freed. :param inform: Information type to be freed. .. warning:: As memory in ``keep`` and ``inform`` has been allocated using Fortran functions, this routine **must** be called to avoid a memory leak. ============= Derived types ============= .. c:type:: struct spral_ssmfe_rcid Real-valued reverse communication interface (RCI) type. .. c:member:: int job Reverse-communication task to perform. .. c:member:: int jx First column of :math:`U` in block. .. c:member:: int kx Block to which :math:`U` belongs. .. c:member:: int nx Number of columns in :math:`U` and :math:`\bar{V}`, and number of rows in :math:`R`. .. c:member:: int jy First column of :math:`V` in block. .. c:member:: int ky Block to which :math:`V` belongs. .. c:member:: int ny Number of columns in :math:`V` and :math:`R`. .. c:member:: int i First row of :math:`R` in ``rr(:,:,:)``. .. c:member:: int j First column of :math:`R` in ``rr(:,:,:)``. .. c:member:: int k Block of :math:`R` in ``rr(:,:,:)``. .. c:member:: double alpha Coefficient for matrix multiplication. .. c:member:: double beta Coefficient for matrix multiplication. .. c:type:: struct spral_ssmfe_rciz Complex-valued reverse communication interface (RCI) type. .. c:member:: int job Reverse-communication task to perform. .. c:member:: int jx First column of :math:`U` in block. .. c:member:: int kx Block to which :math:`U` belongs. .. c:member:: int nx Number of columns in :math:`U` and :math:`\bar{V}`, and number of rows in :math:`R`. .. c:member:: int jy First column of :math:`V` in block. .. c:member:: int ky Block to which :math:`V` belongs. .. c:member:: int ny Number of columns in :math:`V` and :math:`R`. .. c:member:: int i First row of :math:`R` in ``rr(:,:,:)``. .. c:member:: int j First column of :math:`R` in ``rr(:,:,:)``. .. c:member:: int k Block of :math:`R` in ``rr(:,:,:)``. .. c:member:: double complex alpha Coefficient for matrix multiplication. .. c:member:: double complex beta Coefficient for matrix multiplication. .. c:type:: struct spral_ssmfe_options Options that control the algorithm. .. c:member:: double abs_tol_lambda Absolute tolerance for estimated eigenvalue convergence test, see :ref:`method section `. Negative values are treated as the default. Default is `0.0`. .. c:member:: double abs_tol_residual Absolute tolerance for residual convergence test, see :ref:`method section `. Negative values are treated as the default. Default is `0.0`. .. c:member:: int max_iterations Maximum number of iterations. Default is `100`. .. c:member:: double rel_tol_lambda Relative tolerance for estimated eigenvalue error convergence test, see :ref:`method section `. Negative values are treated as the default. Default is `0.0`. .. c:member:: double rel_tol_residual Relative tolerance for residual convergence test, see :ref:`method section `. If both `abs_tol_residual` and `rel_tol_residual` are 0.0, then the residual norms are not taken into consideration by the convergence test. Negative values are treated as the default. Default is `0.0`. .. c:member:: double tol_x Tolerance for estimated eigenvector error convergence test, see :ref:`method section `. If tol_x is set to `0.0`, the eigenvector error is not estimated. If a negative value is assigned, the tolerance is set to `sqrt(DBL_EPSILON)`. Default is `-1.0`. .. c:member:: int print_level Amount of printing. Possible values are: +----+------------------------------------------------------------------+ | <0 | no printing | +----+------------------------------------------------------------------+ | 0 | error and warning messages only | +----+------------------------------------------------------------------+ | 1 | the type (standard or generalized) and the size of the problem, | | | the number of eigenpairs requested, the error tolerances and the | | | size of the subspace are printed before the iterations start | +----+------------------------------------------------------------------+ | 2 | as above but, for each eigenpair tested for convergence, the | | | iteration number, the index of the eigenpair, the eigenvalue, | | | whether it has converged, the residual norm, and the error | | | estimates are also printed | +----+------------------------------------------------------------------+ | >2 | as 1 but with all eigenvalues, whether converged, residual norms | | | and eigenvalue/eigenvector error estimates printed on each | | | iteration. | +----+------------------------------------------------------------------+ Note that for eigenpairs that are far from convergence, ‘rough’ error estimates are printed (the estimates that are actually used by the stopping criteria, see Section [ssmfe:method], only become available on the last few iterations). Default is `0`. .. c:member:: int unit_error Fortran unit number for error messages. Printing suppressed if negative. Default is `6` (stdout). .. c:member:: int unit_diagnostic Fortran unit number for diagnostic messages. Printing suppressed if negative. Default is `6` (stdout). .. c:member:: int unit_warning Fortran unit number for warning messages. Printing suppressed if negative. Default is `6` (stdout). .. c:member:: int err_est Error estimation scheme, one of: +-------------+---------------------------------------------------------+ | 1 | Residual error bounds: modified Davis-Kahan estimate for| | | eigenvector error and Lehmann bounds for eigenvale error| | | (see method section). | +-------------+---------------------------------------------------------+ | 2 (default) | Convergence curve-based estimate. | +-------------+---------------------------------------------------------+ Default is `2`. .. c:member:: int extra_left Number of extra approximate eigenvectors corresponding to leftmost eigenvalues used to enhance convergence. Default is `0`. .. c:member:: int extra_right Number of extra approximate eigenvectors corresponding to rightmost eigenvalues used to enhance convergence. Default is `0`. .. c:member:: double left_gap Minimal acceptable distance between last computed left eigenvalue and rest of spectrum. For :c:func:`spral_ssmfe_expert_standard_double()` and :c:func:`spral_ssmfe_expert_generalized_double()` the last computed left eigenvalue is the rightmost of those computed. For other routines it is the leftmost. If set to a negative value :math:`\delta`, the minimal distance is taken as :math:`|\delta|` times the average distance between the computed eigenvalues. Note that for this option to have any effect, the value of `mep` must be larger than `left+right`. See :ref:`method section ` for further explanation. Default is `0`. .. c:member:: int max_left Number of eigenvalues to left of :math:`\sigma`, or a negative value if not known. Default is `-1`. .. c:member:: int max_right Number of eigenvalues to right of :math:`\sigma`, or a negative value if not known. Default is `-1`. .. c:member:: bool minAprod If true, minimize number of multiplications with :math:`A` by requiring 2 additional blocks of memory for the workspace ``W[:][:][:]``. Must be true for calls to :c:func:`spral_ssmfe_expert_standard_shift_double()`, :c:func:`spral_ssmfe_expert_generalized_shift_double()`, and :c:func:`spral_ssmfe_expert_buckling_double()`. Default is `true`. .. c:member:: bool minBprod If true, minimize number of multiplications with :math:`B` by requiring 2 additional blocks of memory for the workspace ``W[:][:][:]``. Default is `true`. .. c:member:: double right_gap As :c:member:`options.left_gap `, but for right eigenvalues. Default is `0.0`. .. c:member:: int user_x Number of eigenvectors for which an initial guess is supplied in `x[:][:]` on the first call. Such eigenvectors must be lineraly independent. Default is `0`. .. c:type:: struct spral_ssmfe_inform Information on progress of the algorithm. .. c:member:: int converged[mep] Convergence status. * If ``converged[j]>0``, the eigenpair `(lambda(j), X(j))` converged on iteration `converged[j]`. * If ``converged[j]=0``, the eigenpair `(lambda(j), X(j))` is still converging. * If ``converged[j]<0``, the eigenpair `(lambda(j), X(j))` stagnated at iteration `-converged[j]`. This component is allocated by the routine. .. c:member:: double err_lambda[mep]: Estimated eigenvalue errors for converged and stagnated eigenvalues. This component is allocated by the routine. .. c:member:: double err_x[mep] Estimated eigenvector errors for converged and stagnated eigenvectors. This component is allocated by the routine. .. c:member:: int flag Return status of algorithm. See table below. .. c:member:: int iteration Number of iterations. .. c:member:: int left Number of converged left eigenvalues. .. c:member:: double next_left Upon completion, next left eigenvalue in spectrum (see `options.left_gap`). .. c:member:: double next_right Upon completion, next right eigenvalue in spectrum (see `options.right_gap`). .. c:member:: double residual_norms[mep] Euclidean norms of residuals for `(lambda[:], X[:])` on return with ``rci.job=5``. This component is allocated by the routine. .. c:member:: int non_converged Number of non-converged eigenpairs. .. c:member:: int right Number of converged right eigenvalues. .. c:member:: int stat Fortran allocation status in event of failure. +--------------+-----------------------------------------------------------+ | `inform.flag`| | +==============+===========================================================+ | -1 | rci.job is out-of-range. | +--------------+-----------------------------------------------------------+ | -2 | m is out-of-range. | +--------------+-----------------------------------------------------------+ | -3 | options.err_est is out-of-range. | +--------------+-----------------------------------------------------------+ |  -4 | options.minAprod is incompatible with selected routine. | +--------------+-----------------------------------------------------------+ |  -5 | options.extra_left or options.extra_right is out-of-range.| +--------------+-----------------------------------------------------------+ |   -6 | options.min_gap is out-of-range. | +--------------+-----------------------------------------------------------+ | -11 | left is out-of-range. | +--------------+-----------------------------------------------------------+ | -12 | right is out-of-range. | +--------------+-----------------------------------------------------------+ | -13 | mep is less than the number of desired eigenpairs. | +--------------+-----------------------------------------------------------+ | -100 | Not enough memory; `inform.stat` contains the value of the| | | Fortran stat parameter. | +--------------+-----------------------------------------------------------+ | -200 | :math:`B` is not positive definite or `user_x>0` and | | | linearly dependent initial guesses were supplied. | +--------------+-----------------------------------------------------------+ | +1 | The iterations have been terminated because no further | | | improvement in accuracy is possible (this may happen if | | | :math:`B` or the preconditioner is not positive definite, | | | or if the components of the residual vectors are so small | | | that the round-off errors make them essentially random). | | | The value of `inform.non_converged` is set to the number | | | of non-converged eigenpairs. | +--------------+-----------------------------------------------------------+ | +2 | The maximum number of iterations `max_iterations` has been| | | exceeded. The value of `inform.non_converged` is set to | | | the number of non-converged eigenpairs. | +--------------+-----------------------------------------------------------+ | +3 | The solver had run out of storage space for the converged | | | eigenpairs before the gap in the spectrum required by | | | `options.left_gap` and/or `options.right_gap` was reached.| | | The value of `inform.non_converged` is set to the number | | | of non-converged eigenpairs. | +--------------+-----------------------------------------------------------+ .. _example: ======== Examples ======== Preconditioning example ----------------------- The following code computes the 5 leftmost eigenpairs of the matrix :math:`A` of order 100 that approximates the two-dimensional Laplacian operator on a 20-by-20 grid. One forward and one backward Gauss-Seidel update are used for preconditioning, which halves the number of iterations compared with solving the same problem without preconditioning. The header `laplace2d.h` (examples/C/ssmfe/laplace2d.h) supplies the subroutine `apply_laplacian()` that multiplies a block of vectors by :math:`A`, and the subroutine `apply_gauss_seidel_step()` that computes :math:`y = T x` for a block of vectors :math:`x` by applying one forward and one backward update of the Gauss-Seidel method to the system :math:`A y = x`. .. literalinclude:: ../../examples/C/ssmfe/precond_expert.c :language: C This code produces the following output:: 6 eigenpairs converged in 129 iterations lambda[0] = 4.4676695e-02 lambda[1] = 1.1119274e-01 lambda[2] = 1.1119274e-01 lambda[3] = 1.7770878e-01 lambda[4] = 2.2040061e-01 lambda[5] = 2.2040061e-01 Note that the code computed one extra eigenpair because of the insufficient gap between the 5th and 6th eigenvalues. .. _method: ====== Method ====== The algorithm ------------- The solver procedures of :f:mod:`spral_ssmfe_expert` are interfaces to solver procedures of :f:mod:`spral_ssmfe_core`, which implement a block iterative algorithm based on the Jacobi-conjugate preconditioned gradients method [2]_, [3]_. Further information on the algorithm used by :f:mod:`spral_ssmfe_expert` can be found in the specification document for :f:mod:`spral_ssmfe_core` and in [1]_. Stopping criteria ----------------- An approximate eigenpair :math:`\{x,\lambda\}` is considered to have converged if the following three conditions are all satisfied: #. if `options.abs_tol_lambda` and `options.rel_tol_lambda` are not both equal to zero, then the estimated error in the approximate eigenvalue must be less than or equal to :math:`\max(\mathrm{options\.abs\_tol\_lambda}, \delta*\mathrm{options\.rel\_tol\_lambda})`, where :math:`\delta` is the estimated average distance between eigenvalues. #. if `options.tol_x` is not zero, then the estimated sine of the angle between the approximate eigenvector and the invariant subspace corresponding to the eigenvalue approximated by :math:`\lambda` must be less than or equal to `options.tol_x`. #. if `options.abs_tol_residual` and `options.rel_tol_residual` are not both equal to zero, then the Euclidean norm of the residual, :math:`\|A x - \lambda B x\|_2`, must be less than or equal to :math:`\max(\mathrm{options\.abs\_tol\_residual}, \mathrm{options\.rel\_tol\_residual}*\|\lambda B x\|_2)`. The extra eigenpairs are not checked for convergence, as their role is purely auxiliary. Improving eigenvector accuracy ------------------------------ If the gap between the last computed eigenvalue and the rest of the spectrum is small, then the accuracy of the corresponding eigenvector may be very low. To prevent this from happening, the user should set the eigenpairs storage size mep to a value that is larger than the number of desired eigenpairs, and set the options `options.left_gap` and `options.right_gap` to non-zero values :math:`\delta_l` and :math:`\delta_r`. These values determine the size of the minimal acceptable gaps between the computed eigenvalues and the rest of the spectrum, :math:`\delta_l` referring to either leftmost eigenvalues (for :f:subr:`ssmfe_standard()` and :f:subr:`ssmfe_generalized()` only) or those to the left of the shift `sigma`, and :math:`\delta_r` to those to the right of the shift `sigma`. Positive values of :math:`\delta_l` and :math:`\delta_r` set the gap explicitly, and negative values require the gap to be not less than their absolute value times the average distance between the computed eigenvalues. A recommended value of :math:`\delta_l` and :math:`\delta_r` is :math:`-0.1`. The value of `mep` has little effect on the speed of computation, hence it might be set to any reasonably large value. The larger the value of `mep`, the larger the size of an eigenvalue cluster for which accurate eigenvectors can be computed, notably: to safeguard against clusters of size up to :math:`k`, it is sufficient to set mep to the number of desired eigenpairs plus :math:`k - 1`. The use of shifted matrix factorization --------------------------------------- When using the solver procedures that employ the shift-and-invert technique, it is very important to ensure that the numbers of desired eigenvalues each side of the shift do not exceed the actual numbers of these eigenvalues, as the eigenpairs ‘approximating’ non-existing eigenpairs of the problem will not converge. It is therefore strongly recommended that the user employs a linear system solver that performs the :math:`LDL^T` factorization of the shifted system, e.g. `HSL_MA97` or `SPRAL_SSIDS`. The :math:`LDL^T` factorization of the matrix :math:`A - \sigma B` consists in finding a lower triangular matrix :math:`L`, a block-diagonal matrix :math:`D` with :math:`1\times 1` and :math:`2\times 2` blocks on the diagonal and a permutation matrix :math:`P` such that :math:`P^T(A - \sigma B)P = L D L^T`. By the inertia theorem, the number of eigenvalues to the left and right from the shift :math:`\sigma` is equal to the number of negative and positive eigenvalues of :math:`D`, which allows quick computation of the eigenvalue numbers each side of the shift. Error estimation ---------------- Standard problem ~~~~~~~~~~~~~~~~ If ``options.err_est=1``, the error estimates for the eigenvalues are based on the eigenvalues of a matrix of the form .. math:: \begin{aligned} \label{L.mx} \hat A = \tilde\Lambda_k - S_k^T S_k,\end{aligned} where :math:`\tilde\Lambda_k` is a diagonal matrix with the :math:`k-1` leftmost Ritz values :math:`\tilde\lambda_j` on the diagonal, and the columns of :math:`S_k` are the respective residual vectors :math:`r_j = A \tilde x_j - \tilde\lambda_j \tilde x_j` divided by :math:`\sqrt{\lambda_k - \tilde\lambda_j}`. If :math:`k` is such that :math:`\tilde\lambda_{k-1} < \lambda_k`, then the eigenvalues of :math:`\hat A` are the left-hand side bounds for eigenvalues :math:`\lambda_i`, and thus the difference :math:`\tilde\lambda_j - \hat\lambda_j` estimates the eigenvalue error :math:`\tilde\lambda_j - \lambda_j`. The unknown :math:`\lambda_k` is replaced by :math:`\tilde\lambda_k`, and select the maximal :math:`k \le m` for which the distance between :math:`\tilde\lambda_{k-1}` and :math:`\tilde\lambda_k` exceeds the sum of the absolute error tolerance for eigenvalues and the Frobenius norm of the matrix formed by the residuals :math:`r_j, j = 1, \ldots, k-1`. If :math:`\tilde\lambda_j - \hat\lambda_j` is close to the machine accuracy, it may be too polluted by round-off errors to rely upon. In such case, we use instead .. math:: \begin{aligned} \tilde\lambda_j - \lambda_j \le \delta_j \approx \frac{\|r_j\|^2}{\tilde\lambda_k - \lambda_j}.\end{aligned} The eigenvector errors are estimated based on the Davis-Kahan inequality: .. math:: \begin{aligned} \min_{x \in \mathcal{X}_{k-1}} \sin\{\tilde x_j; x\} \le \frac{\|r_j\|}{\lambda_k - \tilde\lambda_j} \approx \frac{\|r_j\|}{\tilde\lambda_k - \tilde\lambda_j},\end{aligned} where :math:`\mathcal{X}_{k-1}` is the invariant subspace corresponding to :math:`k-1` leftmost eigenvalues. If ``options.err_est=2`` the errors are estimated based on the eigenvalue decrements history, which produces an estimate for the average eigenvalue error reduction per iteration, which in turn yields error estimates for both eigenvalues and eigenvectors. Unlike the residual estimates mentioned in this section, such ‘kinematic’ error estimates are not guaranteed to be upper bounds for the actual errors. However, the numerical tests have demonstrated that kinematic error estimates are significantly more accurate, i.e. closer to the actual error, than the residual-based estimates. Furthermore, they straightforwardly apply to the generalized case as well. Generalized problem ~~~~~~~~~~~~~~~~~~~ In the case of the generalized eigenvalue problem solved by iterations with preconditioning, all of the residual norms in the previous section must be replaced with :math:`\|\cdot\|_{B^{-1}}`-norm of the residual :math:`r_j = A \tilde x_j - \tilde\lambda_j B \tilde x_j` (:math:`\|r_j\|_{B^{-1}}^2 = r_j^* B^{-1} r_j`) or its upper estimate, e.g. :math:`\beta_1^{-1/2}\|\cdot\|`, where :math:`\beta_1` is the smallest eigenvalue of :math:`B`. Hence, if :math:`\beta_1` is known, then the error tolerances for eigenvalues and eigenvectors must be multiplied by :math:`\beta_1` and :math:`\sqrt{\beta_1}` respectively. If no estimate for :math:`\|\cdot\|_{B^{-1}}`-norm is available, then the use of non-zero residual tolerances and ``options.err_est=1`` is not recommended. In the case of problems solved by iterations with shift-and-invert and the problem , the residuals are computed as :math:`r_j = T B \tilde x_j - \tilde \lambda_j \tilde x_j` where :math:`T = (A - \sigma B)^{-1}` for and :math:`T = (B - \sigma A)^{-1}` for , and :math:`B`-norms of :math:`r_j` are used, so that Lehmann matrix becomes :math:`\hat A = \tilde\Lambda_k - S_k^T B\ S_k`. 0 Note that the residual estimates may considerably overestimate the actual error of direct iterations because of the use of the Euclidean norm of the residual, which is too strong a norm for it when :math:`A` is the discretization of a differential operator. References ---------- .. [1] E. E. Ovtchinnikov and J. Reid (2010). *A preconditioned block conjugate gradient algorithm for computing extreme eigenpairs of symmetric and Hermitian problems*. Technical Report RAL-TR-2010-19. .. [2] E. E. Ovtchinnikov (2008). *Jacobi correction equation, line search and conjugate gradients in Hermitian eigenvalue computation I: Computing an extreme eigenvalue*. SIAM J. Numer. Anal., 46:2567–2592. .. [3] E. E. Ovtchinnikov (2008). *Jacobi correction equation, line search and conjugate gradients in Hermitian eigenvalue computation II: Computing several extreme eigenvalues*. SIAM J. Numer. Anal., 46:2593–2619.