DIIS

DIIS (Pulay 1980) (direct inversion of the iterative subspace) is a technique to accelerate convergence in solving linear equations. Let’s say we have already found \(n\) estimates to the problem \(\require{physics} \set{\vb{x}_i}\). We can construct a new estimate \(\vb{x}^*\) as a linear combination of the previous ones: \[\begin{equation} \label{eq:DIIS_linear_combination} \vb{x}^* = \sum_i^n c_i \vb{x}_i \thinspace . \end{equation}\] Let’s say we also have a way to construct an error vector \(\vb{e}_i\) for every estimate, such that our goal will be to minimize the error function in a least squares sense: \[\begin{equation} \norm{\sum_i^n c_i \vb{e}_i}^2 \thinspace , \end{equation}\] under the constraint that \[\begin{equation} \sum_i^n c_i = 1 \thinspace . \end{equation}\] We can then construct the Lagriangian for this problem as \[\begin{equation} \mathcal{L}(\set{c_i}, \lambda) = \norm{\sum_i^n c_i \vb{e}_i}^2 - \lambda \qty( \sum_i^n c_i - 1 ) \thinspace , \end{equation}\] and by introducing a suitable scalar product between the error vectors \[\begin{equation} B_{ij} = (\vb{e}_i, \vb{e}_j) \thinspace , \end{equation}\] we can write the Lagrangian as \[\begin{equation} \mathcal{L}(\set{c_i}, \lambda) = \sum_{ij}^n c_i c_j B_{ij} - \lambda \qty(\sum_i^n c_i - 1) \thinspace . \end{equation}\] Differentiating with respect to \(\lambda\) gives us back the original constraint, and differentiating with respect to every coefficient leads to \[\begin{equation} \pdv{\mathcal{L}}{c_k} = 0 = 2 \sum_i^n c_i B_{ik} - \lambda \thinspace , \end{equation}\] as the inner product matrix is symmetric. Absorbing the factor 2 in the Lagrange multiplier, we find the following system of equations \[\begin{equation} \begin{pmatrix} B_{11} & B_{12} & \cdots & B_{1n} & -1 \\ B_{21} & B_{22} & \cdots & B_{2n} & -1 \\ \vdots & \vdots & \ddots & \vdots & \vdots \\ B_{n1} & B_{n2} & \cdots & B_{nn} & -1 \\ -1 & -1 & \cdots & -1 & 0 \end{pmatrix} \begin{pmatrix} c_1 \\ c_2 \\ \vdots \\ c_n \\ \lambda \end{pmatrix} = \begin{pmatrix} 0 \\ 0 \\ \vdots \\ 0 \\ -1 \end{pmatrix} \thinspace . \end{equation}\] We can recognize a linear system of equations of the form \(\vb{B}' \vb{y} = \vb{b}\), which can be easily solved using various decomposition techniques, leading to the coefficients \(\qty{c_i}\) which are then used in constructing the new estimate as in equation \(\eqref{eq:DIIS_linear_combination}\).

What remains is to construct a way to define the error vectors associated to every estimate \(\vb{x}_i\), and a standard way would be to define residual vectors as \[\begin{equation} \vb{e}_i = \vb{x}_{i+1} - \vb{x}_i \thinspace . \end{equation}\] As an example, after 3 standard iterations, we end up with a set \(\qty{\vb{x}_1, \vb{x}_2, \vb{x}_3}\). We can then calculate \[\begin{align} &\vb{e}_1 = \vb{x}_2 - \vb{x}_1 \\ &\vb{e}_2 = \vb{x}_3 - \vb{x}_2 \thinspace , \end{align}\] We can then set up the DIIS equations to find the coefficients \(c_1\) and \(c_2\), in order to construct a new guess vector \(\vb{x}_3\), which is in a sense ‘overwritten’. This DIIS-improved guess vector is then used as a starting point for the next iteration.

References

Pulay, Péter. 1980. Convergence Acceleration of Iterative Sequences. The Case of SCF iIeration.” Chemical Physics Letters 73 (2): 393–98. https://doi.org/10.1016/0009-2614(80)80396-4.