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351 \usepackage[utf8]{inputenc}
352 \usepackage[T1]{fontenc}
353 \usepackage{algorithm}
354 \usepackage{algpseudocode}
357 \usepackage{multirow}
358 \usepackage{graphicx}
360 \algnewcommand\algorithmicinput{\textbf{Input:}}
361 \algnewcommand\Input{\item[\algorithmicinput]}
363 \algnewcommand\algorithmicoutput{\textbf{Output:}}
364 \algnewcommand\Output{\item[\algorithmicoutput]}
366 \newtheorem{proposition}{Proposition}
371 % can use linebreaks \\ within to get better formatting as desired
372 \title{TSIRM: A Two-Stage Iteration with least-squares Residual Minimization algorithm to solve large sparse linear systems}
379 % author names and affiliations
380 % use a multiple column layout for up to two different
383 \author{\IEEEauthorblockN{Rapha\"el Couturier\IEEEauthorrefmark{1}, Lilia Ziane Khodja\IEEEauthorrefmark{2}, and Christophe Guyeux\IEEEauthorrefmark{1}}
384 \IEEEauthorblockA{\IEEEauthorrefmark{1} Femto-ST Institute, University of Franche-Comt\'e, France\\
385 Email: \{raphael.couturier,christophe.guyeux\}@univ-fcomte.fr}
386 \IEEEauthorblockA{\IEEEauthorrefmark{2} INRIA Bordeaux Sud-Ouest, France\\
387 Email: lilia.ziane@inria.fr}
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404 %Eldon Tyrell\IEEEauthorrefmark{4}}
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406 %Georgia Institute of Technology,
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417 % use for special paper notices
418 %\IEEEspecialpapernotice{(Invited Paper)}
423 % make the title area
428 In this article, a two-stage iterative algorithm is proposed to improve the
429 convergence of Krylov based iterative methods, typically those of GMRES
430 variants. The principle of the proposed approach is to build an external
431 iteration over the Krylov method, and to frequently store its current residual
432 (at each GMRES restart for instance). After a given number of outer iterations,
433 a least-squares minimization step is applied on the matrix composed by the saved
434 residuals, in order to compute a better solution and to make new iterations if
435 required. It is proven that the proposal has the same convergence properties
436 than the inner embedded method itself. Experiments using up to 16,394 cores
437 also show that the proposed algorithm runs around 5 or 7 times faster than
442 Iterative Krylov methods; sparse linear systems; two stage iteration; least-squares residual minimization; PETSc
446 % For peer review papers, you can put extra information on the cover
448 % \ifCLASSOPTIONpeerreview
449 % \begin{center} \bfseries EDICS Category: 3-BBND \end{center}
452 % For peerreview papers, this IEEEtran command inserts a page break and
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496 %\label{fig_first_case}}
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538 % footnotes above bottom floats. This can be corrected via the \fnbelowfloat
539 % command of the stfloats package.
543 %%%*********************************************************
544 %%%*********************************************************
545 \section{Introduction}
547 % You must have at least 2 lines in the paragraph with the drop letter
548 % (should never be an issue)
550 Iterative methods have recently become more attractive than direct ones to solve
551 very large sparse linear systems\cite{Saad2003}. They are more efficient in a
552 parallel context, supporting thousands of cores, and they require less memory
553 and arithmetic operations than direct methods~\cite{bahicontascoutu}. This is
554 why new iterative methods are frequently proposed or adapted by researchers, and
555 the increasing need to solve very large sparse linear systems has triggered the
556 development of such efficient iterative techniques suitable for parallel
559 Most of the successful iterative methods currently available are based on
560 so-called ``Krylov subspaces''. They consist in forming a basis of successive
561 matrix powers multiplied by an initial vector, which can be for instance the
562 residual. These methods use vectors orthogonality of the Krylov subspace basis
563 in order to solve linear systems. The most known iterative Krylov subspace
564 methods are conjugate gradient and GMRES ones (Generalized Minimal RESidual).
567 However, iterative methods suffer from scalability problems on parallel
568 computing platforms with many processors, due to their need of reduction
569 operations, and to collective communications to achieve matrix-vector
570 multiplications. The communications on large clusters with thousands of cores
571 and large sizes of messages can significantly affect the performances of these
572 iterative methods. As a consequence, Krylov subspace iteration methods are often
573 used with preconditioners in practice, to increase their convergence and
574 accelerate their performances. However, most of the good preconditioners are
575 not scalable on large clusters.
577 In this research work, a two-stage algorithm based on two nested iterations
578 called inner-outer iterations is proposed. This algorithm consists in solving
579 the sparse linear system iteratively with a small number of inner iterations,
580 and restarting the outer step with a new solution minimizing some error
581 functions over some previous residuals. For further information on two-stage
582 iteration methods, interested readers are invited to
583 consult~\cite{Nichols:1973:CTS}. Two-stage algorithms are easy to parallelize on
584 large clusters. Furthermore, the least-squares minimization technique improves
585 its convergence and performances.
587 The present article is organized as follows. Related works are presented in
588 Section~\ref{sec:02}. Section~\ref{sec:03} details the two-stage algorithm using
589 a least-squares residual minimization, while Section~\ref{sec:04} provides
590 convergence results regarding this method. Section~\ref{sec:05} shows some
591 experimental results obtained on large clusters using routines of PETSc
592 toolkit. This research work ends by a conclusion section, in which the proposal
593 is summarized while intended perspectives are provided.
595 %%%*********************************************************
596 %%%*********************************************************
600 %%%*********************************************************
601 %%%*********************************************************
602 \section{Related works}
604 %Wherever Times is specified, Times Roman or Times New Roman may be used. If neither is available on your system, please use the font closest in appearance to Times. Avoid using bit-mapped fonts if possible. True-Type 1 or Open Type fonts are preferred. Please embed symbol fonts, as well, for math, etc.
605 %%%*********************************************************
606 %%%*********************************************************
610 %%%*********************************************************
611 %%%*********************************************************
612 \section{Two-stage iteration with least-squares residuals minimization algorithm}
614 A two-stage algorithm is proposed to solve large sparse linear systems of the
615 form $Ax=b$, where $A\in\mathbb{R}^{n\times n}$ is a sparse and square
616 nonsingular matrix, $x\in\mathbb{R}^n$ is the solution vector, and
617 $b\in\mathbb{R}^n$ is the right-hand side. As explained previously,
618 the algorithm is implemented as an
619 inner-outer iteration solver based on iterative Krylov methods. The main
620 key-points of the proposed solver are given in Algorithm~\ref{algo:01}.
621 It can be summarized as follows: the
622 inner solver is a Krylov based one. In order to accelerate its convergence, the
623 outer solver periodically applies a least-squares minimization on the residuals computed by the inner one. %Tsolver which does not required to be changed.
625 At each outer iteration, the sparse linear system $Ax=b$ is partially solved
626 using only $m$ iterations of an iterative method, this latter being initialized
627 with the last obtained approximation. GMRES method~\cite{Saad86}, or any of its
628 variants, can potentially be used as inner solver. The current approximation of
629 the Krylov method is then stored inside a $n \times s$ matrix $S$, which is
630 composed by the $s$ last solutions that have been computed during the inner
631 iterations phase. In the remainder, the $i$-th column vector of $S$ will be
634 At each $s$ iterations, another kind of minimization step is applied in order to
635 compute a new solution $x$. For that, the previous residuals of $Ax=b$ are computed by
636 the inner iterations with $(b-AS)$. The minimization of the residuals is obtained by
638 \underset{\alpha\in\mathbb{R}^{s}}{min}\|b-R\alpha\|_2
641 with $R=AS$. The new solution $x$ is then computed with $x=S\alpha$.
644 In practice, $R$ is a dense rectangular matrix belonging in $\mathbb{R}^{n\times s}$,
645 with $s\ll n$. In order to minimize~\eqref{eq:01}, a least-squares method such as
646 CGLS ~\cite{Hestenes52} or LSQR~\cite{Paige82} is used. Remark that these methods are more
647 appropriate than a single direct method in a parallel context.
653 \begin{algorithmic}[1]
654 \Input $A$ (sparse matrix), $b$ (right-hand side)
655 \Output $x$ (solution vector)\vspace{0.2cm}
656 \State Set the initial guess $x_0$
657 \For {$k=1,2,3,\ldots$ until convergence (error$<\epsilon_{tsirm}$)} \label{algo:conv}
658 \State $[x_k,error]=Solve(A,b,x_{k-1},max\_iter_{kryl})$ \label{algo:solve}
659 \State $S_{k \mod s}=x_k$ \label{algo:store} \Comment{update column (k mod s) of S}
660 \If {$k \mod s=0$ {\bf and} error$>\epsilon_{kryl}$}
661 \State $R=AS$ \Comment{compute dense matrix} \label{algo:matrix_mul}
662 \State $\alpha=Least\_Squares(R,b,max\_iter_{ls})$ \label{algo:}
663 \State $x_k=S\alpha$ \Comment{compute new solution}
670 Algorithm~\ref{algo:01} summarizes the principle of the proposed method. The
671 outer iteration is inside the \emph{for} loop. Line~\ref{algo:solve}, the Krylov
672 method is called for a maximum of $max\_iter_{kryl}$ iterations. In practice,
673 we suggest to set this parameter equal to the restart number in the GMRES-like
674 method. Moreover, a tolerance threshold must be specified for the solver. In
675 practice, this threshold must be much smaller than the convergence threshold of
676 the TSIRM algorithm (\emph{i.e.}, $\epsilon_{tsirm}$). We also consider that
677 after the call of the $Solve$ function, we obtain the vector $x_k$ and the error
678 which is defined by $||Ax^k-b||_2$.
680 Line~\ref{algo:store},
681 $S_{k \mod s}=x^k$ consists in copying the solution $x_k$ into the column $k
682 \mod s$ of $S$. After the minimization, the matrix $S$ is reused with the new
683 values of the residuals. To solve the minimization problem, an iterative method
684 is used. Two parameters are required for that: the maximum number of iterations
685 and the threshold to stop the method.
687 Let us summarize the most important parameters of TSIRM:
689 \item $\epsilon_{tsirm}$: the threshold to stop the TSIRM method;
690 \item $max\_iter_{kryl}$: the maximum number of iterations for the Krylov method;
691 \item $s$: the number of outer iterations before applying the minimization step;
692 \item $max\_iter_{ls}$: the maximum number of iterations for the iterative least-squares method;
693 \item $\epsilon_{ls}$: the threshold used to stop the least-squares method.
697 The parallelization of TSIRM relies on the parallelization of all its
698 parts. More precisely, except the least-squares step, all the other parts are
699 obvious to achieve out in parallel. In order to develop a parallel version of
700 our code, we have chosen to use PETSc~\cite{petsc-web-page}. For
701 line~\ref{algo:matrix_mul} the matrix-matrix multiplication is implemented and
702 efficient since the matrix $A$ is sparse and since the matrix $S$ contains few
703 columns in practice. As explained previously, at least two methods seem to be
704 interesting to solve the least-squares minimization, CGLS and LSQR.
706 In the following we remind the CGLS algorithm. The LSQR method follows more or
707 less the same principle but it takes more place, so we briefly explain the parallelization of CGLS which is similar to LSQR.
711 \begin{algorithmic}[1]
712 \Input $A$ (matrix), $b$ (right-hand side)
713 \Output $x$ (solution vector)\vspace{0.2cm}
714 \State Let $x_0$ be an initial approximation
718 \State $\gamma=||s_0||^2_2$
719 \For {$k=1,2,3,\ldots$ until convergence ($\gamma<\epsilon_{ls}$)} \label{algo2:conv}
721 \State $\alpha_k=\gamma/||q_k||^2_2$
722 \State $x_k=x_{k-1}+\alpha_kp_k$
723 \State $r_k=r_{k-1}-\alpha_kq_k$
725 \State $\gamma_{old}=\gamma$
726 \State $\gamma=||s_k||^2_2$
727 \State $\beta_k=\gamma/\gamma_{old}$
728 \State $p_{k+1}=s_k+\beta_kp_k$
735 In each iteration of CGLS, there is two matrix-vector multiplications and some
736 classical operations: dot product, norm, multiplication and addition on vectors. All
737 these operations are easy to implement in PETSc or similar environment.
741 %%%*********************************************************
742 %%%*********************************************************
744 \section{Convergence results}
748 We can now claim that,
751 If $A$ is either a definite positive or a positive matrix and GMRES($m$) is used as solver, then the TSIRM algorithm is convergent.
753 Furthermore, let $r_k$ be the
754 $k$-th residue of TSIRM, then
755 we have the following boundaries:
757 \item when $A$ is positive:
759 ||r_k|| \leqslant \left(1-\dfrac{\alpha}{\beta}\right)^{\frac{km}{2}} ||r_0|| ,
761 where $M$ is the symmetric part of $A$, $\alpha = \lambda_{min}(M)^2$ and $\beta = \lambda_{max}(A^T A)$;
762 \item when $A$ is positive definite:
764 \|r_k\| \leq \left( 1-\frac{\lambda_{\mathrm{min}}^2(1/2(A^T + A))}{ \lambda_{\mathrm{max}}(A^T A)} \right)^{km/2} \|r_0\|.
767 %In the general case, where A is not positive definite, we have
768 %$\|r_n\| \le \inf_{p \in P_n} \|p(A)\| \le \kappa_2(V) \inf_{p \in P_n} \max_{\lambda \in \sigma(A)} |p(\lambda)| \|r_0\|, .$
772 Let us first recall that the residue is under control when considering the GMRES algorithm on a positive definite matrix, and it is bounded as follows:
774 \|r_k\| \leq \left( 1-\frac{\lambda_{\mathrm{min}}^2(1/2(A^T + A))}{ \lambda_{\mathrm{max}}(A^T A)} \right)^{k/2} \|r_0\| .
776 Additionally, when $A$ is a positive real matrix with symmetric part $M$, then the residual norm provided at the $m$-th step of GMRES satisfies:
778 ||r_m|| \leqslant \left(1-\dfrac{\alpha}{\beta}\right)^{\frac{m}{2}} ||r_0|| ,
780 where $\alpha$ and $\beta$ are defined as in Proposition~\ref{prop:saad}, which proves
781 the convergence of GMRES($m$) for all $m$ under such assumptions regarding $A$.
782 These well-known results can be found, \emph{e.g.}, in~\cite{Saad86}.
784 We will now prove by a mathematical induction that, for each $k \in \mathbb{N}^\ast$,
785 $||r_k|| \leqslant \left(1-\dfrac{\alpha}{\beta}\right)^{\frac{mk}{2}} ||r_0||$ when $A$ is positive, and $\|r_k\| \leq \left( 1-\frac{\lambda_{\mathrm{min}}^2(1/2(A^T + A))}{ \lambda_{\mathrm{max}}(A^T A)} \right)^{km/2} \|r_0\|$ when $A$ is positive definite.
787 The base case is obvious, as for $k=1$, the TSIRM algorithm simply consists in applying GMRES($m$) once, leading to a new residual $r_1$ that follows the inductive hypothesis due, to the results recalled above.
789 Suppose now that the claim holds for all $m=1, 2, \hdots, k-1$, that is, $\forall m \in \{1,2,\hdots, k-1\}$, $||r_m|| \leqslant \left(1-\dfrac{\alpha}{\beta}\right)^{\frac{km}{2}} ||r_0||$ in the positive case, and $\|r_k\| \leq \left( 1-\frac{\lambda_{\mathrm{min}}^2(1/2(A^T + A))}{ \lambda_{\mathrm{max}}(A^T A)} \right)^{km/2} \|r_0\|$ in the definite positive one.
790 We will show that the statement holds too for $r_k$. Two situations can occur:
792 \item If $k \not\equiv 0 ~(\textrm{mod}\ m)$, then the TSIRM algorithm consists in executing GMRES once. In that case and by using the inductive hypothesis, we obtain either $||r_k|| \leqslant \left(1-\dfrac{\alpha}{\beta}\right)^{\frac{m}{2}} ||r_{k-1}||\leqslant \left(1-\dfrac{\alpha}{\beta}\right)^{\frac{km}{2}} ||r_0||$ if $A$ is positive, or $\|r_k\| \leqslant \left( 1-\frac{\lambda_{\mathrm{min}}^2(1/2(A^T + A))}{ \lambda_{\mathrm{max}}(A^T A)} \right)^{m/2} \|r_{k-1}\|$ $\leqslant$ $\left( 1-\frac{\lambda_{\mathrm{min}}^2(1/2(A^T + A))}{ \lambda_{\mathrm{max}}(A^T A)} \right)^{km/2} \|r_{0}\|$ in the positive definite case.
793 \item Else, the TSIRM algorithm consists in two stages: a first GMRES($m$) execution leads to a temporary $x_k$ whose residue satisfies:
795 \item $||r_k|| \leqslant \left(1-\dfrac{\alpha}{\beta}\right)^{\frac{m}{2}} ||r_{k-1}||\leqslant \left(1-\dfrac{\alpha}{\beta}\right)^{\frac{km}{2}} ||r_0||$ in the positive case,
796 \item $\|r_k\| \leqslant \left( 1-\frac{\lambda_{\mathrm{min}}^2(1/2(A^T + A))}{ \lambda_{\mathrm{max}}(A^T A)} \right)^{m/2} \|r_{k-1}\|$ $\leqslant$ $\left( 1-\frac{\lambda_{\mathrm{min}}^2(1/2(A^T + A))}{ \lambda_{\mathrm{max}}(A^T A)} \right)^{km/2} \|r_{0}\|$ in the positive definite one,
798 and a least squares resolution.
799 Let $\operatorname{span}(S) = \left \{ {\sum_{i=1}^k \lambda_i v_i \Big| k \in \mathbb{N}, v_i \in S, \lambda _i \in \mathbb{R}} \right \}$ be the linear span of a set of real vectors $S$. So,\\
800 $\min_{\alpha \in \mathbb{R}^s} ||b-R\alpha ||_2 = \min_{\alpha \in \mathbb{R}^s} ||b-AS\alpha ||_2$
803 & = \min_{x \in span\left(S_{k-s+1}, S_{k-s+2}, \hdots, S_{k} \right)} ||b-AS\alpha ||_2\\
804 & = \min_{x \in span\left(x_{k-s+1}, x_{k-s}+2, \hdots, x_{k} \right)} ||b-AS\alpha ||_2\\
805 & \leqslant \min_{x \in span\left( x_{k} \right)} ||b-Ax ||_2\\
806 & \leqslant \min_{\lambda \in \mathbb{R}} ||b-\lambda Ax_{k} ||_2\\
807 & \leqslant ||b-Ax_{k}||_2\\
809 & \leqslant \left(1-\dfrac{\alpha}{\beta}\right)^{\frac{km}{2}} ||r_0||, \textrm{ if $A$ is positive,}\\
810 & \leqslant \left( 1-\frac{\lambda_{\mathrm{min}}^2(1/2(A^T + A))}{ \lambda_{\mathrm{max}}(A^T A)} \right)^{km/2} \|r_{0}\|, \textrm{ if $A$ is}\\
811 & \textrm{positive definite,}
814 which concludes the induction and the proof.
817 %We can remark that, at each iterate, the residue of the TSIRM algorithm is lower
818 %than the one of the GMRES method.
820 %%%*********************************************************
821 %%%*********************************************************
822 \section{Experiments using PETSc}
826 In order to see the behavior of the proposal when considering only one processor, a first
827 comparison with GMRES or FGMRES and the new algorithm detailed previously has been experimented.
828 Matrices that have been used with their characteristics (names, fields, rows, and nonzero coefficients) are detailed in
829 Table~\ref{tab:01}. These latter, which are real-world applications matrices,
831 from the Davis collection, University of
832 Florida~\cite{Dav97}.
836 \begin{tabular}{|c|c|r|r|r|}
838 Matrix name & Field &\# Rows & \# Nonzeros \\\hline \hline
839 crashbasis & Optimization & 160,000 & 1,750,416 \\
840 parabolic\_fem & Comput. fluid dynamics & 525,825 & 2,100,225 \\
841 epb3 & Thermal problem & 84,617 & 463,625 \\
842 atmosmodj & Comput. fluid dynamics & 1,270,432 & 8,814,880 \\
843 bfwa398 & Electromagnetics pb & 398 & 3,678 \\
844 torso3 & 2D/3D problem & 259,156 & 4,429,042 \\
848 \caption{Main characteristics of the sparse matrices chosen from the Davis collection}
853 The following parameters have been chosen for our experiments. As by default
854 the restart of GMRES is performed every 30 iterations, we have chosen to stop
855 the GMRES every 30 iterations (\emph{i.e.} $max\_iter_{kryl}=30$). $s$ is set to 8. CGLS is
856 chosen to minimize the least-squares problem with the following parameters:
857 $\epsilon_{ls}=1e-40$ and $max\_iter_{ls}=20$. The external precision is set to
858 $\epsilon_{tsirm}=1e-10$. Those experiments have been performed on a Intel(R)
859 Core(TM) i7-3630QM CPU @ 2.40GHz with the version 3.5.1 of PETSc.
862 In Table~\ref{tab:02}, some experiments comparing the solving of the linear
863 systems obtained with the previous matrices with a GMRES variant and with out 2
864 stage algorithm are given. In the second column, it can be noticed that either
865 GRMES or FGMRES (Flexible GMRES)~\cite{Saad:1993} is used to solve the linear
866 system. According to the matrices, different preconditioner is used. With
867 TSIRM, the same solver and the same preconditionner are used. This Table shows
868 that TSIRM can drastically reduce the number of iterations to reach the
869 convergence when the number of iterations for the normal GMRES is more or less
870 greater than 500. In fact this also depends on tow parameters: the number of
871 iterations to stop GMRES and the number of iterations to perform the
877 \begin{tabular}{|c|c|r|r|r|r|}
880 \multirow{2}{*}{Matrix name} & Solver / & \multicolumn{2}{c|}{GMRES} & \multicolumn{2}{c|}{TSIRM CGLS} \\
882 & precond & Time & \# Iter. & Time & \# Iter. \\\hline \hline
884 crashbasis & gmres / none & 15.65 & 518 & 14.12 & 450 \\
885 parabolic\_fem & gmres / ilu & 1009.94 & 7573 & 401.52 & 2970 \\
886 epb3 & fgmres / sor & 8.67 & 600 & 8.21 & 540 \\
887 atmosmodj & fgmres / sor & 104.23 & 451 & 88.97 & 366 \\
888 bfwa398 & gmres / none & 1.42 & 9612 & 0.28 & 1650 \\
889 torso3 & fgmres / sor & 37.70 & 565 & 34.97 & 510 \\
893 \caption{Comparison of (F)GMRES and TSIRM with (F)GMRES in sequential with some matrices, time is expressed in seconds.}
902 In order to perform larger experiments, we have tested some example applications
903 of PETSc. Those applications are available in the ksp part which is suited for
904 scalable linear equations solvers:
906 \item ex15 is an example which solves in parallel an operator using a finite
907 difference scheme. The diagonal is equal to 4 and 4 extra-diagonals
908 representing the neighbors in each directions are equal to -1. This example is
909 used in many physical phenomena, for example, heat and fluid flow, wave
911 \item ex54 is another example based on 2D problem discretized with quadrilateral
912 finite elements. For this example, the user can define the scaling of material
913 coefficient in embedded circle called $\alpha$.
915 For more technical details on these applications, interested readers are invited
916 to read the codes available in the PETSc sources. Those problems have been
917 chosen because they are scalable with many cores which is not the case of other
918 problems that we have tested.
920 In the following larger experiments are described on two large scale
921 architectures: Curie and Juqeen. Both these architectures are supercomputer
922 composed of 80,640 cores for Curie and 458,752 cores for Juqueen. Those machines
923 are respectively hosted by GENCI in France and Jülich Supercomputing Centre in
924 Germany. They belongs with other similar architectures of the PRACE initiative (
925 Partnership for Advanced Computing in Europe) which aims at proposing high
926 performance supercomputing architecture to enhance research in Europe. The Curie
927 architecture is composed of Intel E5-2680 processors at 2.7 GHz with 2Gb memory
928 by core. The Juqueen architecture is composed of IBM PowerPC A2 at 1.6 GHz with
929 1Gb memory per core. Both those architecture are equiped with a dedicated high
934 {\bf Description of preconditioners}\\
938 \begin{tabular}{|r|r|r|r|r|r|r|r|r|}
941 nb. cores & precond & \multicolumn{2}{c|}{FGMRES} & \multicolumn{2}{c|}{TSIRM CGLS} & \multicolumn{2}{c|}{TSIRM LSQR} & best gain \\
943 & & Time & \# Iter. & Time & \# Iter. & Time & \# Iter. & \\\hline \hline
944 2,048 & mg & 403.49 & 18,210 & 73.89 & 3,060 & 77.84 & 3,270 & 5.46 \\
945 2,048 & sor & 745.37 & 57,060 & 87.31 & 6,150 & 104.21 & 7,230 & 8.53 \\
946 4,096 & mg & 562.25 & 25,170 & 97.23 & 3,990 & 89.71 & 3,630 & 6.27 \\
947 4,096 & sor & 912.12 & 70,194 & 145.57 & 9,750 & 168.97 & 10,980 & 6.26 \\
948 8,192 & mg & 917.02 & 40,290 & 148.81 & 5,730 & 143.03 & 5,280 & 6.41 \\
949 8,192 & sor & 1,404.53 & 106,530 & 212.55 & 12,990 & 180.97 & 10,470 & 7.76 \\
950 16,384 & mg & 1,430.56 & 63,930 & 237.17 & 8,310 & 244.26 & 7,950 & 6.03 \\
951 16,384 & sor & 2,852.14 & 216,240 & 418.46 & 21,690 & 505.26 & 23,970 & 6.82 \\
955 \caption{Comparison of FGMRES and TSIRM with FGMRES for example ex15 of PETSc with two preconditioners (mg and sor) with 25,000 components per core on Juqueen (threshold 1e-3, restart=30, s=12), time is expressed in seconds.}
960 Table~\ref{tab:03} shows the execution times and the number of iterations of
961 example ex15 of PETSc on the Juqueen architecture. Different numbers of cores
962 are studied ranging from 2,048 up-to 16,383. Two preconditioners have been
963 tested: {\it mg} and {\it sor}. For those experiments, the number of components (or unknowns of the
964 problems) per core is fixed to 25,000, also called weak scaling. This
965 number can seem relatively small. In fact, for some applications that need a lot
966 of memory, the number of components per processor requires sometimes to be
971 In Table~\ref{tab:03}, we can notice that TSIRM is always faster than FGMRES. The last
972 column shows the ratio between FGMRES and the best version of TSIRM according to
973 the minimization procedure: CGLS or LSQR. Even if we have computed the worst
974 case between CGLS and LSQR, it is clear that TSIRM is always faster than
975 FGMRES. For this example, the multigrid preconditioner is faster than SOR. The
976 gain between TSIRM and FGMRES is more or less similar for the two
977 preconditioners. Looking at the number of iterations to reach the convergence,
978 it is obvious that TSIRM allows the reduction of the number of iterations. It
979 should be noticed that for TSIRM, in those experiments, only the iterations of
980 the Krylov solver are taken into account. Iterations of CGLS or LSQR were not
981 recorded but they are time-consuming. In general each $max\_iter_{kryl}*s$ which
982 corresponds to 30*12, there are $max\_iter_{ls}$ which corresponds to 15.
986 \includegraphics[width=0.45\textwidth]{nb_iter_sec_ex15_juqueen}
987 \caption{Number of iterations per second with ex15 and the same parameters than in Table~\ref{tab:03} (weak scaling)}
992 In Figure~\ref{fig:01}, the number of iterations per second corresponding to
993 Table~\ref{tab:03} is displayed. It can be noticed that the number of
994 iterations per second of FMGRES is constant whereas it decreases with TSIRM with
995 both preconditioners. This can be explained by the fact that when the number of
996 cores increases the time for the least-squares minimization step also increases but, generally,
997 when the number of cores increases, the number of iterations to reach the
998 threshold also increases, and, in that case, TSIRM is more efficient to reduce
999 the number of iterations. So, the overall benefit of using TSIRM is interesting.
1006 \begin{table*}[htbp]
1008 \begin{tabular}{|r|r|r|r|r|r|r|r|r|}
1011 nb. cores & threshold & \multicolumn{2}{c|}{FGMRES} & \multicolumn{2}{c|}{TSIRM CGLS} & \multicolumn{2}{c|}{TSIRM LSQR} & best gain \\
1013 & & Time & \# Iter. & Time & \# Iter. & Time & \# Iter. & \\\hline \hline
1014 2,048 & 8e-5 & 108.88 & 16,560 & 23.06 & 3,630 & 22.79 & 3,630 & 4.77 \\
1015 2,048 & 6e-5 & 194.01 & 30,270 & 35.50 & 5,430 & 27.74 & 4,350 & 6.99 \\
1016 4,096 & 7e-5 & 160.59 & 22,530 & 35.15 & 5,130 & 29.21 & 4,350 & 5.49 \\
1017 4,096 & 6e-5 & 249.27 & 35,520 & 52.13 & 7,950 & 39.24 & 5,790 & 6.35 \\
1018 8,192 & 6e-5 & 149.54 & 17,280 & 28.68 & 3,810 & 29.05 & 3,990 & 5.21 \\
1019 8,192 & 5e-5 & 785.04 & 109,590 & 76.07 & 10,470 & 69.42 & 9,030 & 11.30 \\
1020 16,384 & 4e-5 & 718.61 & 86,400 & 98.98 & 10,830 & 131.86 & 14,790 & 7.26 \\
1024 \caption{Comparison of FGMRES and TSIRM with FGMRES algorithms for ex54 of Petsc (both with the MG preconditioner) with 25,000 components per core on Curie (restart=30, s=12), time is expressed in seconds.}
1030 In Table~\ref{tab:04}, some experiments with example ex54 on the Curie architecture are reported.
1033 \begin{table*}[htbp]
1035 \begin{tabular}{|r|r|r|r|r|r|r|r|r|r|r|}
1038 nb. cores & \multicolumn{2}{c|}{FGMRES} & \multicolumn{2}{c|}{TSIRM CGLS} & \multicolumn{2}{c|}{TSIRM LSQR} & best gain & \multicolumn{3}{c|}{efficiency} \\
1039 \cline{2-7} \cline{9-11}
1040 & Time & \# Iter. & Time & \# Iter. & Time & \# Iter. & & FGMRES & TS CGLS & TS LSQR\\\hline \hline
1041 512 & 3,969.69 & 33,120 & 709.57 & 5,790 & 622.76 & 5,070 & 6.37 & 1 & 1 & 1 \\
1042 1024 & 1,530.06 & 25,860 & 290.95 & 4,830 & 307.71 & 5,070 & 5.25 & 1.30 & 1.21 & 1.01 \\
1043 2048 & 919.62 & 31,470 & 237.52 & 8,040 & 194.22 & 6,510 & 4.73 & 1.08 & .75 & .80\\
1044 4096 & 405.60 & 28,380 & 111.67 & 7,590 & 91.72 & 6,510 & 4.42 & 1.22 & .79 & .84 \\
1045 8192 & 785.04 & 109,590 & 76.07 & 10,470 & 69.42 & 9,030 & 11.30 & .32 & .58 & .56 \\
1050 \caption{Comparison of FGMRES and TSIRM with FGMRES for ex54 of Petsc (both with the MG preconditioner) with 204,919,225 components on Curie with different number of cores (restart=30, s=12, threshold 5e-5), time is expressed in seconds.}
1055 \begin{figure}[htbp]
1057 \includegraphics[width=0.45\textwidth]{nb_iter_sec_ex54_curie}
1058 \caption{Number of iterations per second with ex54 and the same parameters than in Table~\ref{tab:05} (strong scaling)}
1062 %%%*********************************************************
1063 %%%*********************************************************
1067 %%%*********************************************************
1068 %%%*********************************************************
1069 \section{Conclusion}
1071 %The conclusion goes here. this is more of the conclusion
1072 %%%*********************************************************
1073 %%%*********************************************************
1075 A novel two-stage iterative algorithm has been proposed in this article,
1076 in order to accelerate the convergence Krylov iterative methods.
1077 Our TSIRM proposal acts as a merger between Krylov based solvers and
1078 a least-squares minimization step.
1079 The convergence of the method has been proven in some situations, while
1080 experiments up to 16,394 cores have been led to verify that TSIRM runs
1081 5 or 7 times faster than GMRES.
1084 For future work, the authors' intention is to investigate
1085 other kinds of matrices, problems, and inner solvers. The
1086 influence of all parameters must be tested too, while
1087 other methods to minimize the residuals must be regarded.
1088 The number of outer iterations to minimize should become
1089 adaptative to improve the overall performances of the proposal.
1090 Finally, this solver will be implemented inside PETSc.
1093 % conference papers do not normally have an appendix
1097 % use section* for acknowledgement
1098 %%%*********************************************************
1099 %%%*********************************************************
1100 \section*{Acknowledgment}
1101 This paper is partially funded by the Labex ACTION program (contract
1102 ANR-11-LABX-01-01). We acknowledge PRACE for awarding us access to resources
1103 Curie and Juqueen respectively based in France and Germany.
1107 % trigger a \newpage just before the given reference
1108 % number - used to balance the columns on the last page
1109 % adjust value as needed - may need to be readjusted if
1110 % the document is modified later
1111 %\IEEEtriggeratref{8}
1112 % The "triggered" command can be changed if desired:
1113 %\IEEEtriggercmd{\enlargethispage{-5in}}
1115 % references section
1117 % can use a bibliography generated by BibTeX as a .bbl file
1118 % BibTeX documentation can be easily obtained at:
1119 % http://www.ctan.org/tex-archive/biblio/bibtex/contrib/doc/
1120 % The IEEEtran BibTeX style support page is at:
1121 % http://www.michaelshell.org/tex/ieeetran/bibtex/
1122 \bibliographystyle{IEEEtran}
1123 % argument is your BibTeX string definitions and bibliography database(s)
1124 \bibliography{biblio}
1126 % <OR> manually copy in the resultant .bbl file
1127 % set second argument of \begin to the number of references
1128 % (used to reserve space for the reference number labels box)
1129 %% \begin{thebibliography}{1}
1131 %% \bibitem{saad86} Y.~Saad and M.~H.~Schultz, \emph{GMRES: A Generalized Minimal Residual Algorithm for Solving Nonsymmetric Linear Systems}, SIAM Journal on Scientific and Statistical Computing, 7(3):856--869, 1986.
1133 %% \bibitem{saad96} Y.~Saad, \emph{Iterative Methods for Sparse Linear Systems}, PWS Publishing, New York, 1996.
1135 %% \bibitem{hestenes52} M.~R.~Hestenes and E.~Stiefel, \emph{Methods of conjugate gradients for solving linear system}, Journal of Research of National Bureau of Standards, B49:409--436, 1952.
1137 %% \bibitem{paige82} C.~C.~Paige and A.~M.~Saunders, \emph{LSQR: An Algorithm for Sparse Linear Equations and Sparse Least Squares}, ACM Trans. Math. Softw. 8(1):43--71, 1982.
1138 %% \end{thebibliography}