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24 \title{A scalable multisplitting algorithm to solve large sparse linear systems}
27 \author[1]{Raphaël Couturier}
28 \author[2]{ Lilia Ziane Khodja}
29 \affil[1]{ Femto-ST Institute\\
30 University of Franche Comte\\
32 email: raphael.couturier@univ-fcomte.fr}
33 \affil[2]{Inria Bordeaux Sud-Ouest\\
35 email: lilia.ziane@inria.fr}
42 %%%%%%%%%%%%%%%%%%%%%%%%
43 %%%%%%%%%%%%%%%%%%%%%%%%
46 In this paper we revisit the Krylov multisplitting algorithm presented in
47 \cite{huang1993krylov} which uses a sequential method to minimize the Krylov
48 iterations computed by a multisplitting algorithm. Our new algorithm is based on
49 a parallel multisplitting algorithm with few blocks of large size using a
50 parallel GMRES method inside each block and on a parallel Krylov minimization in
51 order to improve the convergence. Some large scale experiments with a 3D Poisson
52 problem are presented with up to 8,192 cores. They show the obtained
53 improvements compared to a classical GMRES both in terms of number of iterations
54 and in terms of execution times.
57 %%%%%%%%%%%%%%%%%%%%%%%%
58 %%%%%%%%%%%%%%%%%%%%%%%%
60 \section{Introduction}
61 Iterative methods are used to solve large sparse linear systems of equations of
62 the form $Ax=b$ because they are easier to parallelize than direct ones. Many
63 iterative methods have been proposed and adapted by different researchers. For
64 example, the GMRES method and the Conjugate Gradient method are very well known
65 and used~\cite{S96}. Both methods are based on the
66 Krylov subspace which consists in forming a basis of a sequence of successive
67 matrix powers times the initial residual.
69 When solving large linear systems with many cores, iterative methods often
70 suffer from scalability problems. This is due to their need for collective
71 communications to perform matrix-vector products and reduction operations.
72 Preconditioners can be used in order to increase the convergence of iterative
73 solvers. However, most of the good preconditioners are not scalable when
74 thousands of cores are used.
76 %Traditional iterative solvers have global synchronizations that penalize the
77 %scalability. Two possible solutions consists either in using asynchronous
78 %iterative methods~\cite{ref18} or to use multisplitting algorithms. In this
79 %paper, we will reconsider the use of a multisplitting method. In opposition to
80 %traditional multisplitting method that suffer from slow convergence, as
81 %proposed in~\cite{huang1993krylov}, the use of a minimization process can
82 %drastically improve the convergence.
84 Traditional parallel iterative solvers are based on fine-grain computations that
85 frequently require data exchanges between computing nodes and have global
86 synchronizations that penalize the scalability. Particularly, they are more
87 penalized on large scale architectures or on distributed platforms composed of
88 distant clusters interconnected by a high-latency network. It is therefore
89 imperative to develop coarse-grain based algorithms to reduce the communications
90 in the parallel iterative solvers. Two possible solutions consists either in
91 using asynchronous iterative methods~\cite{ref18} or in using multisplitting
92 algorithmss. In this paper, we will reconsider the use of a multisplitting
93 method. In opposition to traditional multisplitting method that suffer from slow
94 convergence, as proposed in~\cite{huang1993krylov}, the use of a minimization
95 process can drastically improve the convergence.
98 %%% AJOUTE************************
99 %%%*******************************
100 In this work we develop a new parallel two-stage algorithm for large-scale clusters. Our objective is to mix between Krylov based iterative methods and the multisplitting method to improve the scalability. In fact Krylov subspace methods are well-known for their good convergence compared to others iterative methods. So our main contribution is to use the multisplitting method which splits the problem to solve into different blocks in order to reduce the large amount of communications and, to implement both inner and outer iterations as Krylov subspace iterations improving the convergence of the multisplitting algorithm.
101 %%%*******************************
102 %%%*******************************
104 The present paper is organized as follows. First, Section~\ref{sec:02} presents
105 some related works and the principle of multisplitting methods. Then, in
106 Section~\ref{sec:03} the algorithm of our Krylov multisplitting
107 method, based on inner-outer iterations, is presented. Finally, in Section~\ref{sec:04}, the
108 parallel experiments on Hector architecture show the performances of the Krylov
109 multisplitting algorithm compared to the classical GMRES algorithm to solve a 3D
113 %%%%%%%%%%%%%%%%%%%%%%%%
114 %%%%%%%%%%%%%%%%%%%%%%%%
116 \section{Related works and presentation of the multisplitting method}
118 A general framework to study parallel multisplitting methods has been presented in~\cite{o1985multi}
119 by O'Leary and White. Convergence conditions are given for the
120 most general cases. Many authors have improved multisplitting algorithms by proposing,
121 for example, an asynchronous version~\cite{bru1995parallel} or convergence
122 conditions~\cite{bai1999block,bahi2000asynchronous} or other
123 two-stage algorithms~\cite{frommer1992h,bru1995parallel}.
125 In~\cite{huang1993krylov}, the authors have proposed a parallel multisplitting
126 algorithm in which all the tasks except one are devoted to solve a sub-block of
127 the splitting and to send their local solutions to the first task which is in
128 charge of combining the vectors at each iteration. These vectors form a Krylov
129 basis for which the first task minimizes the error function over the basis to
130 increase the convergence, then the other tasks receive the updated solution until the
131 convergence of the global system.
133 In~\cite{couturier2008gremlins}, the authors have developed practical implementations
134 of multisplitting algorithms to solve large scale linear systems. Inner solvers
135 could be based on sequential direct method with the LU method or sequential iterative
138 In~\cite{prace-multi}, the authors have designed a parallel multisplitting
139 algorithm in which large blocks are solved using a GMRES solver. The authors have
140 performed large scale experiments up-to 32,768 cores and they conclude that
141 an asynchronous multisplitting algorithm could be more efficient than traditional
142 solvers on an exascale architecture with hundreds of thousands of cores.
144 So, compared to these works, we propose in this paper a practical multisplitting method based on parallel iterative blocks which gives better results than classical GMRES method for the 3D Poisson problem we considered.
147 The key idea of a multisplitting method to solve a large system of linear equations $Ax=b$ is defined as follows. The first step consists in partitioning the matrix $A$ in $L$ several ways
152 where for all $\ell\in\{1,\ldots,L\}$ $M_\ell$ are non-singular matrices. Then the linear system is solved by an iteration based on the obtained splittings as follows
154 x^{k+1}=\displaystyle\sum^L_{\ell=1} E_\ell M^{-1}_\ell (N_\ell x^k + b),~k=1,2,3,\ldots
157 where $E_\ell$ are non-negative and diagonal weighting matrices and their sum is an identity matrix $I$. The convergence of such a method is dependent on the condition
159 \rho(\displaystyle\sum^L_{\ell=1}E_\ell M^{-1}_\ell N_\ell)<1.
162 where $\rho$ is the spectral radius of the square matrix.
164 The advantage of the multisplitting method is that at each iteration $k$ there are $L$ different linear sub-systems
166 v_\ell^k=M^{-1}_\ell N_\ell x_\ell^{k-1} + M^{-1}_\ell b,~\ell\in\{1,\ldots,L\},
169 to be solved independently by a direct or an iterative method, where $v_\ell$ is the solution of the local sub-system. Thus the computations of $\{v_\ell\}_{1\leq \ell\leq L}$ may be performed in parallel by a set of processors. A multisplitting method using an iterative method as an inner solver is called an inner-outer iterative method or a two-stage method. The results $v_\ell$ obtained from the different splittings~(\ref{eq04}) are combined to compute solution $x$ of the linear system by using the diagonal weighting matrices
171 x^k = \displaystyle\sum^L_{\ell=1} E_\ell v_\ell^k,
174 In the case where the diagonal weighting matrices $E_\ell$ have only zero and one factors (i.e. $v_\ell$ are disjoint vectors), the multisplitting method is non-overlapping and corresponds to the block Jacobi method.
176 %%%%%%%%%%%%%%%%%%%%%%%%
177 %%%%%%%%%%%%%%%%%%%%%%%%
179 \section{A two-stage method with a minimization}
182 %%% MODIFIE ************************
183 %%%*********************************
184 Let $Ax=b$ be a given large and sparse linear system of $n$ equations where $A\in\mathbb{R}^{n\times n}$ is a sparse square and non-singular matrix, $x\in\mathbb{R}^{n}$ is the solution vector and $b\in\mathbb{R}^{n}$ is the right-hand side vector. We use a multisplitting method to solve the linear system on a large computing platform in order to reduce the communications. Let the computing platform be composed of $L$ clusters of processors physically adjacent or geographically distant. In this work we apply the block Jacobi multisplitting to the linear system as follows
185 %%%*********************************
186 %%%*********************************
192 A & = & [A_{1}, \ldots, A_{L}]\\
193 x & = & [X_{1}, \ldots, X_{L}]\\
194 b & = & [B_{1}, \ldots, B_{L}]
199 where for $\ell\in\{1,\ldots,L\}$, $A_\ell$ is a rectangular block of size $n_\ell\times n$ and $X_\ell$ and $B_\ell$ are sub-vectors of size $n_\ell$ each, such that $\sum_\ell n_\ell=n$.
200 %%% MODIFIE ***********************
201 %%%********************************
202 The splitting is performed row-by-row without overlapping in such a way that successive rows of sparse matrix $A$ and both vectors $x$ and $b$ are assigned to one cluster.
203 %%%********************************
204 %%%********************************
205 So, the multisplitting format of the linear system is defined as follows
207 \forall \ell\in\{1,\ldots,L\} \mbox{,~} A_{\ell \ell}X_\ell + \displaystyle\sum_{\substack{m=1\\m\neq\ell}}^L A_{\ell m}X_m = B_\ell,
210 where $A_{\ell m}$ is a sub-block of size $n_\ell\times n_m$ of the rectangular matrix $A_\ell$, $X_m\neq X_\ell$ is a sub-vector of size $n_m$ of the solution vector $x$ and $\sum_{m\neq \ell}n_m+n_\ell=n$, for all $m\in\{1,\ldots,L\}$.
212 Our multisplitting method proceeds by iteration to solve the linear system in such a way that each sub-system
216 A_{\ell \ell}X_\ell = Y_\ell \mbox{,~such that}\\
217 Y_\ell = B_\ell - \displaystyle\sum_{\substack{m=1\\m\neq \ell}}^{L}A_{\ell m}X_m,
222 is solved independently by a {\it cluster of processors} and communications are required to update the right-hand side vectors $Y_\ell$, such that the vectors $X_m$ represent the data dependencies between the clusters. In this work, we use the parallel restarted GMRES method~\cite{ref34} as an inner iteration method to solve sub-systems~(\ref{sec03:eq03}).
223 %%% MODIFIE ***********************
224 %%%********************************
225 GMRES is one of the most used Krylov iterative methods to solve sparse linear systems by minimizing the residuals over an orthonormal basis of a Krylov subspace.
226 %%%********************************
227 %%%********************************
228 %In practice, GMRES is used with a preconditioner to improve its convergence. In this work, we used a preconditioning matrix equivalent to the main diagonal of sparse sub-matrix $A_{ll}$. This preconditioner is straightforward to implement in parallel and gives good performances in many situations.
230 It should be noted that the convergence of the inner iterative solver for the
231 different sub-systems~(\ref{sec03:eq03}) does not necessarily involve the
232 convergence of the multisplitting algorithm. It strongly depends on the properties
233 of the global sparse linear system to be
234 solved~\cite{o1985multi,ref18}. Furthermore, the splitting of the linear system
235 among several clusters of processors increases the spectral radius of the
236 iteration matrix, thereby slowing the convergence. In fact, the larger the
237 number of splitting is, the larger the spectral radius is. In this paper, our
238 work is based on the work presented in~\cite{huang1993krylov} to increase the
239 convergence and improve the scalability of the multisplitting methods.
241 %%% AJOUTE ************************
242 %%%********************************
243 Krylov subspace methods are well-known for their good convergence compared to other iterative methods.
244 %%%********************************
245 %%%********************************
246 In order to accelerate the convergence, we implemented the outer iteration of our multisplitting solver as a Krylov iterative method which minimizes some error function over a Krylov subspace~\cite{S96}. The Krylov subspace that we used is spanned by a basis composed of successive solutions issued from solving the $L$ splittings~(\ref{sec03:eq03})
248 S=\{x^1,x^2,\ldots,x^s\},~s\leq n,
251 where for $j\in\{1,\ldots,s\}$, $x^j=[X_1^j,\ldots,X_L^j]$ is a solution of the global linear system.
252 %%% MODIFIE ***********************
253 %%%********************************
254 The advantage of such a Krylov subspace is that we neither need an orthonormal basis nor any synchronization between clusters is necessary to orthogonalize the generated basis. This avoids to perform other synchronizations between the blocks of processors.
255 %%%********************************
256 %%%********************************
258 The multisplitting method is periodically restarted every $s$ iterations with a new initial guess $\tilde{x}=S\alpha$ which minimizes the error function $\|b-Ax\|_2$ over the Krylov subspace spanned by vectors of $S$. So $\alpha$ is defined as the solution of the large overdetermined linear system
263 where $R=AS$ is a dense rectangular matrix of size $n\times s$ and $s\ll n$. This leads us to solve a system of normal equations
268 which is associated with the least squares problem
270 \text{minimize}~\|b-R\alpha\|_2,
273 where $R^T$ denotes the transpose of matrix $R$. Since $R$ (i.e. $AS$) and $b$ are split among $L$ clusters, the symmetric positive definite system~(\ref{sec03:eq06}) is solved in parallel. Thus an iterative method would be more appropriate than a direct one to solve this system. We use the parallel Conjugate Gradient method for the normal equations CGNR~\cite{S96,refCGNR}.
275 \begin{algorithm}[!t]
276 \caption{A two-stage linear solver with inner iteration GMRES method}
277 \begin{algorithmic}[1]
278 \Input $A_\ell$ (sparse sub-matrix), $B_\ell$ (right-hand side sub-vector)
279 \Output $X_\ell$ (solution sub-vector)\vspace{0.2cm}
280 \State Load $A_\ell$, $B_\ell$
281 \State Set the initial guess $x^0$
282 \State Set the minimizer $\tilde{x}^0=x^0$
283 \For {$k=1,2,3,\ldots$ until the global convergence}
284 \State Restart with $x^0=\tilde{x}^{k-1}$:
285 \For {$j=1,2,\ldots,s$}
286 \State \label{line7}Inner iteration solver: \Call{InnerSolver}{$x^0$, $j$}
287 \State Construct basis $S$: add column vector $X_\ell^j$ to the matrix $S_\ell^k$
288 \State Exchange local values of $X_\ell^j$ with the neighboring clusters
289 \State Compute dense matrix $R$: $R_\ell^{k,j}=\sum^L_{i=1}A_{\ell i}X_i^j$
291 \State \label{line12}Minimization $\|b-R\alpha\|_2$: \Call{UpdateMinimizer}{$S_\ell$, $R$, $b$, $k$}
292 \State Local solution of linear system $Ax=b$: $X_\ell^k=\tilde{X}_\ell^k$
293 \State Exchange the local minimizer $\tilde{X}_\ell^k$ with the neighboring clusters
298 \Function {InnerSolver}{$x^0$, $j$}
299 \State Compute local right-hand side $Y_\ell = B_\ell - \sum^L_{\substack{m=1\\m\neq \ell}}A_{\ell m}X_m^0$
300 \State Solving local splitting $A_{\ell \ell}X_\ell^j=Y_\ell$ using parallel GMRES method, such that $X_\ell^0$ is the initial guess
301 \State \Return $X_\ell^j$
306 \Function {UpdateMinimizer}{$S_\ell$, $R$, $b$, $k$}
307 \State Solving normal equations $(R^k)^TR^k\alpha^k=(R^k)^Tb$ in parallel by $L$ clusters using parallel CGNR method
308 \State Compute local minimizer $\tilde{X}_\ell^k=S_\ell^k\alpha^k$
309 \State \Return $\tilde{X}_\ell^k$
315 The main key points of our Krylov multisplitting method to solve a large sparse linear system are given in Algorithm~\ref{algo:01}. This algorithm is based on a two-stage method with a minimization using restarted GMRES iterative method as an inner solver. It is executed in parallel by each cluster of processors. Matrices and vectors with the subscript $\ell$ represent the local data for cluster $\ell$, where $\ell\in\{1,\ldots,L\}$. The two-stage solver uses two different parallel iterative algorithms: the GMRES method to solve each splitting~(\ref{sec03:eq03}) on a cluster of processors, and the CGNR method, executed periodically in parallel by all clusters to minimize the function error~(\ref{sec03:eq07}) over the Krylov subspace spanned by $S$. The algorithm requires two global synchronizations between $L$ clusters. The first one is performed line~\ref{line12} in Algorithm~\ref{algo:01} to exchange local values of vector solution $x$ (i.e. the minimizer $\tilde{x}$) required to restart the multisplitting solver. The second one is needed to construct the matrix $R$. We chose to perform this latter synchronization $s$ times in every outer iteration $k$ (line~\ref{line7} in Algorithm~\ref{algo:01}). This is a straightforward way to compute the sparse matrix-dense matrix multiplication $R=AS$. We implemented all synchronizations by using message passing collective communications of MPI library.
317 %%%%%%%%%%%%%%%%%%%%%%%%
318 %%%%%%%%%%%%%%%%%%%%%%%%
320 \section{Experiments}
322 In order to illustrate the interest of our algorithm, we have compared our
323 algorithm with the GMRES method which is a commonly used method in many
324 situations. We have chosen to focus on only one problem which is very simple to
325 implement: a 3 dimension Poisson problem.
330 \nabla u&=f \mbox{~in~} \omega\\
331 u &=0 \mbox{~on~} \Gamma=\partial \omega
336 After discretization, with a finite difference scheme, a seven point stencil is
337 used. It is well-known that the spectral radius of matrices representing such
338 problems are very close to 1. Moreover, the larger the number of discretization
339 points is, the closer to 1 the spectral radius is. Hence, to solve a matrix
340 obtained for a 3D Poisson problem, the number of iterations is high. Using a
341 preconditioner it is possible to reduce the number of iterations but
342 preconditioners are not scalable when using many cores.
344 %Doing many experiments with many cores is not easy and requires to access to a supercomputer with several hours for developing a code and then improving it.
345 In the following we present some experiments we could achieve out on the Hector
346 architecture, a UK's high-end computing resource, funded by the UK Research
347 Councils~\cite{hector}. This is a Cray XE6 supercomputer, equipped with two
348 16-core AMD Opteron 2.3 Ghz and 32 GB of memory. Machines are interconnected
351 Table~\ref{tab1} shows the result of the experiments. The first column shows
352 the size of the 3D Poisson problem. The size is chosen in order to have
353 approximately 50,000 components per core. The second column represents the
354 number of cores used. In brackets, one can find the decomposition used for the
355 Krylov multisplitting. The third column and the sixth column respectively show
356 the execution time for the GMRES and the Krylov multisplitting codes. The fourth
357 and the seventh column describe the number of iterations. For the
358 multisplitting code, the total number of inner iterations is represented in
359 brackets. For the GMRES code (alone and in the multisplitting version) the
360 restart parameter is fixed to 16. The precision of the GMRES version is fixed to
361 1e-6. For the multisplitting, there are two precisions, one for the external
362 solver which is fixed to 1e-6 and another one for the inner solver (GMRES) which
363 is fixed to 1e-10. It should be noted that a high precision is used but we also
364 fixed a maximum number of iterations for each internal step. In practice, we
365 limit the number of iterations in the internal step to 10. So an internal iteration is finished
366 when the precision is reached or when the maximum internal number of iterations
367 is reached. The precision and the maximum number of iterations of CGNR method are fixed to 1e-25 and 20 respectively. The size of the Krylov subspace basis $S$ is fixed to 10 vectors.
371 \begin{changemargin}{-1.8cm}{0cm}
373 \begin{tabular}{|c|c||c|c|c||c|c|c||c|}
375 \multirow{2}{*}{Pb size}&\multirow{2}{*}{Nb. cores} & \multicolumn{3}{c||}{GMRES} & \multicolumn{3}{c||}{Krylov Multisplitting} & \multirow{2}{*}{Ratio}\\
377 & & Time (s) & nb Iter. & $\Delta$ & Time (s)& nb Iter. & $\Delta$ & \\
379 $468^3$ & 2,048 (2x1,024) & 299.7 & 41,028 & 5.02e-8 & 48.4 & 691(6,146) & 8.24e-08 & 6.19 \\
381 $590^3$ & 4,096 (2x2,048) & 433.1 & 55,494 & 4.92e-7 & 74.1 & 1,101(8,211) & 6.62e-08 & 5.84 \\
383 $743^3$ & 8,192 (2x4,096) & 704.4 & 87,822 & 4.80e-07 & 151.2 & 3,061(14,914) & 5.87e-08 & 4.65 \\
385 $743^3$ & 8,192 (4x2,048) & 704.4 & 87,822 & 4.80e-07 & 110.3 & 1,531(12,721) & 1.47e-07& 6.39 \\
397 From these experiments, it can be observed that the multisplitting version is
398 always faster than the GMRES version. The acceleration gain of the
399 multisplitting version ranges between 4 and 6. It can be noticed that the number of
400 iterations is drastically reduced with the multisplitting version even it is not
401 negligible. Moreover, with 8,192 cores, we can see that using 4 clusters gives a
402 better performance than simply using 2 clusters. In fact, we can notice that the
403 precision with 2 clusters is slightly better but in both cases the precision is
404 under the specified threshold.
406 \section{Conclusion and perspectives}
407 We have implemented a Krylov multisplitting method to solve sparse linear
408 systems on large-scale computing platforms. We have developed a synchronous
409 two-stage method based on the block Jacobi multisplitting which uses GMRES
410 iterative method as an inner iteration. Our contribution in this paper is
411 twofold. First we provide a multi cluster decomposition that allows us to choose
412 the appropriate size of the clusters according to the architecures of the
413 supercomputer. Second, we have implemented the outer iteration of the
414 multisplitting method as a Krylov subspace method which minimizes some error
415 function. This increases the convergence and improves the scalability of the
416 multisplitting method.
418 We have tested our multisplitting method to solve the sparse linear system
419 issued from the discretization of a 3D Poisson problem. We have compared its
420 performances to the classical GMRES method on a supercomputer composed of 2,048
421 to 8,192 cores. The experimental results showed that the multisplitting method is
422 about 4 to 6 times faster than the GMRES method for different sizes of the
423 problem split into 2 or 4 blocks when using the multisplitting method. Indeed, the
424 GMRES method has difficulties to scale with many cores while the Krylov
425 multisplitting method allows to hide latency and reduce the inter-cluster
428 In future works, we plan to conduct experiments on larger numbers of cores and
429 test the scalability of our Krylov multisplitting method. It would be
430 interesting to validate its performances to solve other linear/nonlinear and
431 symmetric/nonsymmetric problems. Moreover, we intend to develop multisplitting
432 methods based on asynchronous iterations in which communications are overlapped
433 by computations. These methods would be interesting for platforms composed of
434 distant clusters interconnected by a high-latency network. In addition, we
435 intend to investigate the convergence improvements of our method by using
436 preconditioning techniques for Krylov iterative methods and multisplitting
437 methods with overlapping blocks.
439 \section{Acknowledgement}
440 The authors would like to thank Mark Bull of the EPCC his fruitful remarks and the facilities of HECToR.
442 %Other applications (=> other matrices)\\
443 %Larger experiments\\
449 %%%%%%%%%%%%%%%%%%%%%%%%
450 %%%%%%%%%%%%%%%%%%%%%%%%
452 \bibliographystyle{plain}
453 \bibliography{biblio}
