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16 \title{A scalable multisplitting algorithm for solving large sparse linear systems}
21 \author{Raphaël Couturier \and Lilia Ziane Khodja}
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31 In this paper we revist the krylov multisplitting algorithm presented in
32 \cite{huang1993krylov} which uses a scalar method to minimize the krylov
33 iterations computed by a multisplitting algorithm. Our new algorithm is based on
34 a parallel multisplitting algorithm with few blocks of large size using a
35 parallel GMRES method inside each block and on a parallel krylov minimization in
36 order to improve the convergence. Some large scale experiments with a 3D Poisson
37 problem are presented. They show the obtained improvements compared to a
38 classical GMRES both in terms of number of iterations and execution times.
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46 \section{Introduction}
48 Iterative methods are used to solve large sparse linear systems of equations of
49 the form $Ax=b$ because they are easier to parallelize than direct ones. Many
50 iterative methods have been proposed and adapted by many researchers. For
51 example, the GMRES method and the Conjugate Gradient method are very well known
52 and used by many researchers ~\cite{S96}. Both the method are based on the
53 Krylov subspace which consists in forming a basis of the sequence of successive
54 matrix powers times the initial residual.
56 When solving large linear systems with many cores, iterative methods often
57 suffer from scalability problems. This is due to their need for collective
58 communications to perform matrix-vector products and reduction operations.
59 Preconditionners can be used in order to increase the convergence of iterative
60 solvers. However, most of the good preconditionners are not sclalable when
61 thousands of cores are used.
65 On ne peut pas parler de tout...\\
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73 The key idea of the multisplitting method for solving a large system
74 of linear equations $Ax=b$ consists in partitioning the matrix $A$ in
77 A = M_l - N_l,~l\in\{1,\ldots,L\},
80 where $M_l$ are nonsingular matrices. Then the linear system is solved
81 by iteration based on the multisplittings as follows
83 x^{k+1}=\displaystyle\sum^L_{l=1} E_l M^{-1}_l (N_l x^k + b),~k=1,2,3,\ldots
86 where $E_l$ are non-negative and diagonal weighting matrices such that
87 $\sum^L_{l=1}E_l=I$ ($I$ is an identity matrix). Thus the convergence
88 of such a method is dependent on the condition
90 \rho(\displaystyle\sum^L_{l=1}E_l M^{-1}_l N_l)<1.
94 The advantage of the multisplitting method is that at each iteration
95 $k$ there are $L$ different linear sub-systems
97 v_l^k=M^{-1}_l N_l x_l^{k-1} + M^{-1}_l b,~l\in\{1,\ldots,L\},
100 to be solved independently by a direct or an iterative method, where
101 $v_l^k$ is the solution of the local sub-system. Thus, the
102 calculations of $v_l^k$ may be performed in parallel by a set of
103 processors. A multisplitting method using an iterative method for
104 solving the $L$ linear sub-systems is called an inner-outer iterative
105 method or a two-stage method. The results $v_l^k$ obtained from the
106 different splittings~(\ref{eq04}) are combined to compute the solution
107 $x^k$ of the linear system by using the diagonal weighting matrices
109 x^k = \displaystyle\sum^L_{l=1} E_l v_l^k,
112 In the case where the diagonal weighting matrices $E_l$ have only zero
113 and one factors (i.e. $v_l^k$ are disjoint vectors), the
114 multisplitting method is non-overlapping and corresponds to the block
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120 \section{Related works}
123 A general framework for studying parallel multisplitting has been presented in
124 \cite{o1985multi} by O'Leary and White. Convergence conditions are given for the
125 most general case. Many authors improved multisplitting algorithms by proposing
126 for example an asynchronous version \cite{bru1995parallel} and convergence
127 conditions \cite{bai1999block,bahi2000asynchronous} in this case or other
128 two-stage algorithms~\cite{frommer1992h,bru1995parallel}.
130 In \cite{huang1993krylov}, the authors proposed a parallel multisplitting
131 algorithm in which all the tasks except one are devoted to solve a sub-block of
132 the splitting and to send their local solution to the first task which is in
133 charge to combine the vectors at each iteration. These vectors form a Krylov
134 basis for which the first task minimizes the error function over the basis to
135 increase the convergence, then the other tasks receive the update solution until
136 convergence of the global system.
140 In \cite{couturier2008gremlins}, the authors proposed practical implementations
141 of multisplitting algorithms that take benefit from multisplitting algorithms to
142 solve large scale linear systems. Inner solvers could be based on scalar direct
143 method with the LU method or scalar iterative one with GMRES.
145 In~\cite{prace-multi}, the authors have proposed a parallel multisplitting
146 algorithm in which large block are solved using a GMRES solver. The authors have
147 performed large scale experimentations upto 32.768 cores and they conclude that
148 asynchronous multisplitting algorithm could more efficient than traditionnal
149 solvers on exascale architecture with hunders of thousands of cores.
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156 \section{A two-stage method with a minimization}
157 Let $Ax=b$ be a given sparse and large linear system of $n$ equations
158 to solve in parallel on $L$ clusters, physically adjacent or
159 geographically distant, where $A\in\mathbb{R}^{n\times n}$ is a square
160 and nonsingular matrix, $x\in\mathbb{R}^{n}$ is the solution vector
161 and $b\in\mathbb{R}^{n}$ is the right-hand side vector. The
162 multisplitting of this linear system is defined as follows:
166 A & = & [A_{1}, \ldots, A_{L}]\\
167 x & = & [X_{1}, \ldots, X_{L}]\\
168 b & = & [B_{1}, \ldots, B_{L}]
173 where for $l\in\{1,\ldots,L\}$, $A_l$ is a rectangular block of size
174 $n_l\times n$ and $X_l$ and $B_l$ are sub-vectors of size $n_l$, such
175 that $\sum_ln_l=n$. In this case, we use a row-by-row splitting
176 without overlapping in such a way that successive rows of the sparse
177 matrix $A$ and both vectors $x$ and $b$ are assigned to one cluster.
178 So, the multisplitting format of the linear system is defined as
181 \forall l\in\{1,\ldots,L\} \mbox{,~} \displaystyle\sum_{i=1}^{l-1}A_{li}X_i + A_{ll}X_l + \displaystyle\sum_{i=l+1}^{L}A_{li}X_i = B_l,
184 where $A_{li}$ is a block of size $n_l\times n_i$ of the rectangular
185 matrix $A_l$, $X_i\neq X_l$ is a sub-vector of size $n_i$ of the
186 solution vector $x$ and $\sum_{i<l}n_i+\sum_{i>l}n_i+n_l=n$, for all
187 $i\in\{1,\ldots,l-1,l+1,\ldots,L\}$.
189 The multisplitting method proceeds by iteration for solving the linear
190 system in such a way each sub-system
194 A_{ll}X_l = Y_l \mbox{,~such that}\\
195 Y_l = B_l - \displaystyle\sum_{i=1,i\neq l}^{L}A_{li}X_i,
200 is solved independently by a cluster of processors and communication
201 are required to update the right-hand side vectors $Y_l$, such that
202 the vectors $X_i$ represent the data dependencies between the
203 clusters. In this work, we use the parallel GMRES method~\cite{ref34}
204 as an inner iteration method for solving the
205 sub-systems~(\ref{sec03:eq03}). It is a well-known iterative method
206 which gives good performances for solving sparse linear systems in
207 parallel on a cluster of processors.
209 It should be noted that the convergence of the inner iterative solver
210 for the different linear sub-systems~(\ref{sec03:eq03}) does not
211 necessarily involve the convergence of the multisplitting method. It
212 strongly depends on the properties of the sparse linear system to be
213 solved and the computing
214 environment~\cite{o1985multi,ref18}. Furthermore, the multisplitting
215 of the linear system among several clusters of processors increases
216 the spectral radius of the iteration matrix, thereby slowing the
217 convergence. In this paper, we based on the work presented
218 in~\cite{huang1993krylov} to increase the convergence and improve the
219 scalability of the multisplitting methods.
221 In order to accelerate the convergence, we implement the outer
222 iteration of the multisplitting solver as a Krylov subspace method
223 which minimizes some error function over a Krylov subspace~\cite{S96}.
224 The Krylov space of the method that we used is spanned by a basis
225 composed of successive solutions issued from solving the $L$
226 splittings~(\ref{sec03:eq03})
228 S=\{x^1,x^2,\ldots,x^s\},~s\leq n,
231 where for $j\in\{1,\ldots,s\}$, $x^j=[X_1^j,\ldots,X_L^j]$ is a
232 solution of the global linear system. The advantage of such a Krylov subspace is that we need neither an orthogonal basis nor synchronizations between the different clusters to generate this basis.
234 The multisplitting method is periodically restarted every $s$
235 iterations with a new initial guess $\tilde{x}=S\alpha$ which
236 minimizes the error function $\|b-Ax\|_2$ over the Krylov subspace
237 spanned by the vectors of $S$. So, $\alpha$ is defined as the
238 solution of the large overdetermined linear system
243 where $R=AS$ is a dense rectangular matrix of size $n\times s$ and
244 $s\ll n$. This leads us to solve the system of normal equations
249 which is associated with the least squares problem
251 \text{minimize}~\|b-R\alpha\|_2,
254 where $R^T$ denotes the transpose of the matrix $R$. Since $R$
255 (i.e. $AS$) and $b$ are split among $L$ clusters, the symmetric
256 positive definite system~(\ref{sec03:eq06}) is solved in
257 parallel. Thus, an iterative method would be more appropriate than a
258 direct one for solving this system. We use the parallel conjugate
259 gradient method for the normal equations CGNR~\cite{S96,refCGNR}.
261 \begin{algorithm}[!t]
262 \caption{A two-stage linear solver with inner iteration GMRES method}
263 \begin{algorithmic}[1]
264 \Input $A_l$ (local sparse matrix), $B_l$ (local right-hand side), $x^0$ (initial guess)
265 \Output $X_l$ (local solution vector)\vspace{0.2cm}
266 \State Load $A_l$, $B_l$, $x^0$
267 \State Initialize the minimizer $\tilde{x}^0=x^0$
268 \For {$k=1,2,3,\ldots$ until the global convergence}
269 \State Restart with $x^0=\tilde{x}^{k-1}$: \textbf{for} $j=1,2,\ldots,s$ \textbf{do}
270 \State\hspace{0.5cm} Inner iteration solver: \Call{InnerSolver}{$x^0$, $j$}
271 \State\hspace{0.5cm} Construct the basis $S$: add the column vector $X_l^j$ to the matrix $S_l^k$
272 \State\hspace{0.5cm} Exchange the local solution vector $X_l^j$ with the neighboring clusters
273 \State\hspace{0.5cm} Compute the dense matrix $R$: $R_l^{k,j}=\sum^L_{i=1}A_{li}X_i^j$
274 \State\textbf{end for}
275 \State Minimization $\|b-R\alpha\|_2$: \Call{UpdateMinimizer}{$S_l$, $R$, $b$, $k$}
276 \State Local solution of the linear system $Ax=b$: $X_l^k=\tilde{X}_l^k$
277 \State Exchange the local minimizer $\tilde{X}_l^k$ with the neighboring clusters
282 \Function {InnerSolver}{$x^0$, $j$}
283 \State Compute the local right-hand side: $Y_l = B_l - \sum^L_{i=1,i\neq l}A_{li}X_i^0$
284 \State Solving the local splitting $A_{ll}X_l^j=Y_l$ using the parallel GMRES method, such that $X_l^0$ is the initial guess
285 \State \Return $X_l^j$
290 \Function {UpdateMinimizer}{$S_l$, $R$, $b$, $k$}
291 \State Solving the normal equations $(R^k)^TR^k\alpha^k=(R^k)^Tb$ in parallel by $L$ clusters using the parallel CGNR method
292 \State Compute the local minimizer: $\tilde{X}_l^k=S_l^k\alpha^k$
293 \State \Return $\tilde{X}_l^k$
299 The main key points of the multisplitting method for solving large
300 sparse linear systems are given in Algorithm~\ref{algo:01}. This
301 algorithm is based on a two-stage method with a minimization using the
302 GMRES iterative method as an inner solver. It is executed in parallel
303 by each cluster of processors. The matrices and vectors with the
304 subscript $l$ represent the local data for the cluster $l$, where
305 $l\in\{1,\ldots,L\}$. The two-stage solver uses two different parallel
306 iterative algorithms: the GMRES method for solving each splitting on a
307 cluster of processors, and the CGNR method executed in parallel by all
308 clusters for minimizing the function error over the Krylov subspace
309 spanned by $S$. The algorithm requires two global synchronizations
310 between the $L$ clusters. The first one is performed at line~$12$ in
311 Algorithm~\ref{algo:01} to exchange the local values of the vector
312 solution $x$ (i.e. the minimizer $\tilde{x}$) required to restart the
313 multisplitting solver. The second one is needed to construct the
314 matrix $R$ of the Krylov subspace. We choose to perform this latter
315 synchronization $s$ times in every outer iteration $k$ (line~$7$ in
316 Algorithm~\ref{algo:01}). This is a straightforward way to compute the
317 matrix-matrix multiplication $R=AS$. We implement all
318 synchronizations by using the MPI collective communication
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