Document DESC%CNV method and MOLD arguments to CDASB and PREC%BUILD

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Salvatore Filippone
2017-12-14 17:09:59 +00:00
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<TITLE>General overview</TITLE>
@@ -13,7 +9,7 @@ original version by: Nikos Drakos, CBLU, University of Leeds
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<H1><A NAME="SECTION00030000000000000000"></A>
@@ -58,10 +55,10 @@ General overview
</H1>
The PSBLAS library is designed to handle the implementation of
iterative solvers for sparse linear systems on distributed memory
parallel computers. The system coefficient matrix <IMG
parallel computers. The system coefficient matrix <SPAN CLASS="MATH"><IMG
WIDTH="16" HEIGHT="14" ALIGN="BOTTOM" BORDER="0"
SRC="img1.png"
ALT="$A$"> must be square;
ALT="$A$"></SPAN> must be square;
it may be real or complex, nonsymmetric, and its sparsity pattern
needs not to be symmetric. The serial computation parts are based on
the serial sparse BLAS, so that any extension made to the data
@@ -78,10 +75,11 @@ calls to the serial sparse BLAS subroutines.
In a similar way, the inter-process message exchanges are encapsulated
in an applicaiton layer that has been strongly inspired by the Basic
Linear Algebra Communication Subroutines (BLACS) library&nbsp;[<A
HREF="node132.html#BLACS">7</A>].
HREF="node133.html#BLACS">7</A>].
Usually there is no need to deal directly with MPI; however, in some
cases, MPI routines are used directly to improve efficiency. For
further details on our communication layer see Sec.&nbsp;<A HREF="node98.html#sec:parenv">7</A>.
further details on our communication layer see Sec.&nbsp;<A HREF="node99.html#sec:parenv">7</A>.
<P>
<DIV ALIGN="CENTER"><A NAME="fig:psblas"></A><A NAME="272"></A>
@@ -118,7 +116,7 @@ mesh.
<P>
The distribution of the coefficient matrix for the linear system is
based on the ``owner computes'' rule:
based on the &ldquo;owner computes&rdquo; rule:
the variable associated to each mesh point is assigned to a process
that will own the corresponding row in the coefficient matrix and
will carry out all related computations. This allocation strategy
@@ -126,13 +124,14 @@ is equivalent to a partition of the discretization mesh into <EM>sub-domains</EM
Our library supports any distribution that keeps together
the coefficients of each matrix row; there are no other constraints on
the variable assignment.
This choice is consistent with simple data distributions such as <code>CYCLIC(N)</code> and <code>BLOCK</code>,
This choice is consistent with simple data distributions
such as <code>CYCLIC(N)</code> and <code>BLOCK</code>,
as well as completely arbitrary assignments of
equation indices to processes.
In particular it is consistent with the
usage of graph partitioning tools commonly available in the
literature, e.g. METIS&nbsp;[<A
HREF="node132.html#METIS">14</A>].
HREF="node133.html#METIS">14</A>].
Dense vectors conform to sparse
matrices, that is, the entries of a vector follow the same distribution
of the matrix rows.
@@ -143,7 +142,7 @@ process generates its own portion. We never require that the entire
matrix be available on a single node. However, it is possible
to hold the entire matrix in one process and distribute it
explicitly<A NAME="tex2html2"
HREF="footnode.html#foot201"><SUP>1</SUP></A>, even though the resulting memory
HREF="footnode.html#foot201"><SUP><SPAN CLASS="arabic">1</SPAN></SUP></A>, even though the resulting memory
bottleneck would make this option unattractive in most cases.
<P>
@@ -151,45 +150,46 @@ bottleneck would make this option unattractive in most cases.
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<LI><A NAME="tex2html225"
HREF="node4.html">Basic Nomenclature</A>
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<LI><A NAME="tex2html226"
HREF="node5.html">Library contents</A>
HREF="node4.html">Basic Nomenclature</A>
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HREF="node5.html">Library contents</A>
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HREF="node6.html">Application structure</A>
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