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author | Karl Berry <karl@freefriends.org> | 2007-01-10 22:24:14 +0000 |
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committer | Karl Berry <karl@freefriends.org> | 2007-01-10 22:24:14 +0000 |
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tree | 47882be5f5f0fe051b894d8db556833a1f05f718 /Master/texmf-dist/tex/plain/siam/pexample.tex | |
parent | de0d34e2013ef10d645ab355c2a7f53510fc171c (diff) |
remove siam, selling not allowed
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diff --git a/Master/texmf-dist/tex/plain/siam/pexample.tex b/Master/texmf-dist/tex/plain/siam/pexample.tex deleted file mode 100644 index eb2c2f50101..00000000000 --- a/Master/texmf-dist/tex/plain/siam/pexample.tex +++ /dev/null @@ -1,523 +0,0 @@ -% Sample file for SIAM's plain TeX macro package. -% 9-14-94 Paul Duggan -\input siamptex.sty - -% author defined macros included for illustrative purposes only. -% symbols for real numbers, complex, ... (\Bbb font from AMS-TeX -% fonts v2.x also usable) - -\def\fR{{\bf R}} -\def\fC{{\bf C}} -\def\fK{{\bf K}} - -% misc. operators -\def\Span {\mathop{\hbox{\rm span}}\nolimits} -\def\Range{\mathop{\hbox{\rm Range}}\nolimits} -\def\Det {\mathop{\hbox{\rm det}}} -\def\Re {\mathop{\hbox{\rm Re}}} -\def\Im {\mathop{\hbox{\rm Im}}} -\def\Deg {\mathop{\hbox{\rm deg}}} - -% misc. - -\def\Kr{\hbox{\bf K}} -\def\K { { K}} -\def\sT{\hbox{$\cal T$}} -\def\sB{\hbox{$\cal B$}} - -\def\bmatrix#1{\left[ \matrix{#1} \right]} - -% Each of the following commands have to be filled in with -% something. If the data is unknown, the arguments can be -% left blank. - -\topmatter -\journal{SIAM J. E{\smc XAMPLE} F{\smc ILES}} -\vol{1} -\no{1, pp.~000--000} -\date{October 1994} -\copyyear{1994} -\code{000} - - -\title SAMPLE FILE FOR SIAM PLAIN \TeX\ MACRO -PACKAGE\endtitle - -\shorttitle{SIAM MACRO EXAMPLE} - -\recdate{*}{October 1, 1994; accepted by the editors Month, x, -xxxx. This work was supported by the Society for Industrial -and Applied Mathematics, Philadelphia, Pennsylvania} - -\author Paul Duggan\fnmark{$^{\dag}$} \and Various A.~U. -Thors\fnmark{$^{\ddag}$}\endauthor - -\address{$^{\dag}$}{Composition Department, Society for -Industrial and Applied Mathematics, 3600 University City -Science Center, Philadelphia, Pennsylvania, 19104-2688 -({\tt duggan@siam.org})} - -\address{$^{\ddag}$}{Various affiliations, supported by -various foundation grants} - -\abstract{An example of SIAM \TeX\ macros is presented. -Various aspects of composing manuscripts for SIAM's journals -are illustrated with actual examples from accepted -manuscripts. SIAM's stylistic standards are adhered to -throughout, and illustrated.} - -\keywords polynomials, SI model\endkeywords - -\subjclass 33H40, 35C01\endsubjclass - -% if there is only one AMS subject number, the -% command \oneclass should precede the \subjclass command. - -\endtopmatter - -\heading{1}{Introduction and examples} -This paper presents a sample file for the use of SIAM's -\TeX\ macro package. It illustrates the features of the -macro package, using actual examples culled from various -papers published in SIAM's journals. This sample will provide -examples of how to use the -macros to generate standard elements of journal papers, -e.g., equations, theorems, or figures. This paper also -serves as an exmple of SIAM's stylistic preferences for the -formatting of such elements as bibliographic references, -displayed equations, and aligned equations, among others. -Some special circumstances are not dealt with this the -sample file; for that information, please see the -associated documentation file. - -{\it Note}. This paper is not to be read in any form for -content. The conglomeration of equations, lemmas, and other -text elements were put together solely for typographic -illustrative purposes. - -For theoretical reasons, it is desirable to find characterizations of the -conditions of breakdown of the algorithms that are based on the key {\it -spaces} $\Kr_n(r^{(0)},A)$ and $\Kr_n(\tilde r^{(0)},A^*)$ rather than -the {\it formulas} for the algorithms. In particular, we will -characterize breakdown of the three Lanczos algorithms in terms of the -{\it moment matrices} $\K_n(\tilde r^{(0)},A^*)^*\K_n(r^{(0)},A)$ and -$\K_n(\tilde r^{(0)},A^*)^*A\K_n(r^{(0)},A)$. Here we define the matrix -$\K_n(v,A)=\bmatrix{v&Av&\cdots&A^{n-1}v\cr}$, a matrix whose columns span -the Krylov space $\Kr_n(v,A)$. - -The following three theorems give exact conditions for breakdown of the -above algorithms. Detailed proofs may be found in [3]. A -result similar to Theorem 2 is found in [1]; see also [5]. - - -\thm{Theorem 1 {\rm (Lanczos--Orthodir breakdown)}} -Suppose Lanczos/Orthodir has successfully generated -$u^{(n-1)}\not=u$. Then the following are equivalent: - -\meti{$\bullet$} The algorithm does not break down at step $n$. - -\meti{$\bullet$} The matrix $\K_n(\tilde r^{(0)},A^*)^*A\K_n(r^{(0)},A)$ -is nonsingular. - -\meti{$\bullet$} There exists a unique iterate $u^{(n)}$ satisfying $(2)$. -\endthm - - -\thm{Theorem 2 {\rm (Lanczos--Orthomin breakdown)}} -Suppose Lanczos/Orthomin has successfully generated $u^{(n-1)}\not=u$. -Then the following are equivalent: - -\meti{$\bullet$} The algorithm breaks down at step $n$. - -\meti{$\bullet$} Either -$\K_{n-1}(\tilde r^{(0)},A^*)^*\K_{n-1}(r^{(0)},A)$ or -$\K_n(\tilde r^{(0)},A^*)^*A\K_n(r^{(0)},A)$ is singular. -\endthm - - -\prop{Proposition 3 {\rm (zero sets of polynomials)}} -Let $\fK=\fR$ or $\fC$. If $P$ is a complex nonzero polynomial in the -variables $x_1,x_2,\ldots ,x_N\in\fK$, then $P(x)\not=0$ for almost every -$x=(x_1,x_2,\ldots,x_N)\in \fK^N$. -\endprop - -\prf{Proof} -If $\fK=\fR$ and $P$ is nonzero, then either $\Re P(z)$ or $\Im P(z)$ -is a nonzero (real) polynomial; if $\fK=\fC$, we may decompose each $x_i$ -into real and imaginary parts, giving $2N$ variables, and consider the -real polynomial $P(x)^*P(x)$. In any case, we may assume without loss of -generality that $P$ is a nonzero real polynomial of real variables. - -We know that for any point $x$, the polynomial $P$ is the zero polynomial -if and only if the polynomial and all its derivatives are zero at $x$. -Let $V_0$ denote the set of zeros of $P$ in $\fR^N$. Suppose the set -$V_0$ has nonzero measure. We know from integration theory (see, for -example, [6, pp.\ 128f]) that almost every point of $V_0$ is -a point of density in each of the $N$ coordinate directions. We recall -that $x\in\fR$ is a point of density of a measurable subset -$S\subseteq\fR$ if for any sequence of intervals $I_n$ such that -$x\in I_n$ with measure $m(I_n)\rightarrow 0$ we have -$m(S\cap I_n)/m(I_n)\rightarrow 1$. - -It is easily seen that at such points in $V_0$, the first -partial derivatives of $P$ must necessarily be zero. Let $V_1$ be the -points of $V_0$ where all first derivatives are also zero. We have just -shown that $V_0$ and $V_1$ both have the same nonzero measure. The -argument -may be repeated for $V_1$ to show all second partial derivatives of $f$ -are zero at almost every point of $V_0$, and so forth, resulting in the -fact that $P$ and all its derivatives are zero on a set which has nonzero -measure. The proof is completed by selecting any one of these points. -\qquad\endproof - -\thm{Theorem 4 {\rm (Lanczos breakdown, iterate $n$)}} -Let $\fK=\fR$ or $\fC$, $A, \tilde Z\in\fK^{N\times N}$, and $n\leq d(A)$. -Then exactly one of the following three conditions holds for the Lanczos -method with $\tilde r^{(0)}=\tilde Z^* r^{(0)}$. - -\meti{\rm (i)} Hard breakdown at step $n$ occurs for every vector -$r^{(0)}\in\sT_n(A)\cap\fK^N$ $($and thus at least for almost every -$r^{(0)}\in\fK^N)$. - -\meti{\rm (ii)} Hard breakdown at step $n$ occurs for a nonempty measure-zero -set of vectors $r^{(0)}\in\sT_n(A)\cap\fK^N$ -$($and thus a nonempty measure-zero set of vectors in $\fK^N)$. - -\meti{\rm (iii)} Hard breakdown at step $n$ occurs for no vectors -$r^{(0)}\in\sT_n(A)\cap\fK^N$ $($and thus for at most a measure-zero set of -vectors in $\fK^N)$. - -Furthermore, the same result holds if ``hard breakdown'' is replaced by -``soft breakdown'' in the statement of this theorem. -\endthm - - -\prf{Proof} -For vectors $r^{(0)}\in\sT_n(A)\cap\fK^N$, breakdown is equivalent to -singularity of an appropriate moment matrix. The set $\sT_n(A)\cap\fK^N$ -amounts to almost -every vector in $\fK^N$. Now, by Corollary 5, the set $S_n$ of vectors in -$\fK^N$ for which the moment matrix of dimension $n$ is singular is either -the set of all vectors or a subset of measure zero. If the moment matrix -is singular for every vector (i.e., $S_n=\fK^N$), then it is singular for -every vector in $\sT_n(A)\cap\fK^N$, giving case (i) above. Otherwise the -set $S_n$ is measure zero in $\fK^N$. Thus -$\sB_n\equiv S_n\cap(\sT_n(A)\cap\fK^N)$ is of measure zero -and is either empty or nonempty. -\qquad\endproof - -\heading{2}{Tables and figures} -In Tables 1 and 2 we consider the unpreconditioned problem and also the (left) -ILU- and MILU-preconditioned problem (see [2] and [4]). Runs for which -convergence was not possible in ITMAX iterations are labeled by (--). - - -\topinsert -\hbox{\vbox{ \eightpoint -{\parindent 0pt -\centerline{\smc Table 1} -\centerline{\it Model problem, $h^{-1}=128$, {\rm ITMAX=3000}. - Number of iterations.}\vskip 6pt -\hfil\vbox{\offinterlineskip -\hrule -\halign{&\vrule#&\strut\ \hfil#\ \cr -height2pt&\omit&&\omit&&\omit&&\omit&&\omit - &&\omit&&\omit&&\omit&&\omit&&\omit&&\omit&\cr -&{\rm method $\backslash$ Dh: } & - &0&&2${}^{-3}$&&2${}^{-2}$&&2${}^{-1}$&&2${}^{0}$& - &2${}^{1}$&&2${}^{ 2}$&&2${}^{ 3}$&&2${}^{ 4}$&&2${}^{5}$&\cr -height2pt&\omit&&\omit&&\omit&&\omit&&\omit - &&\omit&&\omit&&\omit&&\omit&&\omit&&\omit&\cr -\noalign{\hrule} -height2pt&\omit&&\omit&&\omit&&\omit&&\omit - &&\omit&&\omit&&\omit&&\omit&&\omit&&\omit&\cr -&{GMRES}($\infty$) \hfill & -& 290&& 269&& 245&& 220&& 200&& 189&& 186&& 189&& 207&& 249&\cr -&{BCG} \hfill & -& 308&& 341&& 299&&1518&& -- && -- && -- && -- && 533&& -- &\cr -&{BCG}{\rm, random $u^{(0)}$} \hfill & -& 309&& 354&& 300&& 310&& 313&& 301&& 299&& 302&& 290&& 293&\cr -&{BCGNB} \hfill & -& 308&& 353&& 284&& 338&& 253&& 240&& 243&& 240&& 302&& 962&\cr -&{CGS} \hfill & -& 272&& 254&& 222&& -- && -- && -- && -- && -- && -- && -- &\cr -&{CGS}{\rm, random $u^{(0)}$} \hfill & -& 193&& 189&& 200&& 192&& 193&& 175&& 225&& 212&& 216&& 197&\cr -&{CGSNB} \hfill & -& 272&& 284&& 212&& 196&& 151&& 162&& 158&& 173&& 156&& 256&\cr -height1pt&\omit&&\omit&&\omit&&\omit&&\omit - &&\omit&&\omit&&\omit&&\omit&&\omit&&\omit&\cr -} \hrule}\hfil}}} -\endinsert - - -\topinsert - -\hbox{\vbox{ \eightpoint -{\parindent 0pt -\centerline{\smc Table 2} - -\centerline{\it Model Problem, $h^{-1}=128$,} -\centerline{\it {\rm MILU}-preconditioning, {\rm ITMAX=500.} -Number of iterations.} - -\medskip - -\hfil\vbox{\offinterlineskip -\hrule -\halign{&\vrule#&\strut\ \hfil#\ \cr -height2pt&\omit&&\omit&&\omit&&\omit&&\omit - &&\omit&&\omit&&\omit&&\omit&&\omit&&\omit&\cr -&{\rm Method $\backslash$ Dh: } & - &0&&2${}^{-3}$&&2${}^{-2}$&&2${}^{-1}$&&2${}^{0}$& - &2${}^{1}$&&2${}^{ 2}$&&2${}^{ 3}$&&2${}^{ 4}$&&2${}^{5}$&\cr -height2pt&\omit&&\omit&&\omit&&\omit&&\omit - &&\omit&&\omit&&\omit&&\omit&&\omit&&\omit&\cr -\noalign{\hrule} -height2pt&\omit&&\omit&&\omit&&\omit&&\omit - &&\omit&&\omit&&\omit&&\omit&&\omit&&\omit&\cr -&{\rm {GMRES}($\infty$)} \hfill & -& 27&& 25&& 24&& 26&& 28&& 28&& 25&& 19&& 14&& 10&\cr -&{\rm {GMRES}($\infty$), random $u^{(0)}$} \hfill & -& 33&& 29&& 28&& 29&& 31&& 31&& 29&& 24&& 19&& 14&\cr -&{\rm {BCG}} \hfill & -& 31&& 27&& 29&& 33&& 30&& 37&& 30&& 23&& 15&& 10&\cr -% &{BCG}, random $u^{(0)}$, $\gamma=.1$ \hfill & -% & 35&& 30&& 31&& 35&& 40&& 37&& 34&& 27&& 20&& 15&\cr -&{\rm {BCG}, random $u^{(0)}$} \hfill & -& 38&& 34&& 33&& 37&& 44&& 40&& 38&& 29&& 23&& 18&\cr -&{\rm {BCGNB}} \hfill & -& 28&& 27&& 29&& 30&& 34&& 35&& 30&& 23&& 15&& 10&\cr -&{\rm {CGS}} \hfill & -& 21&& 18&& 17&& 20&& 22&& 22&& 19&& 15&& 9&& 6&\cr -&{\rm {CGS}, random $u^{(0)}$} \hfill & -& 24&& 18&& 20&& 22&& 22&& 23&& 21&& 16&& 12&& 9&\cr -&{\rm {CGSNB}} \hfill & -& 21&& 18&& 17&& 20&& 22&& 27&& 20&& 15&& 9&& 6&\cr -height1pt&\omit&&\omit&&\omit&&\omit&&\omit - &&\omit&&\omit&&\omit&&\omit&&\omit&&\omit&\cr -} \hrule}\hfil}}} -\endinsert - -We make the following observations about these runs. - -\meti{$\bullet$} For the unpreconditioned problem, the standard -{BCG} and {CGS} algorithms break down in a number of cases, but the use -of random $u^{(0)}$ or the use of {BCGNB} or {CGSNB} -resulted in convergence. Furthermore, the iteration counts for the -algorithms {BCG} and {BCGNB} are in -general comparatively close to those of the ``best'' method, -{GMRES}($\infty$), while these algorithms have short economical -recurrences, unlike {GMRES}($\infty$). This underscores the -importance of the Lanczos algorithms as economical solution techniques. - -\meti{$\bullet$} For the ILU-preconditioned problems, in most cases -all methods worked well. For the case of $Dh=1$, {BCG} gave -an excessive number of iterations, but this was remedied significantly -by {BCGNB} and much more so -by the use of random $u^{(0)}$. Similarly, {CGS} could -not converge, but {CGSNB} and {CGS} with random -$u^{(0)}$ both converged. - -\meti{$\bullet$} For all of the MILU-preconditioned problems, all of -the Lanczos-type algorithms performed quite well. In particular, the -{BCG} algorithm gave approximately the same number of -iterations as {GMRES}($\infty$). - -Figures 1 and 2 give representative plots of the convergence behavior of the -algorithms for the case of $h^{-1}=128$, $Dh=4$, and no preconditioning. -These results show that the new algorithms keep the residual size -better behaved than the standard {BCG} and {CGS} -algorithms over the course of the run. - -\topinsert -\vskip 3.2in -\centerline{\eightpoint\smc Fig.~1. \it Residual -behavior: $h^{-1}=128$, $Dh=4$.} -\endinsert - - -\topinsert - \vskip 3.2in -\centerline{\eightpoint\smc Fig.~2. \it Residual -behavior: $h^{-1}=128$, $Dh=4$.} -\endinsert - -We now consider a more difficult class of finite difference problems, -namely, central finite differencing applied to the Dirichlet problem -$$ -u_{xx}(x,y) - u_{yy}(x,y) + - D[(y-\textstyle{1\over 2}\displaystyle) u_x(x,y) + - (x-\textstyle{1\over 3}\displaystyle) - (x-\textstyle{2\over 3}\displaystyle) u_y(x,y)], $$ -$$ - 43\pi^2u(x,y) = G(x,y) \quad {\rm on}\ \Omega=[0,1]^2,$$ -$$u(x,y) = 1 + xy \quad \hbox{\rm on}\ \partial\Omega,$$ -with $G(x,y)$ chosen as before so that the true solution is $u(x,y)=1+xy$. -Again, we let $h$ denote the mesh size in each direction. For $D=0$ -and $h$ small, the matrix generated by this problem is a symmetric -indefinite matrix with 16 distinct negative eigenvalues and the rest -of the spectrum positive. - -The standard conjugate residual algorithm applied to this problem with -$h^{-1}=128$ and $D=0$ requires 766 iterations to converge to -$||r^{(n)}||/||b||<\zeta=10^{-6}$. In any case, this is a difficult -problem to solve. - - \def\qed{\vrule height8pt width4pt depth0pt\par\medskip} - \def\Zero{{\bf 0}} - \def\dis{\displaystyle} - \def\b{\beta} - \def\r{\rho} - \def\X{{\bf X}} - \def\Y{{\bf Y}} - \def\bb{{\bar \beta}} - \def\tbcr{\theta\bb c_h \rho_h} - \def\ep{\varepsilon} - - - -Figures 3(a) and 3(b) show the compartmental diagrams for SI models without -and with deaths due to the disease, for the situation in which the infectious -period has only one stage. Figures 4(a) and 4(b) give the corresponding models -with $m$ stages of infection. Venereal -warts, caused by the human papilloma virus, and ordinary herpes are examples -of sexually transmitted diseases without deaths -due to the disease, although both are not quite SI diseases because of -partial immunity. AIDS is the example of an SI disease with death due to -the disease. Although our main focus is on the latter, we present results -on SI models without deaths due to the -disease because the simplification in the dynamics of such models - throws light on the case with disease-related deaths. - -\topinsert -\vskip 2in -\centerline{\eightpoint {\smc Fig.} 3(a). SI {\it model for subgroup $i$, without death -due to the disease.}} -\vskip 2in -\centerline{\eightpoint {\smc Fig.} 3(b). SI {\it model with death due to the disease.}} -\endinsert - -\topinsert -\vskip 2in -\centerline{\eightpoint {\smc Fig.} 4(a). SI {\it model without deaths due to the -disease with $m$ stages of infection.}} -\vskip 2in -\centerline{\eightpoint {\smc Fig.} 4(b). SI {\it model with deaths due to the disease, -with $m$ stages of infection.}} -\endinsert - -\heading{3}{Equations and alignments} -The equations for the system follow directly from the definitions and the -compartmental diagrams. For one infected stage with no disease-related -deaths, the equations are -$$ \dot X_i=-X_ig_i-\mu X_i+U_i, \leqno(1)$$ -$$ \dot Y_i=X_ig_i-\mu Y_i. \leqno(2)$$ -If there are multiple stages to the infection, (2) is replaced by -(3)--(5) as follows: -$$\leqalignno{\dot Y_{i1}&=X_ig_i-(k+\mu)Y_{i1}, &(3)\cr -\dot Y_{ir}&=kY_{i,r-1}-(k+\mu)Y_{ir},\qquad r=2,\ldots,m-1 &(4)\cr -\dot Y_{im}&=kY_{i,m-1}-\mu Y_{im}. &(5)\cr }$$ - - - -\heading{3.1}{The SI model with structured mixing} -In this subsection we write the equations for the SI model with -structured mixing, with one infected stage and with deaths due to the -disease. The equations for multiple infected stages follow easily, as do -those for SI models without death due to the disease. Recall that $f_{is}$ -gives the fraction of population subgroup $i$'s -contacts that are made in activity group $s$. The total contact rate of -susceptibles from population subgroup $i$ in activity group $s$ must be -$c_iX_if_{is}$. Let $\rho_{ij}(s)$ be the fraction of the contacts of group -$i$ that are with members of group $j$, within activity group $s$. -Assuming random allocation of the susceptibles and infecteds from each -population subgroup to the activity groups, the fraction infected in group -$j$ in activity group $s$ must be $Y_j/N_j$, giving -$$ c_iX_if_{is}\rho_{ij}(s)\beta_j{Y_j \over N_j}\leqno(6) $$ -for the rate at which susceptibles in $i$ are infected by contacts -with infecteds from $j$ in activity group $s$. Thus, in this case, $g_i$ is -given by -$$ - g_i=c_i\sum_sf_{is}\sum_j\rho_{ij}(s)\beta_j{Y_j \over N_j}, -\leqno(7) - $$ -and (1a) and (1b) become -$$ \dot X_i=-c_iX_i\sum_sf_{is}\sum_j\rho_{ij}(s)\beta_j{Y_j \over -N_j}-\mu X_i+U_i, \leqno(8) $$ -$$ \dot Y_i=c_iX_i\sum_sf_{is}\sum_j\rho_{ij}(s)\beta_j{Y_j \over -N_j}-(\mu+k)Y_i. \leqno(9) $$ - -\heading{3.2}{Structured mixing within activity groups} -If the mixing within activity groups is proportional mixing, then -$\rho_{ij}(s)$ is given by (10): -$$\rho_{ij}(s)={f_{js}c_jN_j\over \sum_pf_{ps}c_pN_p}, \leqno(10)$$ -and (8) and (9) become (11) and (12): -$$\dot X_i=-c_iX_i\sum_sf_{is}{\sum_jf_{js}c_j\beta_jY_j \over -\sum_jf_{js}c_jN_j}-\mu X_i+U_i \leqno(11)$$ -$$\dot Y_i=c_iX_i\sum_sf_{is}{\sum_jf_{js}c_j\beta_jY_j \over -\sum_jf_{js}c_jN_j}-(k+\mu)Y_i. \leqno(12)$$ - -Expressions (11) and (12) show an important consequence of death due -to the disease. If there are no deaths due to the disease, $N_j$ is -constant on the asymptotically stable invariant subspace $U_j=\mu -N_j$ for all $j$, and the first term, the nonlinear term, in -(11) and (12) is a sum of {\it quadratic} terms. If there are deaths -due to the disease, $N_j$ is no longer constant and the first term is -a sum of rational expressions, each homogeneous of degree one. This -observation extends to SIS, SIR, and SIRS models. - - - -\Refs - - -\ref 1\\ -{\smc R. Fletcher}, {\it Conjugate gradient methods for indefinite -systems}, in Numerical Analysis Dundee 1975, G.~A. Watson, ed., -Springer-Verlag, New York, Lecture Notes in Math. 506, -1976, pp. 73--89. -\endref - - -\ref 2\\ -{\smc I. Gustafsson}, {\it Stability and rate of convergence of -modified incomplete Cholesky factorization methods}, Ph.D. thesis, -Chalmers University of Technology and the University of Goteborg, -Goteborg, Sweden, 1979. -\endref - - -\ref 3\\ -{\smc W.~D. Joubert}, {\it Generalized conjugate gradient and -Lanczos methods for the solution of nonsymmetric systems of linear -equations}, Ph.D. thesis and Report -CNA-238, Center for Numerical Analysis, University of Texas, -Austin, TX, January 1990. -\endref - - -\ref 4\\ -{\smc J.~A. Meijerink and H.~A. van der Vorst}, {\it An iterative -solution method for linear systems of which the coefficient matrix is -a symmetric $M$-matrix}, Math. Comp., 31 (1977), pp.~148--162. -\endref - - - -\ref 5\\ -{\smc Y.~Saad}, {\it The Lanczos biorthogonalization algorithm and -other oblique projection methods for solving large unsymmetric systems}, -SIAM J. Numer. Anal., 19 (1982), pp. 485--506. -\endref - - -\ref 6\\ -{\smc S. Saks}, {\it The Theory of the Integral}, G.~E. Stechert, -New York, 1937. -\endref - -\ref 7\\ -{\smc M. Tinkham}, {\it Introduction to -Superconductivity}, McGraw-Hill, New York, 1975. -\endref - -\bye |