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20141003-CUBoulder.tex
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20141003-CUBoulder.tex
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% \documentclass[handout]{beamer}
\documentclass{beamer}
\mode<presentation>
{
\usetheme{ANLBlue}
% \usefonttheme[onlymath]{serif}
% \usetheme{Singapore}
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\usepackage{multimedia}
\usepackage{multicol}
\newcommand\hmmax{0}
\newcommand\bmmax{0}
\usepackage{bm}
\usepackage{comment}
\usepackage{subcaption}
% font definitions, try \usepackage{ae} instead of the following
% three lines if you don't like this look
\usepackage{mathptmx}
\usepackage[scaled=.90]{helvet}
% \usepackage{courier}
\usepackage[T1]{fontenc}
\usepackage{tikz}
\usetikzlibrary{decorations.pathreplacing}
\usetikzlibrary{shadows,arrows,shapes.misc,shapes.arrows,shapes.multipart,arrows,decorations.pathmorphing,backgrounds,positioning,fit,petri,calc,shadows,chains,matrix}
\newcommand\vvec{\bm v}
\newcommand\bvec{\bm b}
\newcommand\bxk{\bvec_0 \times \kappa_0 \cdot \nabla}
\newcommand\delp{\nabla_\perp}
% \usepackage{pgfpages}
% \pgfpagesuselayout{4 on 1}[a4paper,landscape,border shrink=5mm]
\usepackage{JedMacros}
\newcommand{\timeR}{t_{\mathrm{R}}}
\newcommand{\timeW}{t_{\mathrm{W}}}
\newcommand{\mglevel}{\ensuremath{\ell}}
\newcommand{\mglevelcp}{\ensuremath{\mglevel_{\mathrm{cp}}}}
\newcommand{\mglevelcoarse}{\ensuremath{\mglevel_{\mathrm{coarse}}}}
\newcommand{\mglevelfine}{\ensuremath{\mglevel_{\mathrm{fine}}}}
%solution and residual
\newcommand{\vx}{\ensuremath{x}}
\newcommand{\vc}{\ensuremath{\hat{x}}}
\newcommand{\vr}{\ensuremath{r}}
\newcommand{\vb}{\ensuremath{b}}
%operators
\newcommand{\vA}{\ensuremath{A}}
\newcommand{\vP}{\ensuremath{I_H^h}}
\newcommand{\vS}{\ensuremath{S}}
\newcommand{\vR}{\ensuremath{I_h^H}}
\newcommand{\vI}{\ensuremath{\hat I_h^H}}
\newcommand{\vV}{\ensuremath{\mathbf{V}}}
\newcommand{\vF}{\ensuremath{F}}
\newcommand{\vtau}{\ensuremath{\mathbf{\tau}}}
\title{On reducing communication and improving adaptivity in nonlinear multigrid methods}
\author{{\bf Jed Brown} \texttt{[email protected]} (ANL and CU Boulder) \\
\quad Mark Adams (LBL), Matt Knepley (UChicago)
}
% - Use the \inst command only if there are several affiliations.
% - Keep it simple, no one is interested in your street address.
% \institute
% {
% Mathematics and Computer Science Division \\ Argonne National Laboratory
% }
\date{CU Boulder Applied Math Colloquium, 2014-10-03 \\[1em]
This talk: \url{http://59A2.org/files/20141003-CUBoulder.pdf}}
% This is only inserted into the PDF information catalog. Can be left
% out.
\subject{Talks}
% If you have a file called "university-logo-filename.xxx", where xxx
% is a graphic format that can be processed by latex or pdflatex,
% resp., then you can add a logo as follows:
% \pgfdeclareimage[height=0.5cm]{university-logo}{university-logo-filename}
% \logo{\pgfuseimage{university-logo}}
% Delete this, if you do not want the table of contents to pop up at
% the beginning of each subsection:
% \AtBeginSubsection[]
% {
% \begin{frame}<beamer>
% \frametitle{Outline}
% \tableofcontents[currentsection,currentsubsection]
% \end{frame}
% }
% \AtBeginSection[]
% {
% \begin{frame}<beamer>
% \frametitle{Outline}
% \tableofcontents[currentsection]
% \end{frame}
% }
% If you wish to uncover everything in a step-wise fashion, uncomment
% the following command:
% \beamerdefaultoverlayspecification{<+->}
\begin{document}
\lstset{language=C}
\normalem
\begin{frame}
\titlepage
\end{frame}
\begin{frame}{Plan: ruthlessly eliminate communication}
\begin{itemize}
\item Eliminate, not ``aggregate and amortize''
\end{itemize}
\begin{block}{Why?}
\begin{itemize}
\item Enables pruning unnecessary work
\item More scope for dynamic load balance
\item Tolerance for high-frequency load imbalance
\begin{itemize}
\item From irregular computation or hardware error correction
\end{itemize}
\item Local recovery despite global coupling
\end{itemize}
\end{block}
\begin{block}{Requirements}
\begin{itemize}
\item Must retain optimal convergence with good constants
\item Flexible, robust, and debuggable
\end{itemize}
\end{block}
\end{frame}
\section{$\tau$-adaptivity and multigrid compression}
\begin{frame}[fragile]{Multigrid Preliminaries}
\begin{figure}
\centering
\begin{tikzpicture}
[>=stealth,
every node/.style={inner sep=2pt},
restrict/.style={thick},
prolong/.style={thick},
mglevel/.style={rounded rectangle,draw=blue!50!black,fill=blue!20,thick,minimum size=4mm},
]
\begin{scope}\scriptsize
\newcommand\mgdx{4.0em}
\newcommand\mgdy{4.0em}
\newcommand\mgl[1]{(pow(2,#1+1))}
\newcommand\mgloc[4]{(#1 + #4*\mgdx*#3,#2 + \mgdy*#3)}
\newcommand\mghx{0.9*\mgdx}
\newcommand\mghy{0.9*\mgdy}
\draw[shift=\mgloc{0*\mgdx}{0}{0}{0},
xstep=\mghy/\mgl{3},
ystep=\mghy/\mgl{3}]
(-0.5*\mghy,-0.5*\mghy) grid (0.5*\mghy,0.5*\mghy);
\draw[shift=\mgloc{1*\mgdx}{0}{0}{0},
xstep=\mghy/\mgl{2},
ystep=\mghy/\mgl{2}]
(-0.5*\mghy,-0.5*\mghy) grid (0.5*\mghy,0.5*\mghy);
\draw[shift=\mgloc{2*\mgdx}{0}{0}{0},
xstep=\mghy/\mgl{1},
ystep=\mghy/\mgl{1}]
(-0.5*\mghy,-0.5*\mghy) grid (0.5*\mghy,0.5*\mghy);
\draw[shift=\mgloc{3*\mgdx}{0}{0}{0},
xstep=\mghy/\mgl{0},
ystep=\mghy/\mgl{0}]
(-0.5*\mghy,-0.5*\mghy) grid (0.5*\mghy,0.5*\mghy);
\end{scope}
\end{tikzpicture}
\label{fig:levels}
\end{figure}
\textbf{Multigrid} is an $O(n)$ method for solving algebraic problems by defining a hierarchy of scale.
A multigrid method is constructed from:
\begin{enumerate}
\item a sequence of discretizations
\begin{itemize}
\item coarser approximations of problem, same or different equations
\item constructed algebraically or geometrically
\end{itemize}
\item intergrid transfer operators
\begin{itemize}
\item residual restriction $I_h^H$ (fine to coarse)
\item state restriction $\hat I_h^H$ (fine to coarse)
\item partial state interpolation $I_H^h$ (coarse to fine, `prolongation')
\item state reconstruction $\mathbb{I}_H^h$ (coarse to fine)
\end{itemize}
\item Smoothers ($S$)
\begin{itemize}
\item correct the high frequency error components
\item Richardson, Jacobi, Gauss-Seidel, etc.
\item Gauss-Seidel-Newton or optimization methods
\item Compatible Monte Carlo, \ldots
\end{itemize}
\end{enumerate}
\end{frame}
\input{slides/MG/TauFAS.tex}
\begin{frame}{Model problem: $\pfrak$-Laplacian with slip boundary conditions}
\begin{itemize}
\item 2-dimensional model problem for power-law fluid cross-section
\begin{equation*}
-\div \big(\abs{\nabla u}^{\pfrak-2} \nabla u \big) - f = 0, \qquad 1 \le \pfrak \le \infty
\end{equation*}
Singular or degenerate when $\nabla u = 0$
\item Regularized variant
\begin{gather*}
-\div (\eta \nabla u) - f = 0 \\
\eta(\gamma) = (\epsilon^2 + \gamma)^{\frac{\pfrak-2}{2}} \qquad \gamma(u) = \half \abs{\nabla u}^2
\end{gather*}
\item Friction boundary condition on one side of domain
\begin{gather*}
\nabla u \cdot \bm n + A(x) \abs{u}^{q-1} u = 0
\end{gather*}
\end{itemize}
\end{frame}
\begin{frame}{Model problem: $\pfrak$-Laplacian with slip boundary conditions}
\begin{itemize}
\item $\pfrak = 1.3$ and $q = 0.2$, checkerboard coefficients $\{10^{-2},1\}$
\item Friction coefficient $A=0$ in center, 1 at corners
\end{itemize}
\begin{columns}
\begin{column}{0.5\textwidth}
\only<1>{\includegraphics[width=\textwidth]{figures/MG/ex15-friction/visit0010.png}}
\only<2>{\includegraphics[width=\textwidth]{figures/MG/ex15-friction/visit0011.png}}
\only<3>{\includegraphics[width=\textwidth]{figures/MG/ex15-friction/visit0012.png}}
\only<4>{\includegraphics[width=\textwidth]{figures/MG/ex15-friction/visit0013.png}}
\only<5>{\includegraphics[width=\textwidth]{figures/MG/ex15-friction/visit0014.png}}
\only<6>{\includegraphics[width=\textwidth]{figures/MG/ex15-friction/visit0015.png}}
\end{column}
\begin{column}{0.5\textwidth}
\includegraphics[width=\textwidth]{figures/MG/newton-convergence.png}
\end{column}
\end{columns}
\end{frame}
\begin{frame}{$\tau$ corrections}
\begin{figure}
\centering
\begin{subfigure}[b]{0.18\textwidth}
\includegraphics[width=\textwidth]{figures/MG/ElasticityCompressTrim}
%\caption{Initial solution.}\label{fig:elast-initial}
\end{subfigure} ~
\begin{subfigure}[b]{0.18\textwidth}
\includegraphics[width=\textwidth]{figures/MG/ElasticityCompressShearTrim}
%\caption{Increment.}\label{fig:elast-increment}
\end{subfigure} ~
\begin{subfigure}[b]{0.28\textwidth}
\includegraphics[width=\textwidth]{figures/MG/ElasticityCompressErrorNoTauTrim}
%\caption{Smoothed error without $\tau$.}\label{fig:elast-error-notau}
\end{subfigure} ~
\begin{subfigure}[b]{0.28\textwidth}
\includegraphics[width=\textwidth]{figures/MG/ElasticityCompressErrorTauTrim}
%\caption{Smoothed error with $\tau$.}\label{fig:elast-error-tau}
\end{subfigure}
\begin{itemize}
\item Plane strain elasticity, $E=1000,\nu=0.4$ inclusions in $E=1,\nu=0.2$ material, coarsen by $3^2$.
\item Solve initial problem everywhere and compute $\tau_h^H = A^H \hat I_h^H u^h - I_h^H A^h u^h$
\item Change boundary conditions and solve FAS coarse problem
\begin{equation*}
N^H \acute u^H = \underbrace{I_h^H \acute f^h}_{\acute f^H} + \underbrace{N^H \hat I_h^H \tilde u^h - I_h^H N^h \tilde u^h}_{\tau_h^H}
\end{equation*}
\item Prolong, post-smooth, compute error $e^h = \acute u^h - (N^h)^{-1} \acute f^h$
\item<2> \alert{Coarse grid \emph{with $\tau$} is nearly $10\times$ better accuracy}
\end{itemize}
% \caption{Plane strain elasticity, $E=1000,\nu=0.4$ inclusions in $E=1,\nu=0.2$ material. 2-level multigrid with coarsening factor of $3^2$.
% Panes (a) and (b) show the deformed body colored by strain.
% The initial problem of compression by 0.2 from the right is solved (a) and $\tau = A^H \hat I_h^H u^h - I_h^H A^h u^h$ is computed.
% Then a shear increment of 0.1 in the $y$ direction is added to the boundary condition, and the coarse-level problem is resolved, interpolated to the fine-grid, and a post-smoother is applied.
% When the coarse problem is solved without a $\tau$ correction (c), the displacement error is nearly $10\times$ larger than when $\tau$ is included in the right hand side of the coarse problem (d).
% }\label{fig:tau-valid}
% ./ex49 -mx 90 -my 90 -da_refine_x 3 -da_refine_y 3 -elas_ksp_converged_reason -elas_ksp_rtol 1e-8 -no_view -c_str 3 -sponge_E0 1 -sponge_E1 1e3 -sponge_nu0 0.4 -sponge_nu1 0.2 -sponge_t 3 -sponge_w 9 -u_o vtk:ex49_sol.vts -use_nonsymbc -elas_pc_type mg -elas_pc_mg_levels 2 -elas_pc_mg_galerkin -tau1_o vtk:ex49_tau1.vts -tau2_o vtk:ex49_tau2.vts -taudiff_o vtk:ex49_taudiff.vts -u2_o vtk:ex49_sol2.vts -u2c_o vtk:ex49_sol2c.vts -u3_o vtk:ex49_sol3.vts -u4_o vtk:ex49_sol4.vts -u2err_o vtk:ex49_sol2err.vts -u3err_o vtk:ex49_sol3err.vts -u3c_o vtk:ex49_sol3c.vts -tau3_o vtk:ex49_tau3.vts
\end{figure}
\end{frame}
\begin{frame}{$\tau$ adaptivity: an idea for heterogeneous media}
\begin{itemize}
\item Applications with localized nonlinearities
\begin{itemize}
\item Subduction, rifting, rupture/fault dynamics
\item Carbon fiber, biological tissues, fracture
\end{itemize}
\item Adaptive methods fail for heterogeneous media
\begin{itemize}
\item Rocks are rough, solutions are not ``smooth''
\item Cannot build accurate coarse space without scale separation
\end{itemize}
\item $\tau$ adaptivity
\begin{itemize}
\item Fine-grid work needed everywhere at first
\item Then $\tau$ becomes accurate in nearly-linear regions
\item Only visit fine grids in ``interesting'' places: active nonlinearity, drastic change of solution
\end{itemize}
\end{itemize}
\end{frame}
\begin{frame}{Comparison to nonlinear domain decomposition}
\begin{itemize}
\item ASPIN (Additive Schwarz preconditioned inexact Newton) \\
\begin{itemize}
\item Cai and Keyes (2003)
\item More local iterations in strongly nonlinear regions
\item Each nonlinear iteration only propagates information locally
\item Many real nonlinearities are activated by long-range forces
\begin{itemize}
\item locking in granular media (gravel, granola)
\item binding in steel fittings, crack propagation
\end{itemize}
\item Two-stage algorithm has different load balancing
\begin{itemize}
\item Nonlinear subdomain solves
\item Global linear solve
\end{itemize}
\end{itemize}
\item $\tau$ adaptivity
\begin{itemize}
\item Minimum effort to communicate long-range information
\item Nonlinearity sees effects as accurate as with global fine-grid feedback
\item Fine-grid work always proportional to ``interesting'' changes
\end{itemize}
\end{itemize}
\end{frame}
\input{slides/MG/SmoothingNonlinearProblems.tex}
\subsection{Reducing communication and memory bandwidth}
\input{slides/MG/LowComm.tex}
\begin{frame}{Segmental refinement: no horizontal communication}
\begin{itemize}
\item 27-point second-order stencil, manufactured analytic solution
\item 5 SR levels: $16^3$ cells/process local coarse grid
\item $\text{Overlap} = \text{Base} + (L-\ell) \text{Increment}$
\begin{itemize}
\item Implementation requires even number of cells---round down.
\end{itemize}
\item FMG with $V(2,2)$ cycles
\end{itemize}
\begin{columns}
\begin{column}{0.4\textwidth}
\begin{table}\small
\centering\caption{$\norm{e_{SR}}_\infty / \norm{e_{FMG}}_\infty$}\label{tab:sr-error}
\begin{tabular}{l rrr}
\toprule
& \multicolumn{3}{c}{Base} \\
Increment & 1 & 2 & 3 \\
\midrule
1 & {\color{red} 1.59} & {\color{red} 2.34} & 1.00 \\
2 & 1.00 & 1.00 & 1.00 \\
3 & 1.00 & 1.00 & 1.00 \\
\bottomrule
\end{tabular}
\end{table}
\end{column}
\begin{column}{0.6\textwidth}
\includegraphics[width=\textwidth]{figures/MG/weak_scaling_edison-eps-converted-to.pdf}
\end{column}
\end{columns}
\end{frame}
\begin{frame}{Reducing memory bandwidth}
\includegraphics[width=\textwidth]{figures/MG/SRMGWindow}
\begin{itemize}
\item Sweep through ``coarse'' grid with moving window
\item Zoom in on new slab, construct fine grid ``window'' in-cache
\item Interpolate to new fine grid, apply pipelined smoother ($s$-step)
\item Compute residual, accumulate restriction of state and residual into coarse grid, expire slab from window
\end{itemize}
\end{frame}
\begin{frame}{Arithmetic intensity of sweeping visit}
\begin{itemize}
\item Assume 3D cell-centered, 7-point stencil
\item 14 flops/cell for second order interpolation
\item $\ge 15$ flops/cell for fine-grid residual or point smoother
\item 2 flops/cell to enforce coarse-grid compatibility
\item 2 flops/cell for plane restriction
\item assume coarse grid points are reused in cache
\item Fused visit reads $u^H$ and writes $\hat I_h^H u^h$ and $I_h^H r^h$
\item Arithmetic Intensity
\begin{equation}
\frac{{\overbrace{15}^{\text{interp}}} + {\overbrace{2\cdot (15+2)}^{\text{compatible relaxation}}} + \overbrace{2\cdot 15}^{\text{smooth}} + \overbrace{15}^{\text{residual}} + \overbrace{2}^{\text{restrict}}}{3 \cdot \texttt{sizeof(scalar)} / \underbrace{2^3}_{\text{coarsening}}} \gtrsim 30
\end{equation}
\item Still $\gtrsim 10$ with non-compressible fine-grid forcing
\end{itemize}
\end{frame}
\begin{frame}{Regularity}
Accuracy of recovery depends on operator regularity
\begin{itemize}
\item Even with regularity, we can only converge up to discretization error, unless we add a \emph{consistent} fine-grid residual evaluation
\item Visit fine grid with some overlap, but patches do not agree exactly in overlap
\item Need decay length for high-frequency error components (those that restrict to zero) that is bounded with respect to grid size
\item Required overlap $J$ is proportional to the number of cells to cover decay length
\item Can enrich coarse space along boundary, but causes loss of coarse-grid sparsity
\item Brandt and Diskin (1994) has two-grid LFA showing $J \lesssim 2$ is sufficient for Laplacian
\item With $L$ levels, overlap $J(k)$ on level $k$,
\begin{equation*}
2J(k) \ge s (L-k+1)
\end{equation*}
where $s$ is the smoothness order of the solution or the discretization order (whichever is smaller)
\end{itemize}
\end{frame}
\begin{frame}{Basic resilience strategy}
\begin{tikzpicture}
[scale=0.8,every node/.style={scale=0.8},
>=stealth,
control/.style={rectangle,rounded corners,draw=blue!50!black,fill=blue!20,thick,minimum width=5em},
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ephemeral/.style={rectangle,rounded corners,draw=gray!50!black,fill=gray!20,thick,minimum width=5em},
statebox/.style={rectangle,draw=green!50!black,thick},
statetitle/.style={rectangle,draw=green!50!black,fill=green!20,thick},
storebox/.style={rectangle,draw=},
rightbrace/.style={decorate,decoration={brace,amplitude=1ex,raise=4pt}},
leftbrace/.style={decorate,decoration={brace,amplitude=1ex,raise=4pt,mirror}}
]
\scriptsize
\node[control,minimum width=8em] (progcontrol) {control};
\node[essential,below=2pt of progcontrol.south,rectangle split,rectangle split parts=2,rectangle split horizontal,minimum width=12em] (progessential) {essential \nodepart{two} coarse};
\node[ephemeral,minimum width=8em,below=2pt of progessential.south] (progephemeral) {ephemeral};
\node[statebox,fit=(progcontrol)(progessential)(progephemeral)] (progbox) {};
\node[above=0pt of progbox.north,anchor=south] {\textbf{program $n=0$}};
\node[control,right=9em of progcontrol] (storecontrol) {control};
\node[essential,below=2pt of storecontrol.south] (storeessential) {essential};
\node[essential,minimum width=4em,below=6pt of storeessential.south, double copy shadow] (storecoarse) {coarse};
\node[statebox,decorate,decoration={bumps,mirror},fit=(storecontrol)(storecoarse)] (storebox) {};
\node[above=1pt of storebox.north,anchor=south] {\textbf{storage}};
\node[control,right=7em of storecontrol] (reccontrol) {control};
\node[essential,below=2pt of reccontrol.south] (recessential) {essential};
\node[statebox,fit=(reccontrol)(recessential)] (recbox) {};
\node[above=0pt of recbox.north,anchor=south] {\textbf{restored $n=0$}};
\node[control,right=6em of reccontrol] (donecontrol) {control};
\node[essential,below=2pt of donecontrol.south] (doneessential) {essential};
\node[ephemeral,below=2pt of doneessential.south] (doneephemeral) {ephemeral};
\node[statebox,fit=(donecontrol)(doneephemeral)] (donebox) {};
\node[above=0pt of donebox.north,anchor=south] {\textbf{recovered $n=N$}};
\draw[decorate,decoration={brace,amplitude=1ex,raise=4pt}] ($(progcontrol.north east) + (3pt,0)$) -- ($(progephemeral.north east) + (3pt,0)$) node[midway,xshift=1ex] (progbrace) {};
\draw[leftbrace] ($(storecontrol.north west) - (4pt,0)$) -- ($(storeessential.south west) - (4pt,0)$) node[midway,xshift=-1ex] (storebrace) {};
\draw[rightbrace] ($(storecontrol.north east) + (4pt,0)$) -- ($(storeessential.south east) + (4pt,0)$) node[midway,xshift=1ex] (storerbrace) {};
\draw[->,shorten >=4pt,shorten <=4pt] (progbrace) -- (storebrace) node[midway,above] (midarrow) {MPI/BLCR};
\node[below=1.4em of midarrow,essential,draw=red!50!gray!70,fill=red!10] (coarserun) {};
\draw[->,dashed,shorten >=14pt,shorten <=4pt] (coarserun) |- (storecoarse) node [near start,below,yshift=-3pt] {\scriptsize $n=1,2,\dotsc,N$};
\draw[->,shorten >=4pt,shorten <=4pt] (storerbrace) -- (recbox.west) node[midway,above,text width=5em,align=center] (midarrow) {restart failed ranks};
\draw[->,shorten >=5pt,shorten <=4pt] (recessential.east) -- (doneessential) node[midway,above,text width=5em,align=center] (fmgrecover) {FMG recovery};
\draw[->,dashed,shorten >=1pt,shorten <=3pt] ($(storecoarse.east) + (1em,0)$) -| (fmgrecover) node[midway,below,xshift=-1em] {\scriptsize $n=1,2,\dotsc,N$};
\draw[->,dashed,shorten >=3pt,shorten <=3pt] (donecontrol.east) -| ($(donecontrol.east) + (3ex,0)$) |- (doneephemeral.east) node[midway,right,text width=4em] {\cverb|malloc| at $n=0$};
\end{tikzpicture}
\begin{description}
\item[control] contains program stack, solver configuration, etc.
\item[essential] program state that cannot be easily reconstructed: time-dependent solution, current optimization/bifurcation iterate
\item[ephemeral] easily recovered structures: assembled matrices, preconditioners, residuals, Runge-Kutta stage solutions
\end{description}
\begin{itemize}
\item Essential state at time/optimization step $n$ is \alert{inherently globally coupled} to step $n-1$ (otherwise we could use an explicit method)
\item \emph{Coarse} level checkpoints are orders of magnitude smaller, but allow rapid recovery of essential state
\item FMG recovery needs only \alert{nearest neighbors}
\end{itemize}
\end{frame}
\begin{frame}[fragile]{Multiscale compression and recovery using $\tau$ form}
\begin{tikzpicture}
[scale=0.7,every node/.style={scale=0.7},
>=stealth,
restrict/.style={thick,double},
prolong/.style={thick,double},
cprestrict/.style={green!50!black,thick,double,dashed},
control/.style={rectangle,red!40!black,draw=red!40!black,thick},
mglevel/.style={rounded rectangle,draw=blue!50!black,fill=blue!20,thick,minimum size=6mm},
checkpoint/.style={rectangle,draw=green!50!black,fill=green!20,thick,minimum size=6mm},
mglevelhide/.style={rounded rectangle,draw=gray!50!black,fill=gray!20,thick,minimum size=6mm},
tau/.style={text=red!50!black,draw=red!50!black,fill=red!10,inner sep=1pt},
crelax/.style={text=green!50!black,fill=green!10,inner sep=0pt}
]
\begin{scope}
\newcommand\mgdx{1.9em}
\newcommand\mgdy{2.5em}
\newcommand\mgloc[4]{(#1 + #4*\mgdx*#3,#2 + \mgdy*#3)}
\node[mglevel] (fine0) at \mgloc{0}{0}{4}{-1} {\mglevelfine};
\node[mglevel] (finem1down0) at \mgloc{0}{0}{3}{-1} {};
\node[mglevel] (cp1down0) at \mgloc{0}{0}{2}{-1} {$\mglevelcp+1$};
\node[mglevel] (cpdown0) at \mgloc{0}{0}{1}{-1} {\mglevelcp};
\node[mglevel] (coarser0) at \mgloc{0}{0}{0}{0} {\ldots};
\node[mglevelhide] (cpup0) at \mgloc{0}{0}{1}{1} {};
\node (cp1up0) at \mgloc{0}{0}{2}{1} {};
\node (cpdown1) at \mgloc{4em}{0}{1}{-1} {};
\node[mglevelhide] (coarser1) at \mgloc{4em}{0}{0}{1} {\ldots};
\node[mglevel] (cpup1) at \mgloc{4em}{0}{1}{1} {\mglevelcp};
\node[mglevel] (cp1up1) at \mgloc{4em}{0}{2}{1} {$\mglevelcp+1$};
\node[mglevel] (finem1up1) at \mgloc{4em}{0}{3}{1} {};
\node[mglevel] (fine1) at \mgloc{4em}{0}{4}{1} {\mglevelfine};
\draw[->,restrict,dashed] (fine0) -- (finem1down0);
\draw[->,restrict] (finem1down0) -- (cp1down0);
\draw[->,restrict] (cp1down0) -- (cpdown0);
\draw[->,restrict,dashed] (cpdown0) -- (coarser0);
\draw[->,prolong,dashed] (coarser0) -- (cpup0);
\draw[->,prolong,dashed] (cpup0) -- (cp1up0);
\draw[->,restrict,dashed] (cpdown1) -- (coarser1);
\draw[->,prolong,dashed] (coarser1) -- (cpup1);
\draw[->,prolong] (cpup1) -- (cp1up1);
\draw[->,prolong] (cp1up1) -- (finem1up1);
\draw[->,prolong,dashed] (finem1up1) -- (fine1);
\node[checkpoint] at (4em + \mgdx*4,\mgdy) (cp) {CP};
\draw[>->,cprestrict] (fine1) -- node[below,sloped] {Restrict} (cp);
\node[left=\mgdx of fine0] (bnanchor) {};
\node[control,fill=red!20] at (1.1*\mgdx,3*\mgdy) {Solve $F(u^n;b^n) = 0$};
\node[mglevel,right=of fine1] (finedt) {next solve};
\draw[->, >=stealth, control] (fine1) to[out=20,in=170] node[above] {$b^{n+1}(u^n,b^n)$} (finedt);
\draw[->, >=stealth, control] (bnanchor) to[out=45,in=155] node[above] {$b^n$} (fine0);
% Recovery process
\begin{scope}[xshift=8*\mgdx]
\node[checkpoint] (rcp) at \mgloc{0}{0}{0}{0} {CP};
\node[mglevel] (r0a) at \mgloc{0}{\mgdy}{0}{0} {CR};
\node[mglevel] (r1a) at \mgloc{0}{\mgdy}{1}{1} {};
\node[mglevel] (r0b) at \mgloc{2*\mgdx}{\mgdy}{0}{0} {CR};
\node[mglevel] (r1b) at \mgloc{2*\mgdx}{\mgdy}{1}{1} {};
\node[mglevel] (r2b) at \mgloc{2*\mgdx}{\mgdy}{2}{1} {\mglevelfine};
\node[mglevel] (r1c) at \mgloc{6*\mgdx}{\mgdy}{1}{-1} {};
\node[mglevel] (r0d) at \mgloc{6*\mgdx}{\mgdy}{0}{0} {CR};
\node[mglevel] (r1d) at \mgloc{6*\mgdx}{\mgdy}{1}{1} {};
\node[mglevel] (r2d) at \mgloc{6*\mgdx}{\mgdy}{2}{1} {\mglevelfine};
\draw[-,prolong,green!50!black] (rcp) -- (r0a);
\draw[->,prolong] (r0a) -- (r1a);
\draw[->,restrict] (r1a) -- (r0b);
\draw[->,restrict] (r0b) -- (r1b);
\draw[->,restrict,dashed] (r1b) -- (r2b);
\draw[->,restrict,dashed] (r2b) -- (r1c);
\draw[->,restrict] (r1c) -- (r0d);
\draw[->,restrict] (r0d) -- (r1d);
\draw[->,restrict,dashed] (r1d) -- (r2d);
\foreach \smooth in {finem1down0, cp1down0, cpdown0, coarser0,
cpup1, cp1up1, finem1up1,
r0b,r1c,r0d,r1d} {
\node[above left=-5pt of \smooth.west,tau] {$\tau$};
}
\node[rectangle,fill=none,draw=green!50!black,thick,fit=(rcp)(r2d)] (recoverbox) {};
\node[rectangle,draw=green!50!black,fill=green!20,thick,minimum size=6mm,above={0cm of recoverbox.south east},anchor=south east] (recover) {FMG Recovery};
\end{scope}
\node (notation) at (\mgdx,5*\mgdy) {
\begin{minipage}{18em}\small\sf
\begin{itemize}\addtolength{\itemsep}{-5pt}
\item checkpoint converged coarse state
\item recover using FMG anchored at $\mglevelcp+1$
\item needs only $\mglevelcp$ neighbor points
\item $\tau$ correction is local
\end{itemize}
\end{minipage}
};
\end{scope}
\end{tikzpicture}
\begin{itemize}
\item Normal multigrid cycles visit all levels moving from $n \to n+1$
\item FMG recovery only accesses levels finer than $\ell_{CP}$
% \item Only failed processes and neighbors participate in recovery
\item Lightweight checkpointing for transient adjoint computation
\item Postprocessing applications, e.g., in-situ visualization at high temporal resolution in part of the domain
\end{itemize}
\end{frame}
\begin{frame}{First-order cost model for FAS resilience}
Extend first-order locality-unaware model of Young (1974):
\begin{description}
\item[$\timeW$] time to write a heavy fine-grid checkpointed state
\item[$\timeR$] time to read back lost state
\item[$R$] fraction of forward simulation needed for recomputation from a saved state
\item[$P$] the heavy checkpoint interval
\item[$M$] mean time to failure
\end{description}
Neglect cost of I/O for lightweight coarse-grid checkpoints
\begin{equation*}\label{eq:overhead}
\text{Overhead} = 1 - \text{AppUtilization} = \underbrace{\frac{\timeW}{P}}_{\text{writing}}
+ \underbrace{\frac{\timeR}{M}}_{\text{reading after failure}}
+ \underbrace{\frac{R P}{2M}}_{\text{recomputation}}
\end{equation*}
Minimized for a heavy checkpointing interval $P = \sqrt{2 M \timeW / R}$
\begin{equation*}\label{eq:minoverhead}
\text{Overhead}^* = \sqrt{2 \timeW R / M} + \timeR / M
% $ \text{Overhead}^* = \sqrt{\frac{2 \timeW R}{M}} + \frac{\timeR}{M} $,
\end{equation*}
where the first term is always larger than the second.
Conventional checkpointing schemes store only fine-grid state, thus $R=1$ (recovery costs the same as initial computation).
\end{frame}
\begin{frame}{Other uses}
\begin{itemize}
\item Transient adjoints
\begin{itemize}
\item Adjoint model runs backward-in-time, needs state from solution of forward model
\item Status quo: hierarchical checkpointing
\item Memory-constrained and requires computing forward model multiple times
\item If forward model is stiff, each step has global dependence
\item Compression via $\tau$-FAS accelerates recomputation, can be local
\end{itemize}
\item Visualization and analysis
\begin{itemize}
\item Targeted visualization in small part of domain
\item Interesting features emergent so can't predict where to look
\end{itemize}
\end{itemize}
\end{frame}
\begin{frame}{Outlook on $\tau$-FAS adaptivity and compression}
\begin{itemize}
\item Benefits of AMR without fine-scale smoothness
\item Coarse-centric restructuring is a major interface change
\item Nonlinear smoothers (and discretizations)
\begin{itemize}
\item Smooth in neighborhood of ``interesting'' fine-scale features
\item Which discretizations can provide efficient matrix-free smoothers?
\item Does there exist an efficient smoother based on element Neumann problems?
\end{itemize}
\item Dynamic load balancing
\item Reliability of error estimates for refreshing $\tau$
\begin{itemize}
\item We want a coarse indicator for whether $\tau$ needs to change
\end{itemize}
\item Worthwhile for resilience and to better use hardware
\end{itemize}
\end{frame}
\end{document}