\documentclass[12pt,titlepage]{article} \usepackage{amsmath} \usepackage{mathrsfs} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsthm} \usepackage{mathtools} \usepackage{graphicx} \usepackage{color} \usepackage{ucs} \usepackage[utf8x]{inputenc} \usepackage{xparse} \usepackage{hyperref} %----Macros---------- % % Unresolved issues: % % \righttoleftarrow % \lefttorightarrow % % \color{} with HTML colorspec % \bgcolor % \array with options (without options, it's equivalent to the matrix environment) % Of the standard HTML named colors, white, black, red, green, blue and yellow % are predefined in the color package. Here are the rest. \definecolor{aqua}{rgb}{0, 1.0, 1.0} \definecolor{fuschia}{rgb}{1.0, 0, 1.0} \definecolor{gray}{rgb}{0.502, 0.502, 0.502} \definecolor{lime}{rgb}{0, 1.0, 0} \definecolor{maroon}{rgb}{0.502, 0, 0} \definecolor{navy}{rgb}{0, 0, 0.502} \definecolor{olive}{rgb}{0.502, 0.502, 0} \definecolor{purple}{rgb}{0.502, 0, 0.502} \definecolor{silver}{rgb}{0.753, 0.753, 0.753} \definecolor{teal}{rgb}{0, 0.502, 0.502} % Because of conflicts, \space and \mathop are converted to % \itexspace and \operatorname during preprocessing. % itex: \space{ht}{dp}{wd} % % Height and baseline depth measurements are in units of tenths of an ex while % the width is measured in tenths of an em. \makeatletter \newdimen\itex@wd% \newdimen\itex@dp% \newdimen\itex@thd% \def\itexspace#1#2#3{\itex@wd=#3em% \itex@wd=0.1\itex@wd% \itex@dp=#2ex% \itex@dp=0.1\itex@dp% \itex@thd=#1ex% \itex@thd=0.1\itex@thd% \advance\itex@thd\the\itex@dp% \makebox[\the\itex@wd]{\rule[-\the\itex@dp]{0cm}{\the\itex@thd}}} \makeatother % \tensor and \multiscript \makeatletter \newif\if@sup \newtoks\@sups \def\append@sup#1{\edef\act{\noexpand\@sups={\the\@sups #1}}\act}% \def\reset@sup{\@supfalse\@sups={}}% \def\mk@scripts#1#2{\if #2/ \if@sup ^{\the\@sups}\fi \else% \ifx #1_ \if@sup ^{\the\@sups}\reset@sup \fi {}_{#2}% \else \append@sup#2 \@suptrue \fi% \expandafter\mk@scripts\fi} \def\tensor#1#2{\reset@sup#1\mk@scripts#2_/} \def\multiscripts#1#2#3{\reset@sup{}\mk@scripts#1_/#2% \reset@sup\mk@scripts#3_/} \makeatother % \slash \makeatletter \newbox\slashbox \setbox\slashbox=\hbox{$/$} \def\itex@pslash#1{\setbox\@tempboxa=\hbox{$#1$} \@tempdima=0.5\wd\slashbox \advance\@tempdima 0.5\wd\@tempboxa \copy\slashbox \kern-\@tempdima \box\@tempboxa} \def\slash{\protect\itex@pslash} \makeatother % math-mode versions of \rlap, etc % from Alexander Perlis, "A complement to \smash, \llap, and lap" % http://math.arizona.edu/~aprl/publications/mathclap/ \def\clap#1{\hbox to 0pt{\hss#1\hss}} \def\mathllap{\mathpalette\mathllapinternal} \def\mathrlap{\mathpalette\mathrlapinternal} \def\mathclap{\mathpalette\mathclapinternal} \def\mathllapinternal#1#2{\llap{$\mathsurround=0pt#1{#2}$}} \def\mathrlapinternal#1#2{\rlap{$\mathsurround=0pt#1{#2}$}} \def\mathclapinternal#1#2{\clap{$\mathsurround=0pt#1{#2}$}} % Renames \sqrt as \oldsqrt and redefine root to result in \sqrt[#1]{#2} \let\oldroot\root \def\root#1#2{\oldroot #1 \of{#2}} \renewcommand{\sqrt}[2][]{\oldroot #1 \of{#2}} % Manually declare the txfonts symbolsC font \DeclareSymbolFont{symbolsC}{U}{txsyc}{m}{n} \SetSymbolFont{symbolsC}{bold}{U}{txsyc}{bx}{n} \DeclareFontSubstitution{U}{txsyc}{m}{n} % Manually declare the stmaryrd font \DeclareSymbolFont{stmry}{U}{stmry}{m}{n} \SetSymbolFont{stmry}{bold}{U}{stmry}{b}{n} % Manually declare the MnSymbolE font \DeclareFontFamily{OMX}{MnSymbolE}{} \DeclareSymbolFont{mnomx}{OMX}{MnSymbolE}{m}{n} \SetSymbolFont{mnomx}{bold}{OMX}{MnSymbolE}{b}{n} \DeclareFontShape{OMX}{MnSymbolE}{m}{n}{ <-6> MnSymbolE5 <6-7> MnSymbolE6 <7-8> MnSymbolE7 <8-9> MnSymbolE8 <9-10> MnSymbolE9 <10-12> MnSymbolE10 <12-> MnSymbolE12}{} % Declare specific arrows from txfonts without loading the full package \makeatletter \def\re@DeclareMathSymbol#1#2#3#4{% \let#1=\undefined \DeclareMathSymbol{#1}{#2}{#3}{#4}} \re@DeclareMathSymbol{\neArrow}{\mathrel}{symbolsC}{116} \re@DeclareMathSymbol{\neArr}{\mathrel}{symbolsC}{116} \re@DeclareMathSymbol{\seArrow}{\mathrel}{symbolsC}{117} \re@DeclareMathSymbol{\seArr}{\mathrel}{symbolsC}{117} \re@DeclareMathSymbol{\nwArrow}{\mathrel}{symbolsC}{118} \re@DeclareMathSymbol{\nwArr}{\mathrel}{symbolsC}{118} \re@DeclareMathSymbol{\swArrow}{\mathrel}{symbolsC}{119} \re@DeclareMathSymbol{\swArr}{\mathrel}{symbolsC}{119} \re@DeclareMathSymbol{\nequiv}{\mathrel}{symbolsC}{46} \re@DeclareMathSymbol{\Perp}{\mathrel}{symbolsC}{121} \re@DeclareMathSymbol{\Vbar}{\mathrel}{symbolsC}{121} \re@DeclareMathSymbol{\sslash}{\mathrel}{stmry}{12} \re@DeclareMathSymbol{\bigsqcap}{\mathop}{stmry}{"64} \re@DeclareMathSymbol{\biginterleave}{\mathop}{stmry}{"6} \re@DeclareMathSymbol{\invamp}{\mathrel}{symbolsC}{77} \re@DeclareMathSymbol{\parr}{\mathrel}{symbolsC}{77} \makeatother % \llangle, \rrangle, \lmoustache and \rmoustache from MnSymbolE \makeatletter \def\Decl@Mn@Delim#1#2#3#4{% \if\relax\noexpand#1% \let#1\undefined \fi \DeclareMathDelimiter{#1}{#2}{#3}{#4}{#3}{#4}} \def\Decl@Mn@Open#1#2#3{\Decl@Mn@Delim{#1}{\mathopen}{#2}{#3}} \def\Decl@Mn@Close#1#2#3{\Decl@Mn@Delim{#1}{\mathclose}{#2}{#3}} \Decl@Mn@Open{\llangle}{mnomx}{'164} \Decl@Mn@Close{\rrangle}{mnomx}{'171} \Decl@Mn@Open{\lmoustache}{mnomx}{'245} \Decl@Mn@Close{\rmoustache}{mnomx}{'244} \makeatother % Widecheck \makeatletter \DeclareRobustCommand\widecheck[1]{{\mathpalette\@widecheck{#1}}} \def\@widecheck#1#2{% \setbox\z@\hbox{\m@th$#1#2$}% \setbox\tw@\hbox{\m@th$#1% \widehat{% \vrule\@width\z@\@height\ht\z@ \vrule\@height\z@\@width\wd\z@}$}% \dp\tw@-\ht\z@ \@tempdima\ht\z@ \advance\@tempdima2\ht\tw@ \divide\@tempdima\thr@@ \setbox\tw@\hbox{% \raise\@tempdima\hbox{\scalebox{1}[-1]{\lower\@tempdima\box \tw@}}}% {\ooalign{\box\tw@ \cr \box\z@}}} \makeatother % \mathraisebox{voffset}[height][depth]{something} \makeatletter \NewDocumentCommand\mathraisebox{moom}{% \IfNoValueTF{#2}{\def\@temp##1##2{\raisebox{#1}{$\m@th##1##2$}}}{% \IfNoValueTF{#3}{\def\@temp##1##2{\raisebox{#1}[#2]{$\m@th##1##2$}}% }{\def\@temp##1##2{\raisebox{#1}[#2][#3]{$\m@th##1##2$}}}}% \mathpalette\@temp{#4}} \makeatletter % udots (taken from yhmath) \makeatletter \def\udots{\mathinner{\mkern2mu\raise\p@\hbox{.} \mkern2mu\raise4\p@\hbox{.}\mkern1mu \raise7\p@\vbox{\kern7\p@\hbox{.}}\mkern1mu}} \makeatother %% Fix array \newcommand{\itexarray}[1]{\begin{matrix}#1\end{matrix}} %% \itexnum is a noop \newcommand{\itexnum}[1]{#1} %% Renaming existing commands \newcommand{\underoverset}[3]{\underset{#1}{\overset{#2}{#3}}} \newcommand{\widevec}{\overrightarrow} \newcommand{\darr}{\downarrow} \newcommand{\nearr}{\nearrow} \newcommand{\nwarr}{\nwarrow} \newcommand{\searr}{\searrow} \newcommand{\swarr}{\swarrow} \newcommand{\curvearrowbotright}{\curvearrowright} \newcommand{\uparr}{\uparrow} \newcommand{\downuparrow}{\updownarrow} \newcommand{\duparr}{\updownarrow} \newcommand{\updarr}{\updownarrow} \newcommand{\gt}{>} \newcommand{\lt}{<} \newcommand{\map}{\mapsto} \newcommand{\embedsin}{\hookrightarrow} \newcommand{\Alpha}{A} \newcommand{\Beta}{B} \newcommand{\Zeta}{Z} \newcommand{\Eta}{H} \newcommand{\Iota}{I} \newcommand{\Kappa}{K} \newcommand{\Mu}{M} \newcommand{\Nu}{N} \newcommand{\Rho}{P} \newcommand{\Tau}{T} \newcommand{\Upsi}{\Upsilon} \newcommand{\omicron}{o} \newcommand{\lang}{\langle} \newcommand{\rang}{\rangle} \newcommand{\Union}{\bigcup} \newcommand{\Intersection}{\bigcap} \newcommand{\Oplus}{\bigoplus} \newcommand{\Otimes}{\bigotimes} \newcommand{\Wedge}{\bigwedge} \newcommand{\Vee}{\bigvee} \newcommand{\coproduct}{\coprod} \newcommand{\product}{\prod} \newcommand{\closure}{\overline} \newcommand{\integral}{\int} \newcommand{\doubleintegral}{\iint} \newcommand{\tripleintegral}{\iiint} \newcommand{\quadrupleintegral}{\iiiint} \newcommand{\conint}{\oint} \newcommand{\contourintegral}{\oint} \newcommand{\infinity}{\infty} \newcommand{\bottom}{\bot} \newcommand{\minusb}{\boxminus} \newcommand{\plusb}{\boxplus} \newcommand{\timesb}{\boxtimes} \newcommand{\intersection}{\cap} \newcommand{\union}{\cup} \newcommand{\Del}{\nabla} \newcommand{\odash}{\circleddash} \newcommand{\negspace}{\!} \newcommand{\widebar}{\overline} \newcommand{\textsize}{\normalsize} \renewcommand{\scriptsize}{\scriptstyle} \newcommand{\scriptscriptsize}{\scriptscriptstyle} \newcommand{\mathfr}{\mathfrak} \newcommand{\statusline}[2]{#2} \newcommand{\tooltip}[2]{#2} \newcommand{\toggle}[2]{#2} % Theorem Environments \theoremstyle{plain} \newtheorem{theorem}{Theorem} \newtheorem{lemma}{Lemma} \newtheorem{prop}{Proposition} \newtheorem{cor}{Corollary} \newtheorem*{utheorem}{Theorem} \newtheorem*{ulemma}{Lemma} \newtheorem*{uprop}{Proposition} \newtheorem*{ucor}{Corollary} \theoremstyle{definition} \newtheorem{defn}{Definition} \newtheorem{example}{Example} \newtheorem*{udefn}{Definition} \newtheorem*{uexample}{Example} \theoremstyle{remark} \newtheorem{remark}{Remark} \newtheorem{note}{Note} \newtheorem*{uremark}{Remark} \newtheorem*{unote}{Note} %------------------------------------------------------------------- \begin{document} %------------------------------------------------------------------- \section*{shape theory} \hypertarget{context}{}\subsubsection*{{Context}}\label{context} \hypertarget{topology}{}\paragraph*{{Topology}}\label{topology} [[!include topology - contents]] \hypertarget{homotopy_theory}{}\paragraph*{{Homotopy theory}}\label{homotopy_theory} [[!include homotopy - contents]] \hypertarget{contents}{}\section*{{Contents}}\label{contents} \noindent\hyperlink{motivation}{Motivation}\dotfill \pageref*{motivation} \linebreak \noindent\hyperlink{idea}{Idea}\dotfill \pageref*{idea} \linebreak \noindent\hyperlink{history}{History}\dotfill \pageref*{history} \linebreak \noindent\hyperlink{borsuks_shape_theory_k_borsuk_1968}{Borsuk's shape theory (K. Borsuk, (1968))}\dotfill \pageref*{borsuks_shape_theory_k_borsuk_1968} \linebreak \noindent\hyperlink{anrsystems_approach_mardei_and_segal_1970}{ANR-systems approach (Marde\v{s}i and Segal (1970))}\dotfill \pageref*{anrsystems_approach_mardei_and_segal_1970} \linebreak \noindent\hyperlink{abstract_shape_category}{Abstract shape category}\dotfill \pageref*{abstract_shape_category} \linebreak \noindent\hyperlink{idea_2}{Idea}\dotfill \pageref*{idea_2} \linebreak \noindent\hyperlink{definition}{Definition}\dotfill \pageref*{definition} \linebreak \noindent\hyperlink{examples}{Examples}\dotfill \pageref*{examples} \linebreak \noindent\hyperlink{prospaces_in_a_shape_context}{Pro-spaces in a shape context}\dotfill \pageref*{prospaces_in_a_shape_context} \linebreak \noindent\hyperlink{profinite_groups}{Profinite groups}\dotfill \pageref*{profinite_groups} \linebreak \noindent\hyperlink{ForTopSpaces}{Shape theory for topological spaces}\dotfill \pageref*{ForTopSpaces} \linebreak \noindent\hyperlink{definition_2}{Definition}\dotfill \pageref*{definition_2} \linebreak \noindent\hyperlink{strong_shape_in_terms_of_sheaves_on_a_space}{Strong shape in terms of $(\infty,1)$-sheaves on a space}\dotfill \pageref*{strong_shape_in_terms_of_sheaves_on_a_space} \linebreak \noindent\hyperlink{applications_of_shape_theory}{Applications of Shape Theory}\dotfill \pageref*{applications_of_shape_theory} \linebreak \noindent\hyperlink{geometric_topology}{Geometric Topology}\dotfill \pageref*{geometric_topology} \linebreak \noindent\hyperlink{dynamical_systems}{Dynamical Systems}\dotfill \pageref*{dynamical_systems} \linebreak \noindent\hyperlink{related_concepts}{Related concepts}\dotfill \pageref*{related_concepts} \linebreak \noindent\hyperlink{references}{References}\dotfill \pageref*{references} \linebreak \hypertarget{motivation}{}\subsection*{{Motivation}}\label{motivation} While the idea of a [[homotopy type]] is very suitable for the study of (locally) good [[topological space]]s, the [[weak homotopy type]] fails to give useful information for `bad' spaces, of which classical examples include the [[Warsaw Circle]], \href{http://en.wikipedia.org/wiki/Sierpinski_triangle}{Sierpinski gasket}, \href{http://en.wikipedia.org/wiki/Solenoid_%28mathematics%29}{p-adic solenoid} and so on. Even if our initial and principal interest is more often than not in good spaces, bad spaces arise naturally in their study. For example, in the study of dynamical systems on manifolds, an important issue is the study of the attractors of such systems, which are typically fractal sets, and thus not `locally nice' at all! The intuitive idea of shape theory is to define invariants of quite general topological spaces by approximating them with `good' spaces, either by embedding them into good spaces, and looking at open or polyhedral neighborhoods of them, or by considering abstract inverse systems of good spaces. The two approaches are closely related. \hypertarget{idea}{}\subsection*{{Idea}}\label{idea} If there are few maps from polyhedra (e.g. from spheres) into the space, then the [[weak homotopy type]] may tell too little about the space. Therefore one ``expands'' the space into a successive system of spaces which are good recipients of maps from polyhedra (e.g. ANR-s, polyhedra) and one adapts the homotopy theory to such expansions. The analogue of (strong) homotopy type in this setting is the shape of a space; the shape is an invariant of the strong homotopy type and agrees with it on the ANR-s for metric spaces and on the polyhedra. It is more crude for other spaces, but more suitable than the weak homotopy type, or more exactly gives complementary information. Instead of embedding a space, one may abstractly expand or resolve the space or its homotopy class into a pro-object in a category of nice spaces. [[Strong shape theory]] is a variant which is closer to the usual kind of homotopy, is more geometric and has more homotopy theoretic constructions available in its `toolkit'. It differs by passing to the homotopy category at a later stage in the theory, so one gets homotopy coherent approximating systems rather than homotopy commutative ones. \hypertarget{history}{}\subsection*{{History}}\label{history} Shape theory was first explicitly introduced by Polish mathematician \href{http://www-groups.dcs.st-and.ac.uk/~history/Biographies/Borsuk.html}{Karol Borsuk} in the 1960s, although Christie, a student of Lefshetz, had done some initial development work on the same basic idea much earlier. One of the modern versions of shape theory is developed in terms of inverse systems of absolute neighbourhood retracts (ANRs) (which are [[pro-object]]s in the homotopy category of polyhedra). These were introduced in this setting by [[Sibe Mardesic|S. Mardešić]], and [[Jack Segal|J. Segal]] (1971) and independently, in a slightly different form, by [[Tim Porter]] (thesis, 1971), using the more combinatorial framework of [[pro-objects]] in the category of simplicial sets. This latter approach also indicated the possible link with the \'e{}tale homotopy theory of Artin and Mazur, (Springer Lecture Notes 100). Shape theory is a `[[Cech methods|ech homotopy theory]]', having a similar relationship to ech homology as homotopy theory, based on the singular complex construction, has to singular homology. In fact, as mentioned above, the origins of both shape theory and strong shape theory go back than further Borsuk's initial papers to work by \href{http://www-groups.dcs.st-and.ac.uk/~history/Mathematicians/Lefschetz.html}{Lefshetz} and his student, D. Christie (thesis plus article, D.E. Christie, \emph{Net homotopy for compacta}, \href{www.ams.org/journals/tran/1944-056-00/home.html}{Trans. Amer. Math. Soc., 56 (1944) 275--308}). Christie considered a 2-truncated form of strong shape theory, categorically this corresponds to a lax or op-lax 2-categorical version of shape theory. Although many of the initial ideas were developed by Christie, the paper went unnoticed until Borsuk developed his slightly different approach in the late 1960s. For many applications one needs more refined invariants which build up [[strong shape theory]], while sometimes more crude versions may be useful, for example the recent theory of [[coarse shape]]. Strong Shape Theory developed in the 1970s through the work of Edwards and Hastings (lecture notes, see below), Porter, Quigley, and others. It has, especially in the approach pioneered by Edwards and Hastings, strong links to [[proper homotopy theory]]. The links are a form of duality related to some of the more geometric duality theorems of classical cohomology. M. Batanin further elucidated strong shape theory from a categorical and 2-categorical point of view, but his approach is as yet not much used. His 1997 paper, shows the connections between this theory and a homotopy theory of simplicial [[distributor|distributors]] linked to $A_{\infty}$-categories. The structure of the [[strong shape theory]] of compact spaces is related to certain structure and constructions on the corresponding (commutative) $C^*$-algebras of functions. These are related to the algebraic K-theory of such commutative $C^*$-algebras. Extensions to non-commutative $C^*$-algebras have been made; see (\hyperlink{Blackadar}{Blackadar}) and (\hyperlink{Dadarlat}{Dadarkat}) below, for a start. As shape theory is a [[Čech methods|Čech homotopy theory]], its corresponding homology is Čech homology, but what is the corresponding construction for strong shape? The answer is Steenrod--Sitnikov homology. This is discussed in Marde\v{s}i`s book, \emph{Strong Shape and Homology}, (see below). Many of the themes of homotopy coherence and related ideas occur in this theory and this suggests an infinity categorical approach (closely related to Batanin's) may be important. This seems to be emerging with interpretations of work by Toen and Vezzosi, and by Lurie, and perhaps suggests a review of Batanin's work from that new viewpoint. \hypertarget{borsuks_shape_theory_k_borsuk_1968}{}\subsection*{{Borsuk's shape theory (K. Borsuk, (1968))}}\label{borsuks_shape_theory_k_borsuk_1968} This was the original form and applies to compact metric spaces. It uses the fact that any compact metric space can be embedded in the [[Hilbert Cube]]. For any such embedded compact metric spaces, $X$ and $Y$, one considers \textbf{shape maps} from the collection of open neighbourhoods of $X$ to those of $Y$. These shape maps are families of continuous maps satisfying a compatibility relationship ` up to homotopy'. These compose nicely and form the Borsuk shape category. Two spaces have the same shape if they are isomorphic in this category. Full details of the definition of such shape morphisms are given in the separate entry, [[Borsuk shape theory]]. A remarkable and beautiful theorem of Chapman (the Chapman complement theorem) shows that the shape of two compact metric spaces, $X$ and $Y$ embedded in the [[Hilbert cube|pseudo-interior]] of the Hilbert cube, $Q$, have the same shape if and only if their complements $Q\setminus X$ and $Q\setminus Y$ are homeomorphic. \hypertarget{anrsystems_approach_mardei_and_segal_1970}{}\subsection*{{ANR-systems approach (Marde\v{s}i and Segal (1970))}}\label{anrsystems_approach_mardei_and_segal_1970} \hypertarget{abstract_shape_category}{}\subsection*{{Abstract shape category}}\label{abstract_shape_category} \hypertarget{idea_2}{}\subsubsection*{{Idea}}\label{idea_2} The idea of abstract shape theory is very simple. You have a category, $C$, of objects that you want to study. (In Borsuk's classical topological case this was the (homotopy) category of compact metric spaces.) You have a well behaved set of methods that work well for some subcategory, $D$, of those objects (polyhedra in Borsuk's case, where the methods were those of homotopy theory). The categorical idea that can be glimpsed behind the topological constructions of topological shape theory is that of replacing an object $X$ of $C$ with approximations to $X$ by objects of $D$, (so `approximating' a compact metric space by polyhedra, for instance). Categorically this replaces the object $X$ by the [[comma category]], $(X/D)$, which comes with a projection functor to $D$, which `records' the approximating $D$-object for each approximation. You then use your invariants for objects in $D$ to define (and study) the more general objects in $C$. This does not come without consequences as you obtain new types of maps, (shape maps) between the objects of $C$, namely functors between the comma categories that respect the projections. The objects of $C$ together with your new shape maps form the shape category of your situation. \hypertarget{definition}{}\subsubsection*{{Definition}}\label{definition} The \textbf{shape category} $Shape(C,D)$ is associated to a pair $(C,D)$ of a category $C$ and a [[dense subcategory]] $D$. Here \emph{dense subcategory} is used in the second sense of that term: for every object $X$ in $C$ there is its $D$-expansion, which is the object $\bar{X}$ in the category $pro D$ of [[pro-object]]s in $D$ that is universal ([[initial object|initial]]) with the property that it is equipped with a morphism $X\to\bar{X}$ in $pro D$. The shape category $Shape(C,D)$ has \begin{itemize}% \item the same objects as $C$ \item its morphisms are equivalence classes of maps between the $D$-expansions. \end{itemize} A more [[categorical shape theory|categorical form of shape theory]] was studied by Deleanu and Hilton in a series of papers in the 1970s. They consider a more general setting of a functor $K : D \to C$, which in the classical Borsuk case would be the inclusion of the homotopy category of compact [[simplicial complex|polyhedra]] into that of all compact [[metric space]]s. This was developed further by Bourn and Cordier, and a strong shape version was then found by Batanin. \hypertarget{examples}{}\subsubsection*{{Examples}}\label{examples} \hypertarget{prospaces_in_a_shape_context}{}\paragraph*{{Pro-spaces in a shape context}}\label{prospaces_in_a_shape_context} The classical application of shape theoretic idea is to the study of [[topological space]]s that do not have the [[homotopy type]] of a [[CW-complex]]. This is the case obtained from the above general setup by choosing \begin{itemize}% \item $C =$ [[HoTop]]${}_{he}$ the [[homotopy category]] of the category [[Top]] of all [[topological space]]s localised at the \textbf{[[homotopy equivalence]]s}; \item $D = Ho(CW Cplx)$ the full [[subcategory]] given by [[CW-complex]]es. \end{itemize} More on this is in the section \href{ForTopSpaces}{Shape theory for topological spaces} below and in [[Cech homotopy]]. \hypertarget{profinite_groups}{}\paragraph*{{Profinite groups}}\label{profinite_groups} Consider the category $C =$[[Grp]] of groups and its subcategory $D$ of finite group. A shape map between two groups is a map between their [[profinite completion of a group|profinite completion]]s. This sort of behaviour is quite general as this form of abstract shape theory is related to equational completions; see \begin{itemize}% \item Gildenhuys and Kennison, \emph{Equational completions, model induced triples and pro-objects}, J. Pure Applied Algebra, 4 (1971) 317-346. \end{itemize} This aspect is explored reasonably fully in the book by Cordier and Porter (see below). A different terminology and slightly different emphasis is often used within the shape theoretic literature as it corresponds more to the geometric intuition needed there, deriving originally from the important classical motivation of Borsuk, [[Sibe Mardesic|Mardešić]], and [[J. Segal|Segal]]. \hypertarget{ForTopSpaces}{}\subsection*{{Shape theory for topological spaces}}\label{ForTopSpaces} \hypertarget{definition_2}{}\subsubsection*{{Definition}}\label{definition_2} \ldots{} \hypertarget{strong_shape_in_terms_of_sheaves_on_a_space}{}\subsubsection*{{Strong shape in terms of $(\infty,1)$-sheaves on a space}}\label{strong_shape_in_terms_of_sheaves_on_a_space} There is a way to study the [[strong shape theory]] of a [[topological space]] $X$ in terms of [[∞-stack]]s on $X$, i.e. in terms of the [[(∞,1)-category of (∞,1)-sheaves]] $Sh_{(\infty,1)}(X) := Sh_{(\infty,1)}(Op(X))$ on the [[category of open subsets]] of $X$. This is described in \begin{itemize}% \item [[Bertrand Toen]] and [[Gabriele Vezzosi]], \emph{Segal topoi and stacks over Segal categories} in Proceedings of the Program \emph{Stacks, Intersection theory and Non-abelian Hodge Theory} , MSRI, Berkeley, January-May 2002 (\href{http://arxiv.org/abs/math/0212330}{arXiv:math/0212330}) \end{itemize} and in section 7.1.6 of \begin{itemize}% \item [[Jacob Lurie]], \emph{[[Higher Topos Theory]]} \end{itemize} For more details see [[shape of an (infinity,1)-topos]]. This theory fits into the general picture above of a subcategory $D\subset C$, where now $C$ is the $(\infty,1)$-category of $(\infty,1)$-toposes, while $D$ is the category of $\infty$-groupoids, regarded as their presheaf $(\infty,1)$-toposes. Thus, the ``shape'' of an $(\infty,1)$-topos $X$ is the functor $Hom(X,-)\colon \infty Gpd \to \infty Gpd$. Alternately, since a [[geometric morphism]] from an $(\infty,1)$-topos $X$ into presheaves on an $\infty$-groupoid $K$ is the same as a [[global section]] of the [[constant ∞-stack]] $L Const(K)$ over $X$, we can also describe this functor as the composite \begin{displaymath} \infty Grpd \xrightarrow{LConst} Sh_{(\infty,1)}(X) \xrightarrow{\Gamma} \infty Grpd \,. \end{displaymath} Thus, we can equivalently describe the shape of $X$ by mapping out of it into topological spaces \emph{over} $X$ that are at least fiberwise nice topological spaces: in other words, to look at $\infty$-[[covering space]]s over $X$. Now, for a [[small category|small]] [[(∞,1)-category]] $C$, a functor $C \to \infty Grpd$ that preserves finite limits may be thought of as a [[pro-object]] in $C$. Now $\infty Gpd$ is not small, but one may hope that the functors $Shape(X)\colon \infty Gpd \to \infty Gpd$ arising in this way are determined by a small amount of data, and thus give honest pro-$\infty$-groupoids. We can, if we wish, define for the nonce \begin{displaymath} Pro(\infty Grpd) \subset Func(\infty Grpd, \infty Grpd)^{op} \end{displaymath} to be the fully subcategory of [[(∞,1)-functor]]s that preserve finite limits, although as discussed above this is not quite correct. We call the objects in $Pro(\infty Grpd)$ \textbf{pro-spaces} or \textbf{shapes}. Notice that by the [[homotopy hypothesis]]-theorem, we can think here of $\infty Grpd \simeq Top_{cg,wH}$ as the category of [[nice topological space]]s, considered up to [[homotopy equivalence]]. The first description of shapes makes it obviously functorial in [[geometric morphisms]] of $(\infty,1)$-toposes. This can be seen from the second definition as well: given $(f^* \dashv f_*) \colon \mathbf{H} \to \mathbf{K}$, the [[unit of an adjunction|unit]] $Id_{\mathbf{K}} \to f_* \circ f^*$ induces a transformation \begin{displaymath} \Gamma_{\mathbf{K}}\circ LConst_{\mathbf{K}} \to \Gamma_{\mathbf{K}} \circ f_* \circ f^* \circ LConst_{\mathbf{K}} \simeq \Gamma_{\mathbf{H}}\circ LConst_{\mathbf{H}} \end{displaymath} that may be regarded as a morphism of shapes \begin{displaymath} Shape(f) : Shape(\mathbf{K}) \to Shape(\mathbf{H}) \,. \end{displaymath} We say the geometric morphism $f$ is a \textbf{shape invariance} if $Shape(f)$ is an equivalence of pro-spaces. \begin{uprop} For $f : X \to Y$ a continuous map of [[paracompact space]]s, the induced geometric morphism $(f^* \dashv f*) : Sh_{(\infty,1)}(X) \to Sh_{(\infty,1)}(Y)$ is a shape equivalence, precisely if for each [[CW-complex]] $K$ the map \begin{displaymath} Top(Y,K) \to Top(X,K) \end{displaymath} is an equivalence. \end{uprop} \begin{proof} This is [[Higher Topos Theory|HTT, prop. 7.1.6.8]]. \end{proof} \hypertarget{applications_of_shape_theory}{}\subsection*{{Applications of Shape Theory}}\label{applications_of_shape_theory} \hypertarget{geometric_topology}{}\subsubsection*{{Geometric Topology}}\label{geometric_topology} \hypertarget{dynamical_systems}{}\subsubsection*{{Dynamical Systems}}\label{dynamical_systems} In a [[dynamical system]], the [[attractor]]s are rarely polyhedra and their homotopy properties correspond more nearly to shape theoretic ones than to standard homotopy theoretic ones. This seems first to have been studied by [[Hastings]] in 1988, (see references) and more recently has been explored in papers by [[José Sanjurjo]] and his coworkers, see below. Adapting this idea [[Luis Javier Hernandez|Hernandez]], [[Teresa Rivas]] and [[José García Calcines]] have been using ideas developed for [[proper homotopy theory]] and shape involving [[pro-spaces]], to describe limiting properties of dynamical systems. \hypertarget{related_concepts}{}\subsection*{{Related concepts}}\label{related_concepts} \begin{itemize}% \item [[topology]] \item [[shape]], [[shape modality]], [[shape of an (infinity,1)-topos]] \item [[strong shape theory]], [[Borsuk's shape theory]] \item [[geometric realization]] \end{itemize} \hypertarget{references}{}\subsection*{{References}}\label{references} See also $n$lab entries [[shape fibration]], [[approximate fibration]], \ldots{} and references The original references for the shape theory of metric compacta are: \begin{itemize}% \item [[K. Borsuk]], \emph{Concerning homotopy properties of compacta}, Fund Math. 62 (1968) 223-254 \item [[K. Borsuk]], \emph{Theory of Shape}, Monografie Matematyczne Tom 59,Warszawa 1975. \end{itemize} A generalization in categorical approach is given in \begin{itemize}% \item W. Holsztyski, \emph{An extension and axiomatic characterization of Borsuk's theory of shape}, Fund. Math. 70 (1971) no. 2, 157--168 \href{https://www.impan.pl/shop/en/publication/transaction/download/product/79189}{pdf} \end{itemize} The `ANR-systems' approach of Marde\v{s}i and Segal appeared a bit later in \begin{itemize}% \item [[Sibe Mardesic|S. Mardešić]], J. Segal, \emph{Shapes of compacta and ANR-systems, Fund. Math. 72 (1971) 41-59,} \end{itemize} and is fully developed in \begin{itemize}% \item [[Sibe Mardesic|S. Mardešić]], J. Segal, \emph{Shape theory}, North Holland, 1982. \end{itemize} The more or less equivalent pro-object approach was independently developed by Porter in \begin{itemize}% \item [[Tim Porter|T. Porter]], \emph{ech homotopy I}, Jour. London Math. Soc., 1, 6, 1973, pp. 429-436 \href{https://dx.doi.org/10.1112/jlms/s2-6.3.429}{doi} \item [[Tim Porter|T. Porter]], \emph{ech homotopy II}, Jour. London Math. Soc., 2, 6, 1973, pp. 667-675 \href{https://dx.doi.org/10.1112/jlms/s2-6.4.667}{doi} \end{itemize} References relating more to strong shape theory include: \begin{itemize}% \item D.A. Edwards and H. M. Hastings, (1976), ech and Steenrod homotopy theories with applications to geometric topology, Lecture Notes in Maths. 542, Springer-Verlag, \href{http://www.math.uga.edu/~davide/Cech_and_Steenrod_Homotopy_Theories_with_Applications_to_Geometric_Topology.pdf}{pdf} \item J.T. Lisica and [[Sibe Mardesic|S. Mardešić]], Coherent prohomotopy and strong shape theory, Glasnik Mat. 19(39) (1984) 335--399. \item [[Sibe Mardesic|S. Mardešić]], \emph{Strong shape and homology}, Springer monographs in mathematics, Springer-Verlag. \item [[Michael Batanin]], \href{http://www.numdam.org/numdam-bin/fitem?id=CTGDC_1997__38_1_3_0}{Categorical strong shape theory}, Cahiers Topologie G\'e{}om. Diff\'e{}rentielle Cat\'e{}g. 38 (1997), no. 1, 3--66. \item [[T. Porter]], \emph{Stability Results for Topological Spaces}, Math. Zeit. 150, 1974, pp. 1-21. \item [[T. Porter]], \emph{Abstract homotopy theory in procategories}, Cahiers Top. G\'e{}om. Diff., 17, 1976, pp. 113-124, \href{http://archive.numdam.org/article/CTGDC_1976__17_2_113_0.pdf}{numdam} \item [[T. Porter]], \emph{Coherent prohomotopical algebra}, \href{http://archive.numdam.org/article/CTGDC_1977__18_2_139_0.pdf}{numdam}, Cahiers Top. G\'e{}om. Diff. \textbf{18}, (1978) pp. 139-179; \item [[T. Porter]], \emph{Coherent prohomotopy theory}, Cahiers Top. G\'e{}om. Diff. \textbf{19}, (1978) pp. 3-46, \href{http://archive.numdam.org/article/CTGDC_1978__19_1_3_0.pdf}{numdam}. \end{itemize} These last three papers developed a version of the [[BrownAHT]] to pro-categories of simplicial sets and of chain complexes, so as to give [[strong shape theory]] a better foundation and toolbox of homotopical methods. These methods were complementary to those of Edwards and Hastings, (listed above), who used a Quillen model category structure on the pro-category. References to the categorical forms of shape theory include \begin{itemize}% \item A. Deleanu, P.J. Hilton, \emph{On the categorical shape of a functor}, Fund. Math. 97 (1977) 157 - 176. \item A. Deleanu, P.J. Hilton, \emph{Borsuk's shape and Grothendieck categories of pro-objects}, Math. Proc. Camb. Phil. Soc. 79 (1976) 473-482. \item D. Bourn, [[Jean-Marc Cordier|J.-M. Cordier]], \emph{Distributeurs et th\'e{}orie de la forme}, Cahiers Topologie G\'e{}om. Diff\'e{}rentielle Cat\'e{}g. 21,(1980), no. 2, 161--188, \href{http://www.numdam.org/numdam-bin/feuilleter?id=CTGDC_1980__21_2}{numdam}. \end{itemize} and \begin{itemize}% \item [[Jean-Marc Cordier|J.-M. Cordier]] and [[Tim Porter|T. Porter]], (1989), Shape Theory: Categorical Methods of Approximation, Mathematics and its Applications, Ellis Horwood. Reprinted Dover (2008), \end{itemize} which explores categorical methods in the area. The relationship between invariants of $C^*$-algebras and the shape of their spectra was explored in \begin{itemize}% \item [[Bruce Blackadar]], \emph{Shape theory for $C^*$-algebras}, Math. Scand. 56 (1985) 249 - 275, \href{http://www.mscand.dk/article.php?id=2767}{journal link}. \end{itemize} The links are with K-theory and Kasparov's theory. This connection and a related one to `asymptotic morphisms' is explored in some neat notes by Anderson and Grodal: \begin{itemize}% \item \href{http://www.math.ku.dk/~jg/papers/etheory.html}{Noncommutative topology - homotopy functors and E-theory} \end{itemize} That connection with [[asymptotic morphisms]] is fully explored in the work of [[Marius Dadarlat|Dadarlat]]; see his papers, \begin{itemize}% \item [[Marius Dadarlat|Marius Dādārlat]], \emph{Shape theory and asymptotic morphisms for C$^\ast$-algebras}, Duke Math. J. 73(3):687-711, 1994, \href{http://www.ams.org/mathscinet-getitem?mr=1262931}{MR95c:46117}, \href{http://dx.doi.org/10.1215/S0012-7094-94-07327-4}{doi} \end{itemize} \begin{itemize}% \item [[Marius Dadarlat|Marius Dādārlat]], Terry A. Loring, \emph{Deformations of topological spaces predicted by E-theory}, in Algebraic methods in operator theory, pages 316-327. Birkh\"a{}user 1994. \end{itemize} For links with dynamical systems see the early paper \begin{itemize}% \item [[H. M. Hastings]], \emph{Shape theory and dynamical systems} in M.G.Markely and W.Perizzo: The structure of attractors in dynamical systems, Lect. Notes in Math. 688 (1978) 150-160. Springer-Verlag. \end{itemize} and more recently \begin{itemize}% \item [[Joel W. Robbin]], Dietmar A. Salamon, \emph{Dynamical systems, shape theory and the Conley index}, Ergodic Theory Dynam. Systems 8 (1988) 375 - 393, \item A. Giraldo, M. A. Mor\'o{}n, F. R. Ruiz del Portal, [[J. M. R. Sanjurjo]], \emph{Shape of global attractors in topological spaces}, Nonlinear Analysis 60 (2005) 837 - 847 \href{https://dx.doi.org/10.1016/j.na.2004.03.036}{doi} \item J. J. S\'a{}nchez-Gabites, [[J. M. R. Sanjurjo|José M. R. Sanjurjo]], \emph{Shape properties of the boundary of attractors}, Glas. Mat. Ser. III 42(62) (2007), no. 1, 117--130 \item J. Garc\'i{}a Calcines, [[Luis Javier Hernández|L. J. Hernández]] and [[Teresa Rivas|M.T. Rivas]], \emph{Limit and end functors of dynamical systems via exterior spaces,} \href{http://www.unirioja.es/cu/luhernan/puben.html}{Preprint (2011)}. \end{itemize} [[!redirects shape of a topological space]] \end{document}