词条 | Glossary of algebraic topology |
释义 |
This is a glossary of properties and concepts in algebraic topology in mathematics. See also: glossary of topology, list of algebraic topology topics, glossary of category theory, glossary of differential geometry and topology, Timeline of manifolds.
!$@{{glossary}}{{term|*}}{{defn|1=The base point of a based space.}}{{term|}}{{defn|1=For an unbased space X, X+ is the based space obtained by adjoining a disjoint base point.}}{{glossary end}}A{{glossary}}{{term|absolute neighborhood retract}}{{term|abstract}}{{defn|no=1|Abstract homotopy theory}}{{term|Adams}}{{defn|no=1|1=John Frank Adams.}}{{defn|no=2|1=The Adams spectral sequence.}}{{defn|no=3|1=The Adams conjecture.}}{{defn|no=4|1=The Adams e-invariant.}}{{defn|no=5|1=The Adams operations.}}{{term|Alexander duality}}{{term|Alexander trick}}{{defn|The Alexander trick produces a section of the restriction map , Top denoting a homeomorphism group; namely, the section is given by sending a homeomorphism to the homeomorphism. This section is in fact a homotopy inverse.[1]}} {{term|Analysis Situs}}{{term|aspherical space}}{{term|assembly map}}{{term|Atiyah}}{{defn|no=1|1=Michael Atiyah.}}{{defn|no=2|1=Atiyah duality.}}{{defn|no=3|1=The Atiyah–Hirzebruch spectral sequence.}}{{glossary end}}B{{glossary}}{{term|bar construction}}{{term|based space}}{{defn|1=A pair (X, x0) consisting of a space X and a point x0 in X.}}{{term|Betti number}}{{term|Bockstein homomorphism}}{{term|Borel–Moore homology}}{{term|Borsuk's theorem}}{{term|Bott}}{{defn|no=1|Raoul Bott.}}{{defn|no=2|The Bott periodicity theorem for unitary groups say: .}}{{defn|no=3|The Bott periodicity theorem for orthogonal groups say: .}}{{term|Brouwer fixed point theorem}}{{defn|1=The Brouwer fixed-point theorem says that any map has a fixed point.}}{{glossary end}}C{{glossary}}{{term|cap product}}{{term|Čech cohomology}}{{term|cellular}}{{defn|no=1|A map ƒ:X→Y between CW complexes is cellular if for all n.}}{{defn|no=2|The cellular approximation theorem says that every map between CW complexes is homotopic to a cellular map between them.}}{{defn|no=3|The cellular homology is the (canonical) homology of a CW complex. Note it applies to CW complexes and not to spaces in general. A cellular homology is highly computable; it is especially useful for spaces with natural cell decompositions like projective spaces or Grassmannian.}}{{term|chain homotopy}}{{defn|1=Given chain maps between chain complexes of modules, a chain homotopy s from f to g is a sequence of module homomorphisms satisfying .}}{{term|chain map}}{{defn|1=A chain map between chain complexes of modules is a sequence of module homomorphisms that commutes with the differentials; i.e., .}}{{term|chain homotopy equivalence}}{{defn|1=A chain map that is an isomorphism up to chain homotopy; that is, if ƒ:C→D is a chain map, then it is a chain homotopy equivalence if there is a chain map g:D→C such that gƒ and ƒg are chain homotopic to the identity homomorphisms on C and D, respectively.}}{{term|change of fiber}}{{defn|The change of fiber of a fibration p is a homotopy equivalence, up to homotopy, between the fibers of p induced by a path in the base.}}{{term|character variety}}{{defn|1=The character variety[2] of a group π and an algebraic group G (e.g., a reductive complex Lie group) is the geometric invariant theory quotient by G:.}}{{term|characteristic class}}{{defn|1=Let Vect(X) be the set of isomorphism classes of vector bundles on X. We can view as a contravariant functor from Top to Set by sending a map ƒ:X → Y to the pullback ƒ* along it. Then a characteristic class is a natural transformation from Vect to the cohomology functor H*. Explicitly, to each vector bundle E we assign a cohomology class, say, c(E). The assignment is natural in the sense that ƒ*c(E) = c(ƒ*E).}}{{term|chromatic homotopy theory}}{{defn|1=chromatic homotopy theory.}}{{term|class}}{{defn|no=1|Chern class.}}{{defn|no=2|Stiefel–Whitney class.}}{{term|classifying space}}{{defn|1=Loosely speaking, a classifying space is a space representing some contravariant functor defined on the category of spaces; for example, is the classifying space in the sense is the functor that sends a space to the set of isomorphism classes of real vector bundles on the space.}}{{term|clutching}}{{term|cobar spectral sequence}}{{term|cobordism}}{{defn|no=1|1=See cobordism.}}{{defn|no=2|1=A cobordism ring is a ring whose elements are cobordism classes.}}{{defn|no=3|See also h-cobordism theorem, s-cobordism theorem.}}{{term|coefficient ring}}{{defn|1=If E is a ring spectrum, then the coefficient ring of it is the ring .}}{{term|cofiber sequence}}{{defn|1=A cofiber sequence is any sequence that is equivalent to the sequence for some ƒ where is the reduced mapping cone of ƒ (called the cofiber of ƒ).}}{{term|cofibrant approximation}}{{term|cofibration}}{{defn|1=A map is a cofibration if it satisfies the property: given and homotopy such that , there is a homotopy such that .[3] A cofibration is injective and is a homeomorphism onto its image.}}{{term|coherent homotopy}}{{term|cohomotopy group}}{{defn|1=For a based space X, the set of homotopy classes is called the n-th cohomotopy group of X.}}{{term|cohomology operation}}{{term|completion}}{{term|complex bordism}}{{term|complex-oriented}}{{defn|1=A multiplicative cohomology theory E is complex-oriented if the restriction map E2(CP∞) → E2(CP1) is surjective.}}{{term|cone}}{{defn|1=The cone over a space X is . The reduced cone is obtained from the reduced cylinder by collapsing the top.}}{{term|connective}}{{defn|A spectrum E is connective if for all negative integers q.}}{{term|configuration space}}{{term|1=constant}}{{defn|1=A constant sheaf on a space X is a sheaf on X such that for some set A and some map , the natural map is bijective for any x in X.}}{{term|contractible space}}{{defn|1=A space is contractible if the identity map on the space is homotopic to the constant map.}}{{term|covering}}{{defn|no=1|A map p: Y → X is a covering or a covering map if each point of x has a neighborhood N that is evenly covered by p; this means that the pre-image of N is a disjoint union of open sets, each of which maps to N homeomorphically.}}{{defn|no=2|It is n-sheeted if each fiber p−1(x) has exactly n elements.}}{{defn|no=3|It is universal if Y is simply connected.}}{{defn|no=4|A morphism of a covering is a map over X. In particular, an automorphism of a covering p:Y→X (also called a deck transformation) is a map Y→Y over X that has inverse; i.e., a homeomorphism over X.}}{{defn|no=5|A G-covering is a covering arising from a group action on a space X by a group G, the covering map being the quotient map from X to the orbit space X/G. The notion is used to state the universal property: if X admits a universal covering (in particular connected), then is the set of isomorphism classes of G-coverings. In particular, if G is abelian, then the left-hand side is (cf. nonabelian cohomology.)}}{{term|cup product}}{{term|CW complex}}{{defn|1=A CW complex is a space X equipped with a CW structure; i.e., a filtration such that (1) X0 is discrete and (2) Xn is obtained from Xn-1 by attaching n-cells.}}{{term|cyclic homology}}{{glossary end}} D{{glossary}}{{term|deck transformation}}{{defn|Another term for an automorphism of a covering.}}{{term|delooping}}{{term|degeneracy cycle}}{{term|degree}}{{glossary end}}E{{glossary}}{{term|Eckmann–Hilton argument}}{{defn|1=The Eckmann–Hilton argument.}}{{term|Eckmann–Hilton duality}}{{term|Eilenberg–MacLane spaces}}{{defn|1=Given an abelian group π, the Eilenberg–MacLane spaces are characterized by.}}{{term|Eilenberg–Steenrod axioms}}{{defn|1=The Eilenberg–Steenrod axioms are the set of axioms that any cohomology theory (singular, cellular, etc.) must satisfy. Weakening the axioms (namely dropping the dimension axiom) leads to a generalized cohomology theory.}}{{term|Eilenberg–Zilber theorem}}{{term|1=E_n-algebra|2=En-algebra}}{{term|equivariant algebraic topology}}{{defn|1=Equivariant algebraic topoloy is the study of spaces with (continuous) group action.}}{{term|exact}}{{defn|1=A sequence of pointed sets is exact if the image of f coincides with the pre-image of the chosen point of Z.}}{{term|excision}}{{defn|1=The excision axiom for homology says: if and , then for each q, is an isomorphism.}}{{term|excisive pair/triad}}{{glossary end}} F{{glossary}}{{term|factorization homology}}{{term|fiber-homotopy equivalence}}{{defn|1=Given D→B, E→B, a map ƒ:D→E over B is a fiber-homotopy equivalence if it is invertible up to homotopy over B. The basic fact is that if D→B, E→B are fibrations, then a homotopy equivalence from D to E is a fiber-homotopy equivalence.}}{{term|fibration}}{{defn|1=A map p:E → B is a fibration if for any given homotopy and a map such that , there exists a homotopy such that . (The above property is called the homotopy lifting property.) A covering map is a basic example of a fibration.}}{{term|fibration sequence}}{{defn|1=One says is a fibration sequence to mean that p is a fibration and that F is homotopy equivalent to the homotopy fiber of p, with some understanding of base points.}}{{term|finitely dominated}}{{term|fundamental class}}{{term|fundamental group}}{{defn|1=The fundamental group of a space X with base point x0 is the group of homotopy classes of loops at x0. It is precisely the first homotopy group of (X, x0) and is thus denoted by .}}{{term|fundamental groupoid}}{{defn|1=The fundamental groupoid of a space X is the category whose objects are the points of X and whose morphisms x → y are the homotopy classes of paths from x to y; thus, the set of all morphisms from an object x0 to itself is, by definition, the fundament group .}}{{term|free}}{{defn|1=Synonymous with unbased. For example, the free path space of a space X refers to the space of all maps from I to X; i.e., while the path space of a based space X consists of such map that preserve the base point (i.e., 0 goes to the base point of X).}}{{term|Freudenthal suspension theorem}}{{defn|1=For a nondegenerately based space X, the Freudenthal suspension theorem says: if X is (n-1)-connected, then the suspension homomorphismis bijective for q < 2n - 1 and is surjective if q = 2n - 1.}} {{glossary end}}G{{glossary}}{{term|G-fibration}}{{defn|1=A G-fibration with some topological monoid G. An example is Moore's path space fibration.}}{{term|Γ-space}}{{term|generalized cohomology theory}}{{defn|1=A generalized cohomology theory is a contravariant functor from the category of pairs of spaces to the category of abelian groups that satisfies all of the Eilenberg–Steenrod axioms except the dimension axiom.}}{{term|genus}}{{term|group completion}}{{term|grouplike}}{{defn|1=An H-space X is said to be group-like or grouplike if is a group; i.e., X satisfies the group axioms up to homotopy.}}{{term|Gysin sequence}}{{glossary end}}H{{glossary}}{{term|Hilton–Milnor theorem}}{{defn|1=The Hilton–Milnor theorem.}}{{term|H-space}}{{defn|1=An H-space is a based space that is a unital magma up to homotopy.}}{{term|homologus}}{{defn|1=Two cycles are homologus if they belong to the same homology class.}}{{term|homotopy category}}{{defn|1=Let C be a subcategory of the category of all spaces. Then the homotopy category of C is the category whose class of objects is the same as the class of objects of C but the set of morphisms from an object x to an object y is the set of the homotopy classes of morphisms from x to y in C. For example, a map is a homotopy equivalence if and only if it is an isomorphism in the homotopy category.}}{{term|homotopy colimit}}{{term|homotopy over a space B}}{{defn|A homotopy ht such that for each fixed t, ht is a map over B.}}{{term|homotopy equivalence}}{{defn|no=1|A map ƒ:X→Y is a homotopy equivalence if it is invertible up to homotopy; that is, there exists a map g: Y→X such that g ∘ ƒ is homotopic to th identity map on X and ƒ ∘ g is homotopic to the identity map on Y.}}{{defn|no=2|Two spaces are said to be homotopy equivalent if there is a homotopy equivalence between the two. For example, by definition, a space is contractible if it is homotopy equivalent to a point space.}}{{term|homotopy excision theorem}}{{defn|1=The homotopy excision theorem is a substitute for the failure of excision for homotopy groups.}}{{term|homotopy fiber}}{{defn|1=The homotopy fiber of a based map ƒ:X→Y, denoted by Fƒ, is the pullback of along f.}}{{term|homotopy fiber product}}{{defn|1=A fiber product is a particular kind of a limit. Replacing this limit lim with a homotopy limit holim yields a homotopy fiber product.}}{{term|homotopy group}}{{defn|no=1|For a based space X, let , the set of homotopy classes of based maps. Then is the set of path-connected components of X, is the fundamental group of X and are the (higher) n-th homotopy groups of X.}}{{defn|no=2|For based spaces , the relative homotopy group is defined as of the space of paths that all start at the base point of X and end somewhere in A. Equivalently, it is the of the homotopy fiber of .}}{{defn|no=3|If E is a spectrum, then }}{{defn|no=4|If X is a based space, then the stable k-th homotopy group of X is . In other words, it is the k-th homotopy group of the suspension spectrum of X.}}{{term|homotopy quotient}}{{defn|1=If G is a Lie group acting on a manifold X, then the quotient space is called the homotopy quotient (or Borel construction) of X by G, where EG is the universal bundle of G.}}{{term|homotopy spectral sequence}}{{term|homotopy sphere}}{{term|Hopf}}{{defn|no=1|1=Heinz Hopf.}}{{defn|no=2|1=Hopf invariant.}}{{defn|no=3|1=The Hopf index theorem.}}{{defn|no=4|1=Hopf construction.}}{{term|Hurewicz}}{{defn|1=The Hurewicz theorem establishes a relationship between homotopy groups and homology groups.}}{{glossary end}}I{{glossary}}{{term|infinite loop space}}{{term|infinite loop space machine}}{{term|infinite mapping telescope}}{{term|integration along the fiber}}{{term|isotopy}}{{glossary end}}J{{glossary}}{{term|J-homomorphism}}{{defn|See J-homomorphism.}}{{term|join}}{{defn|The join of based spaces X, Y is }}{{glossary end}}K{{glossary}}{{term|k-invariant}}{{term|Kan complex}}{{defn|See Kan complex.}}{{term|Kervaire invariant}}{{defn|1=The Kervaire invariant.}}{{term|Koszul duality}}{{defn|1=Koszul duality.}}{{term|Künneth formula}}{{glossary end}}L{{glossary}}{{term|Lazard ring}}{{defn|1=The Lazard ring L is the (huge) commutative ring together with the formal group law ƒ that is universal among all the formal group laws in the sense that any formal group law g over a commutative ring R is obtained via a ring homomorphism L → R mapping ƒ to g. According to Quillen's theorem, it is also the coefficient ring of the complex bordism MU. The Spec of L is called the moduli space of formal group laws.}}{{term|Lefschetz fixed point theorem}}{{defn|1=The Lefschetz fixed point theorem says: given a finite simplicial complex K and its geometric realization X, if a map has no fixed point, then the Lefschetz number of f; that is,is zero. For example, it implies the Brouwer fixed-point theorem since the Lefschetz number of is, as higher homologies vanish, one.}} {{term|lens space}}{{defn|1=The lens space is the quotient space where is the group of p-th roots of unity acting on the unit sphere by .}}{{term|Leray spectral sequence}}{{term|local coefficient}}{{defn|no=1|1=A module over the group ring for some based space B; in other words, an abelian group together with a homomorphism .}}{{defn|no=2|1=The local coefficient system over a based space B with an abelian group A is a fiber bundle over B with discrete fiber A. If B admits a universal covering , then this meaning coincides with that of 1. in the sense: every local coefficient system over B can be given as the associated bundle .}}{{term|local sphere}}{{defn|1=The localization of a sphere at some prime number}}{{term|localization}}{{term|locally constant sheaf}}{{defn|1=A locally constant sheaf on a space X is a sheaf such that each point of X has an open neighborhood on which the sheaf is constant.}}{{term|loop space}}{{defn|The loop space of a based space X is the space of all loops starting and ending at the base point of X.}}{{glossary end}}M{{glossary}}{{term|Madsen–Weiss theorem}}{{term|mapping}}{{defn|no=1|1=The mapping cone (or cofiber) of a map ƒ:X→Y is .}}{{defn|no=2|1=The mapping cylinder of a map ƒ:X→Y is . Note: .}}{{defn|no=3|1=The reduced versions of the above are obtained by using reduced cone and reduced cylinder.}}{{defn|no=4|1=The mapping path space Pp of a map p:E→B is the pullback of along p. If p is fibration, then the natural map E→Pp is a fiber-homotopy equivalence; thus, roughly speaking, one can replace E by the mapping path space without changing the homotopy type of the fiber.}}{{term|Mayer–Vietoris sequence}}{{term|model category}}{{defn|1=A presentation of an ∞-category.[4] See also model category.}}{{term|Moore space}}{{term|multiplicative}}{{defn|1=A generalized cohomology theory E is multiplicative if E*(X) is a graded ring. For example, the ordinary cohomology theory and the complex K-theory are multiplicative (in fact, cohomology theories defined by E∞-rings are multiplicative.) }}{{glossary end}}N{{glossary}}{{term|n-cell}}{{defn|1=Another term for an n-disk.}}{{term|n-connected}}{{defn|1=A based space X is n-connected if for all integers q ≤ n. For example, "1-connected" is the same thing as "simply connected".}}{{term|n-equivalent}}{{term|NDR-pair}}{{defn|1=A pair of spaces is said to be an NDR-pair (=neighborhood deformation retract pair) if there is a map and a homotopy such that , , and .If A is a closed subspace of X, then the pair is an NDR-pair if and only if is a cofibration. }}{{term|nilpotent}}{{defn|no=1|1=nilpotent space; for example, a simply connected space is nilpotent.}}{{defn|no=2|1=The nilpotent theorem.}}{{term|normalized}}{{defn|1=Given a simplicial group G, the normalized chain complex NG of G is given by with the n-th differential given by ; intuitively, one throws out degenerate chains.[5] It is also called the Moore complex.}}{{glossary end}}O{{glossary}}{{term|obstruction cocycle}}{{term|obstruction theory}}{{defn|1=Obstruction theory is the collection of constructions and calculations indicating when some map on a submanifold (subcomplex) can or cannot be extended to the full manifold. These typically involve the Postnikov tower, killing homotopy groups, obstruction cocycles, etc.}}{{term|of finite type}}{{defn|1=A CW complex is of finite type if there are only finitely many cells in each dimension.}}{{term|operad}}{{defn|1=The portmanteau of “operations” and “monad”. See operad.}}{{term|orbit category}}{{term|orientation}}{{defn|no=1|1=The orientation covering (or orientation double cover) of a manifold is a two-sheeted covering so that each fiber over x corresponds to two different ways of orienting a neighborhood of x.}}{{defn|no=2|1=An orientation of a manifold is a section of an orientation covering; i.e., a consistent choice of a point in each fiber.}}{{defn|no=3|1=An orientation character (also called the first Stiefel–Whitney class) is a group homomorphism that corresponds to an orientation covering of a manifold X (cf. #covering.)}}{{defn|no=4|1=See also orientation of a vector bundle as well as orientation sheaf.}}{{glossary end}}P{{glossary}}{{term|p-adic homotopy theory}}{{defn|1=The p-adic homotopy theory.}}{{term|path class}}{{defn|An equivalence class of paths (two paths are equivalent if they are homotopic to each other).}}{{term|path lifting}}{{defn|1=A path lifting function for a map p: E → B is a section of where is the mapping path space of p. For example, a covering is a fibration with a unique path lifting function. By formal consideration, a map is a fibration if and only if there is a path lifting function for it.}}{{term|path space}}{{defn|1=The path space of a based space X is , the space of based maps, where the base point of I is 0. Put in another way, it is the (set-theoretic) fiber of over the base point of X. The projection is called the path space fibration, whose fiber over the base point of X is the loop space . See also mapping path space.}}{{term|phantom map}}{{term|Poincaré}}{{defn|1=The Poincaré duality theorem says: given a manifold M of dimension n and an abelian group A, there is a natural isomorphism.}}{{term|Pontrjagin–Thom construction}}{{term|Postnikov system}}{{defn|1=A Postnikov system is a sequence of fibrations, such that all preceding manifolds have vanishing homotopy groups below a given dimension.}}{{term|principal fibration}}{{defn|1=Usually synonymous with G-fibration.}}{{term|profinite}}{{defn|1=profinite homotopy theory; it studies profinite spaces.}}{{term|properly discontinuous}}{{defn|Not particularly a precise term. But it could mean, for example, that G is discrete and each point of the G-space has a neighborhood V such that for each g in G that is not the identity element, gV intersects V at finitely many points.}}{{term|pullback}}{{defn|1=Given a map p:E→B, the pullback of p along ƒ:X→B is the space (succinctly it is the equalizer of p and f). It is a space over X through a projection.}}{{term|Puppe sequence}}{{defn|1=The Puppe sequence refers ro either of the sequences where are homotopy cofiber and homotopy fiber of f.}}{{term|pushout}}{{defn|1=Given and a map , the pushout of X and B along f is ; that is X and B are glued together along A through f. The map f is usually called the attaching map. The important example is when B = Dn, A = Sn-1; in that case, forming such a pushout is called attaching an n-cell (meaning an n-disk) to X.}}{{glossary end}} Q{{glossary}}{{term|quasi-fibration}}{{defn|1=A quasi-fibration is a map such that the fibers are homotopy equivalent to each other.}}{{term|Quillen}}{{defn|no=1|1=Daniel Quillen}}{{defn|no=2|1=Quillen’s theorem says that is the Lazard ring.}}{{glossary end}}R{{glossary}}{{term|rational}}{{defn|no=1|1=The rational homotopy theory.}}{{defn|no=2|1=The rationalization of a space X is, roughly, the localization of X at zero. More precisely, X0 together with j: X → X0 is a rationalization of X if the map induced by j is an isomorphism of vector spaces and .}}{{defn|no=3|1=The rational homotopy type of X is the weak homotopy type of X0.}}{{term|Reidemeister}}{{defn|1=Reidemeister torsion.}}{{term|reduced}}{{defn|1=The reduced suspension of a based space X is the smash product . It is related to the loop functor by where is the loop space.}}{{term|ring spectrum}}{{defn|1=A ring spectrum is a spectrum that satisfying the ring axioms, either on nose or up to homotopy. For example, a complex K-theory is a ring spectrum.}}{{glossary end}}S{{glossary}}{{term|Samelson product}}{{term|Serre}}{{defn|no=1|1=Jean-Pierre Serre.}}{{defn|no=2|1=Serre class.}}{{defn|no=3|1=Serre spectral sequence.}}{{term|simple}}{{term|simple-homotopy equivalence}}{{defn|A map ƒ:X→Y between finite simplicial complexes (e.g., manifolds) is a simple-homotopy equivalence if it is homotopic to a composition of finitely many elementary expansions and elementary collapses. A homotopy equivalence is a simple-homotopy equivalence if and only if its Whitehead torsion vanishes.}}{{term|simplicial approximation}}{{defn|1=See simplicial approximation theorem.}}{{term|simplicial complex}}{{defn|1=See simplicial complex; the basic example is a triangulation of a manifold.}}{{term|simplicial homology}}{{defn|1=A simplicial homology is the (canonical) homology of a simplicial complex. Note it applies to simplicial complexes and not to spaces; cf. #singular homology.}}{{term|signature invariant}}{{term|singular}}{{defn|no=1|1=Given a space X and an abelian group π, the singular homology group of X with coefficients in π iswhere is the singular chain complex of X; i.e., the n-th degree piece is the free abelian group generated by all the maps from the standard n-simplex to X. A singular homology is a special case of a simplicial homology; indeed, for each space X, there is the singular simplicial complex of X [6] whose homology is the singular homology of X.}} {{defn|no=2|The singular simplices functor is the functor from the category of all spaces to the category of simplicial sets, that is the right adjoint to the geometric realization functor.}}{{defn|no=3|The singular simplicial complex of a space X is the normalized chain complex of the singular simplex of X.}}{{term|slant product}}{{term|small object argument}}{{term|smash product}}{{defn|1=The smash product of based spaces X, Y is . It is characterized by the adjoint relation.}}{{term|Spanier–Whitehead}}{{defn|1=The Spanier–Whitehead duality.}}{{term|spectrum}}{{defn|1=Roughly a sequence of spaces together with the maps (called the structure maps) between the consecutive terms; see spectrum (topology).}}{{term|sphere bundle}}{{defn|1=A sphere bundle is a fiber bundle whose fibers are spheres.}}{{term|sphere spectrum}}{{defn|The sphere spectrum is a spectrum consisting of a sequence of spheres together with the maps between the spheres given by suspensions. In short, it is the suspension spectrum of .}}{{term|stable homotopy group}}{{defn|1=See #homotopy group.}}{{term|Steenrod homology}}{{defn|1=Steenrod homology.}}{{term|Steenrod operation}}{{term|Sullivan}}{{defn|no=1|1=Dennis Sullivan.}}{{defn|no=2|1=The Sullivan conjecture.}}{{defn|no=3|1={{citation| title=Infinitesimal computations in topology|year=1977|url=http://www.numdam.org/item?id=PMIHES_1977__47__269_0}} - introduces rational homotopy theory (along with Quillen's paper).}}{{defn|no=4|The Sullivan algebra in the rational homotopy theory.}}{{term|suspension spectrum}}{{defn|The suspension spectrum of a based space X is the spectrum given by .}}{{term|symmetric spectrum}}{{defn|1=See symmetric spectrum.}}{{glossary end}} T{{glossary}}{{term|Thom}}{{defn|no=1|1=René Thom.}}{{defn|no=2|1=If E is a vector bundle on a paracompact space X, then the Thom space of E is obtained by first replacing each fiber by its compactification and then collapsing the base X.}}{{defn|no=3|1=The Thom isomorphism says: for each orientable vector bundle E of rank n on a manifold X, a choice of an orientation (the Thom class of E) induces an isomorphism.}}{{term|topological chiral homology}}{{term|transfer}}{{term|transgression}}{{glossary end}} U{{glossary}}{{term|universal coefficient}}{{defn|1=The universal coefficient theorem.}}{{term|up to homotopy}}{{defn|1=A statement holds in the homotopy category as opposed to the category of spaces.}}{{glossary end}}V{{glossary}}{{term|van Kampen}}{{defn|1=The van Kampen theorem says: if a space X is path-connected and if x0 is a point in X, thenwhere the colimit runs over some open cover of X consisting of path-connected open subsets containing x0 such that the cover is closed under finite intersections.}} {{glossary end}}W{{glossary}}{{term|Waldhausen S-construction}}{{defn|1=Waldhausen S-construction.}}{{term|Wall's finiteness obstruction}}{{term|weak equivalence}}{{defn|1=A map ƒ:X→Y of based spaces is a weak equivalence if for each q, the induced map is bijective.}}{{term|wedge}}{{defn|1=For based spaces X, Y, the wedge product of X and Y is the coproduct of X and Y; concretely, it is obtained by taking their disjoint union and then identifying the respective base points.}}{{term|well pointed}}{{defn|1=A based space is well pointed (or non-degenerately based) if the inclusion of the base point is a cofibration.}}{{term|Whitehead}}{{defn|no=1|J. H. C. Whitehead.}}{{defn|no=2|Whitehead's theorem says that for CW complexes, the homotopy equivalence is the same thing as the weak equivalence.}}{{defn|no=3|Whitehead group.}}{{defn|no=4|Whitehead product.}}{{term|winding number}}{{glossary end}}Notes1. ^Let r, s denote the restriction and the section. For each f in , define . Then . 2. ^Despite the name, it may not be an algebraic variety in the strict sense; for example, it may not be irreducible. Also, without some finiteness assumption on G, it is only a scheme. 3. ^{{harvnb|Hatcher|loc=Ch. 4. H.}} 4. ^http://mathoverflow.net/questions/2185/how-to-think-about-model-categories 5. ^https://ncatlab.org/nlab/show/Moore+complex 6. ^http://ncatlab.org/nlab/show/singular+simplicial+complex References
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2 : Algebraic topology|Glossaries of mathematics |
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