360:
43:
1273:
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2722:
112:
4371:, and a Cartesian product of charts is a chart for the product manifold. Thus, an atlas for the product manifold can be constructed using atlases for its factors. If these atlases define a differential structure on the factors, the corresponding atlas defines a differential structure on the product manifold. The same is true for any other structure defined on the factors. If one of the factors has a boundary, the product manifold also has a boundary. Cartesian products may be used to construct tori and finite
2399:. It is not generally possible to describe a manifold with just one chart, because the global structure of the manifold is different from the simple structure of the charts. For example, no single flat map can represent the entire Earth without separation of adjacent features across the map's boundaries or duplication of coverage. When a manifold is constructed from multiple overlapping charts, the regions where they overlap carry information essential to understanding the global structure.
1903:, possibly with additional structure. A manifold can be constructed by giving a collection of coordinate charts, that is, a covering by open sets with homeomorphisms to a Euclidean space, and patching functions: homeomorphisms from one region of Euclidean space to another region if they correspond to the same part of the manifold in two different coordinate charts. A manifold can be given additional structure if the patching functions satisfy axioms beyond continuity. For instance,
6518:. Gluing the circles together will produce a new, closed manifold without boundary, the Klein bottle. Closing the surface does nothing to improve the lack of orientability, it merely removes the boundary. Thus, the Klein bottle is a closed surface with no distinction between inside and outside. In three-dimensional space, a Klein bottle's surface must pass through itself. Building a Klein bottle which is not self-intersecting requires four or more dimensions of space.
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open, so that it could unroll to become a rectangle, but keep a grasp on the cut ends. Twist one end 180°, making the inner surface face out, and glue the ends back together seamlessly. This results in a strip with a permanent half-twist: the Möbius strip. Its boundary is no longer a pair of circles, but (topologically) a single circle; and what was once its "inside" has merged with its "outside", so that it now has only a
6476:
4391:
100:
6446:, a chart causes its piece of the manifold to itself acquire a sense of ordering, which in 3-dimensions can be viewed as either right-handed or left-handed. Overlapping charts are not required to agree in their sense of ordering, which gives manifolds an important freedom. For some manifolds, like the sphere, charts can be chosen so that overlapping regions agree on their "handedness"; these are
1678:, so neither chart alone is sufficient to cover the whole circle. It can be proved that it is not possible to cover the full circle with a single chart. For example, although it is possible to construct a circle from a single line interval by overlapping and "gluing" the ends, this does not produce a chart; a portion of the circle will be mapped to both ends at once, losing invertibility.
1259:
6556:) to mathematically merge each antipode pair into a single point. The closed surface so produced is the real projective plane, yet another non-orientable surface. It has a number of equivalent descriptions and constructions, but this route explains its name: all the points on any given line through the origin project to the same "point" on this "plane".
6568:, or "number of handles" present in a surface. A torus is a sphere with one handle, a double torus is a sphere with two handles, and so on. Indeed, it is possible to fully characterize compact, two-dimensional manifolds on the basis of genus and orientability. In higher-dimensional manifolds genus is replaced by the notion of
6533:
6262:
Orientable surfaces can be visualized, and their diffeomorphism classes enumerated, by genus. Given two orientable surfaces, one can determine if they are diffeomorphic by computing their respective genera and comparing: they are diffeomorphic if and only if the genera are equal, so the genus forms a
5727:
All differentiable manifolds (of constant dimension) can be given the structure of a
Riemannian manifold. The Euclidean space itself carries a natural structure of Riemannian manifold (the tangent spaces are naturally identified with the Euclidean space itself and carry the standard scalar product of
4340:
between the two boundaries. Two points are identified when they are mapped onto each other. For a topological manifold, this bijection should be a homeomorphism, otherwise the result will not be a topological manifold. Similarly, for a differentiable manifold, it has to be a diffeomorphism. For other
663:
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algebraic varieties over the real or complex numbers are manifolds. One generalizes this first by allowing singularities, secondly by allowing different fields, and thirdly by emulating the patching construction of manifolds: just as a manifold is glued together from open subsets of
Euclidean space,
3975:
of points which are mapped to each other by transition maps. Charts map equivalence classes to points of a single patch. There are usually strong demands on the consistency of the transition maps. For topological manifolds they are required to be homeomorphisms; if they are also diffeomorphisms, the
3967:
A manifold can be constructed by gluing together pieces in a consistent manner, making them into overlapping charts. This construction is possible for any manifold and hence it is often used as a characterisation, especially for differentiable and
Riemannian manifolds. It focuses on an atlas, as the
1049:
6270:
This is much harder in higher dimensions: higher-dimensional manifolds cannot be directly visualized (though visual intuition is useful in understanding them), nor can their diffeomorphism classes be enumerated, nor can one in general determine if two different descriptions of a higher-dimensional
1865:
However, excluded are examples like two touching circles that share a point to form a figure-8; at the shared point, a satisfactory chart cannot be created. Even with the bending allowed by topology, the vicinity of the shared point looks like a "+", not a line. A "+" is not homeomorphic to a line
6489:
Begin with an infinite circular cylinder standing vertically, a manifold without boundary. Slice across it high and low to produce two circular boundaries, and the cylindrical strip between them. This is an orientable manifold with boundary, upon which "surgery" will be performed. Slice the strip
5401:. By definition, all manifolds are topological manifolds, so the phrase "topological manifold" is usually used to emphasize that a manifold lacks additional structure, or that only its topological properties are being considered. Formally, a topological manifold is a topological space
2549:
Charts in an atlas may overlap and a single point of a manifold may be represented in several charts. If two charts overlap, parts of them represent the same region of the manifold, just as a map of Europe and a map of Russia may both contain Moscow. Given two overlapping charts, a
2212:
5452:
manifold looks locally like a
Euclidean space in a rather weak manner: while for each individual chart it is possible to distinguish differentiable functions or measure distances and angles, merely by virtue of being a topological manifold a space does not have any
7016:(top dimensional manifold and codimension 1 boundary) and manifolds with corners (top dimensional manifold, codimension 1 boundary, codimension 2 corners). Whitney stratified spaces are a broad class of spaces, including algebraic varieties, analytic varieties,
7049:
is a space that behaves like a manifold from the point of view of homology theory. These are not all manifolds, but (in high dimension) can be analyzed by surgery theory similarly to manifolds, and failure to be a manifold is a local obstruction, as in surgery
8234:(3rd edition) Publish or Perish Inc. Encyclopedic five-volume series presenting a systematic treatment of the theory of manifolds, Riemannian geometry, classical differential geometry, and numerous other topics at the first- and second-year graduate levels.
1598:
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485:
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2425:, of a manifold is an invertible map between a subset of the manifold and a simple space such that both the map and its inverse preserve the desired structure. For a topological manifold, the simple space is a subset of some Euclidean space
932:
2541:(i.e. an equivalence class containing that given atlas). Unlike an ordinary atlas, the maximal atlas of a given manifold is unique. Though useful for definitions, it is an abstract object and not used directly (e.g. in calculations).
2640:
An atlas can also be used to define additional structure on the manifold. The structure is first defined on each chart separately. If all transition maps are compatible with this structure, the structure transfers to the manifold.
5299:, formulated in the 1970s, provided a far-reaching extension of the Poincaré conjecture to the general three-dimensional manifolds. Four-dimensional manifolds were brought to the forefront of mathematical research in the 1980s by
3814:
6259:. This is a classification in principle: the general question of whether two smooth manifolds are diffeomorphic is not computable in general. Further, specific computations remain difficult, and there are many open questions.
7034:
is a topological space formed by gluing disks of different dimensionality together. In general the resulting space is singular, hence not a manifold. However, they are of central interest in algebraic topology, especially in
5496:
manifold have the same dimension. Some authors require that all charts of a topological manifold map to
Euclidean spaces of same dimension. In that case every topological manifold has a topological invariant, its dimension.
2043:
367:
After a line, a circle is the simplest example of a topological manifold. Topology ignores bending, so a small piece of a circle is treated the same as a small piece of a line. Considering, for instance, the top part of the
4738:), depending on whether the value changes continuously or not. As continuous examples, Riemann refers to not only colors and the locations of objects in space, but also the possible shapes of a spatial figure. Using
2959:
1254:{\displaystyle {\begin{aligned}T(a)&=\chi _{\mathrm {right} }\left(\chi _{\mathrm {top} }^{-1}\left\right)\\&=\chi _{\mathrm {right} }\left(a,{\sqrt {1-a^{2}}}\right)\\&={\sqrt {1-a^{2}}}\end{aligned}}}
5469:
discussed below. In particular, the same underlying topological manifold can have several mutually incompatible classes of differentiable functions and an infinite number of ways to specify distances and angles.
4035:. When a manifold is viewed in this way, it is easy to use intuition from Euclidean spaces to define additional structure. For example, in a Euclidean space, it is always clear whether a vector at some point is
6284:, because, while they may be defined in terms of some presentation (such as the genus in terms of a triangulation), they are the same relative to all possible descriptions of a particular manifold: they are
1361:
5515:, is used. If the local charts on a manifold are compatible in a certain sense, one can define directions, tangent spaces, and differentiable functions on that manifold. In particular it is possible to use
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Two manifolds with boundaries can be glued together along a boundary. If this is done the right way, the result is also a manifold. Similarly, two boundaries of a single manifold can be glued together.
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formalisms of classical mechanics. This space is, in fact, a high-dimensional manifold, whose dimension corresponds to the degrees of freedom of the system and where the points are specified by their
6384:
In dimensions two and higher, a simple but important invariant criterion is the question of whether a manifold admits a meaningful orientation. Consider a topological manifold with charts mapping to
2363:
is locally isomorphic to the sheaf of continuous (or differentiable, or complex-analytic, etc.) functions on
Euclidean space. This definition is mostly used when discussing analytic manifolds in
1484:
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manifolds. For others, this is impossible. The latter possibility is easy to overlook, because any closed surface embedded (without self-intersection) in three-dimensional space is orientable.
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The definition of a manifold can be generalized by dropping the requirement of finite dimensionality. Thus an infinite dimensional manifold is a topological space locally homeomorphic to a
5548:. For smooth manifolds the transition maps are smooth, that is, infinitely differentiable. Analytic manifolds are smooth manifolds with the additional condition that the transition maps are
4123:
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The top, bottom, left, and right charts do not form the only possible atlas. Charts need not be geometric projections, and the number of charts is a matter of choice. Consider the charts
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independently discovered them 100 years later. Their research uncovered two types of spaces whose geometric structures differ from that of classical
Euclidean space; these gave rise to
2534:. An atlas is not unique as all manifolds can be covered in multiple ways using different combinations of charts. Two atlases are said to be equivalent if their union is also an atlas.
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One could hope to develop an arsenal of invariant criteria that would definitively classify all manifolds up to isomorphism. It is known that for manifolds of dimension 4 and higher,
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side. Similarly to the Klein Bottle below, this two dimensional surface would need to intersect itself in two dimensions, but can easily be constructed in three or more dimensions.
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7980:. The most complete account, with historical insights and excellent, but difficult, problems. The standard reference for those wishing to have a deep understanding of the subject.
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As with the circle, one may define one chart that covers the whole sphere excluding one point. Thus two charts are sufficient, but the sphere cannot be covered by a single chart.
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In technical language, a manifold with boundary is a space containing both interior points and boundary points. Every interior point has a neighborhood homeomorphic to the open
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This is the standard way differentiable manifolds are defined. If the transition functions of an atlas for a topological manifold preserve the natural differential structure of
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in which the surface lies. Such a surface would, in modern terminology, be called a manifold; and in modern terms, the theorem proved that the curvature of the surface is an
4344:
A finite cylinder may be constructed as a manifold by starting with a strip Ă and gluing a pair of opposite edges on the boundary by a suitable diffeomorphism. A
272:
because it allows complicated structures to be described in terms of well-understood topological properties of simpler spaces. Manifolds naturally arise as solution sets of
4577:
faces, and in fact, will remain true for any spherical map, even if it does not arise from any convex polytope. Thus 2 is a topological invariant of the sphere, called its
7000:
A "stratified space" is a space that can be divided into pieces ("strata"), with each stratum a manifold, with the strata fitting together in prescribed ways (formally, a
6945:
are likewise glued together from affine schemes, which are a generalization of algebraic varieties. Both are related to manifolds, but are constructed algebraically using
4797:
of a continuously differentiable function is a manifold in the latter sense. He then proposes a new, more general, definition of manifold based on a 'chain of manifolds' (
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with each other, so that the manifold has a well-defined set of functions which are differentiable in each neighborhood, thus differentiable on the manifold as a whole.
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A sphere can be treated in almost the same way as the circle. In mathematics a sphere is just the surface (not the solid interior), which can be defined as a subset of
3427:
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825:
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4597: = 1 face. Thus the Euler characteristic of the torus is 1 â 2 + 1 = 0. The Euler characteristic of other surfaces is a useful
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4486:. Manifold theory has come to focus exclusively on these intrinsic properties (or invariants), while largely ignoring the extrinsic properties of the ambient space.
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in a neighborhood of every point except the points (1, 0) and (â1, 0); and in a neighborhood of those points, it can be thought of as the graph of, respectively,
4252:
It is possible to define different points of a manifold to be the same point. This can be visualized as gluing these points together in a single point, forming a
3599:
2035:
6111:
4046:
The patchwork construction does not use any embedding, but simply views the manifold as a topological space by itself. This abstract point of view is called the
4027:
The first construction and this construction are very similar, but represent rather different points of view. In the first construction, the manifold is seen as
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gave an intrinsic definition for differentiable manifolds in his lecture course on
Riemann surfaces in 1911â1912, opening the road to the general concept of a
4711:
translated as "manifoldness". In his Göttingen inaugural lecture, Riemann described the set of all possible values of a variable with certain constraints as a
3609:
A single manifold can be constructed in different ways, each stressing a different aspect of the manifold, thereby leading to a slightly different viewpoint.
2341:
a pure manifold. Since dimension is a local invariant (i.e. the map sending each point to the dimension of its neighbourhood over which a chart is defined, is
658:{\displaystyle {\begin{aligned}\chi _{\mathrm {bottom} }(x,y)&=x\\\chi _{\mathrm {left} }(x,y)&=y\\\chi _{\mathrm {right} }(x,y)&=y.\end{aligned}}}
2696:
The structure on the manifold depends on the atlas, but sometimes different atlases can be said to give rise to the same structure. Such atlases are called
7636:
5752:
allows the definition of distance but does not require the concept of angle; it is an analytic manifold in which each tangent space is equipped with a
5473:
Usually additional technical assumptions on the topological space are made to exclude pathological cases. It is customary to require that the space be
4256:. There is, however, no reason to expect such quotient spaces to be manifolds. Among the possible quotient spaces that are not necessarily manifolds,
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plane of coordinates. This provides two charts; the four other charts are provided by a similar construction with the two other coordinate planes.
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showed in 1960 that no algorithm exists for classifying four-dimensional manifolds. Important work on higher-dimensional manifolds, including
6802:, by analogy with algebraic geometry or linear algebra. These are of interest both in their own right, and to study the underlying manifold.
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6236:
Different notions of manifolds have different notions of classification and invariant; in this section we focus on smooth closed manifolds.
9139:
2207:{\displaystyle \mathbf {B} ^{n}=\left\{(x_{1},x_{2},\dots ,x_{n})\in \mathbb {R} ^{n}:x_{1}^{2}+x_{2}^{2}+\cdots +x_{n}^{2}<1\right\}.}
5255:
showed that the intrinsic definition in terms of charts was equivalent to
Poincaré's definition in terms of subsets of Euclidean space.
4688:, gives another example where the manifold is nontrivial. Geometrical and topological aspects of classical mechanics were emphasized by
3971:
The manifold is constructed by specifying an atlas, which is itself defined by transition maps. A point of the manifold is therefore an
8426:
6514:
Take two Möbius strips; each has a single loop as a boundary. Straighten out those loops into circles, and let the strips distort into
6325:
Smooth closed manifolds have no local invariants (other than dimension), though geometric manifolds have local invariants, notably the
6299:
417:
8450:
5817:
A Euclidean vector space with the group operation of vector addition is an example of a non-compact Lie group. A simple example of a
5243:
aspects of the subject, and thus intuitions dating back to the latter half of the 19th century became precise, and developed through
2528:
The description of most manifolds requires more than one chart. A specific collection of charts which covers a manifold is called an
4808:
is a precursor to the modern notion of atlas. In particular, he considers two manifolds defined respectively as graphs of functions
9556:
8645:
7174:
5165:. The circle can be represented by a graph in the neighborhood of every point because the left hand side of its defining equation
7307:
5461:
choice of such concepts. In order to discuss such properties for a manifold, one needs to specify further structure and consider
6758:
2387:
The spherical Earth is navigated using flat maps or charts, collected in an atlas. Similarly, a manifold can be described using
1766:
This example is historically significant, as it has motivated the terminology; it became apparent that the whole surface of the
6724:
5279:. Poincaré pioneered the study of three-dimensional manifolds and raised a fundamental question about them, today known as the
3968:
patches naturally provide charts, and since there is no exterior space involved it leads to an intrinsic view of the manifold.
3662:
grew historically from constructions like this. Here is another example, applying this method to the construction of a sphere:
17:
9705:
6252:
5372:
The simplest kind of manifold to define is the topological manifold, which looks locally like some "ordinary" Euclidean space
2313:
of the manifold. Generally manifolds are taken to have a constant local dimension, and the local dimension is then called the
8515:
8249:
8153:
6414:
280:
of functions. The concept has applications in computer-graphics given the need to associate pictures with coordinates (e.g.
8741:
6927:. The singularities correspond to fixed points of the group actions, and the actions must be compatible in a certain sense.
6548:
Begin with a sphere centered on the origin. Every line through the origin pierces the sphere in two opposite points called
6338:
5316:
3858:
4463:. In the modern theory of manifolds, these notions correspond to Riemannian manifolds with constant negative and positive
8794:
8322:
4470:
Carl
Friedrich Gauss may have been the first to consider abstract spaces as mathematical objects in their own right. His
6941:
is glued together from affine algebraic varieties, which are zero sets of polynomials over algebraically closed fields.
5700:(or scalar) product is a typical example of an inner product. This allows one to define various notions such as length,
5488:
of the manifold at a certain point is the dimension of the Euclidean space that the charts at that point map to (number
3629:
Perhaps the simplest way to construct a manifold is the one used in the example above of the circle. First, a subset of
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maps an open subset around an interior point to an open Euclidean subset, while the boundary chart with transition map
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2333:. For example, the (surface of a) sphere has a constant dimension of 2 and is therefore a pure manifold whereas the
57:
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is a two-dimensional manifold that cannot be realized in three dimensions without self-intersection, shown here as
5595:
2836:(sphere plus interior) is a 3-manifold with boundary. Its boundary is a sphere, a 2-manifold. (Do not confuse with
2716:
8826:
8435:
7099:
6846:
6621:. In addition to continuous functions and smooth functions generally, there are maps with special properties. In
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Riemann was the first one to do extensive work generalizing the idea of a surface to higher dimensions. The name
4676:. For an unconstrained movement of free particles the manifold is equivalent to the Euclidean space, but various
6915:" in the topology. Roughly speaking, it is a space which locally looks like the quotients of some simple space (
4523:
1833:, unless the dimension of the manifold is 0. Putting these freedoms together, other examples of manifolds are a
7009:
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5413:
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400:
363:
Figure 1: The four charts each map part of the circle to an open interval, and together cover the whole circle.
6278:
if there is some intrinsic characteristic that differentiates them. Such criteria are commonly referred to as
2321:. However, some authors admit manifolds that are not connected, and where different points can have different
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1593:{\displaystyle {\begin{aligned}x&={\frac {1-s^{2}}{1+s^{2}}}\\y&={\frac {2s}{1+s^{2}}}\end{aligned}}}
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6337:. This distinction between local invariants and no local invariants is a common way to distinguish between
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5734:-spheres, are specified as subspaces of a Euclidean space and inherit a metric from their embedding in it.
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The same formula will hold if we project the vertices and edges of the polytope onto a sphere, creating a
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4050:. It can make it harder to imagine what a tangent vector might be, and there is no intrinsic notion of a
3934:) plane. A similar chart exists for the southern hemisphere. Together with two charts projecting on the (
1947:
excludes spaces such as "the line with two origins" (these generalizations of manifolds are discussed in
381:
191:
4633:
in the first half of 19th century led them to consider special types of complex manifolds, now known as
4217:{\displaystyle \mathbb {R} ^{n}\setminus \{0\}\to \mathbb {R} ^{n}\setminus \{0\}:x\mapsto x/\|x\|^{2}.}
4019:= 0 are not identified with any point on the first and second copy, respectively). This gives a circle.
482:. Similarly, there are charts for the bottom (red), left (blue), and right (green) parts of the circle:
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The dimension of the product manifold is the sum of the dimensions of its factors. Its topology is the
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1971:
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respectively, overlap in their domain: their intersection lies in the quarter of the circle where both
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In Riemannian geometry, one may ask for maps to preserve the Riemannian metric, leading to notions of
6420:
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6125:
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is a generalisation of the idea of a circle (1-sphere) and sphere (2-sphere) to higher dimensions. An
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by closed subsets). There are various technical definitions, notably a Whitney stratified space (see
6893:. Usually one relaxes one or the other condition: manifolds with the point-set axioms are studied in
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The study of manifolds combines many important areas of mathematics: it generalizes concepts such as
4327:
4253:
4226:
This function is its own inverse and thus can be used in both directions. As the transition map is a
2677:), the differential structure transfers to the manifold and turns it into a differentiable manifold.
31:
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on the manifold. Two points are identified if one is moved onto the other by some group element. If
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maps a closed subset around a boundary point to a closed Euclidean subset. The boundary is itself a
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1870:(i.e. pieces), whereas deleting a point from a line segment gives a space with at most two pieces;
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51:
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from the second half of the circle example. Start with two copies of the line. Use the coordinate
3093:{\displaystyle \{(x_{1},x_{2},\dots ,x_{n})\vert \Sigma x_{i}^{2}<1{\text{ and }}x_{1}\geq 0\}}
927:{\displaystyle T:(0,1)\rightarrow (0,1)=\chi _{\mathrm {right} }\circ \chi _{\mathrm {top} }^{-1}}
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is a source of a number of important global invariant properties. Some key criteria include the
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One method of identifying points (gluing them together) is through a right (or left) action of a
3390:. The boundary points can be characterized as those points which land on the boundary hyperplane
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5786:, defining the length of a curve; but it cannot in general be used to define an inner product.
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to a Euclidean space. This means that every point has a neighbourhood for which there exists a
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The sphere is two-dimensional, so each chart will map part of the sphere to an open subset of
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are introduced in an analogous way by requiring that the transition functions of an atlas are
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4754:) as a continuous stack of (nâ1) dimensional manifoldnesses. Riemann's intuitive notion of a
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Grundlagen fĂŒr eine allgemeine Theorie der Functionen einer verĂ€nderlichen complexen Grösse.
4660:. The possible states of a mechanical system are thought to be points of an abstract space,
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4684:. The theory of a rotating solid body, developed in the 18th century by Leonhard Euler and
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Figure 2: A circle manifold chart based on slope, covering all but one point of the circle.
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property and orientability (see below). Indeed, several branches of mathematics, such as
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Manifolds can be equipped with additional structure. One important class of manifolds are
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Bryant, J.; Ferry, S.; Mio, W.; Weinberger, S. (1996). "Topology of homology manifolds".
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5556:). The sphere can be given analytic structure, as can most familiar curves and surfaces.
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For example, the unit circle in the plane can be thought of as the graph of the function
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2014:
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The surface of the Earth requires (at least) two charts to include every point. Here the
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5782:, in a manner which varies smoothly from point to point. This norm can be extended to a
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further contributed to their theory, clarifying the geometric meaning of the process of
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336:
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6154:'Infinite dimensional manifolds': to allow for infinite dimensions, one may consider
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Lie group is the circle: the group operation is simply rotation. This group, known as
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Kervaire, M. (1961). "A Manifold which does not admit any differentiable structure".
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A basic example of maps between manifolds are scalar-valued functions on a manifold,
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function between Euclidean spaces that satisfies the nondegeneracy hypothesis of the
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3972:
3809:{\displaystyle S=\left\{(x,y,z)\in \mathbb {R} ^{3}\mid x^{2}+y^{2}+z^{2}=1\right\}.}
3658:
is identified, and then an atlas covering this subset is constructed. The concept of
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The atlas containing all possible charts consistent with a given atlas is called the
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Calculus on Manifolds: A Modern Approach to Classical Theorems of Advanced Calculus
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over the reals. This omits the point-set axioms, allowing higher cardinalities and
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is a special kind of combinatorial manifold which is defined in digital space. See
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5743:
5300:
5292:
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4368:
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2721:
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1272:
668:
404:
242:
7536: â locally convex vector spaces satisfying a very mild completeness condition
7131:. It is an algebra with respect to the pointwise addition and multiplication. Let
6890:
6163:
2824:(circle plus interior) is a 2-manifold with boundary. Its boundary is a circle, a
2454:
and interest focuses on the topological structure. This structure is preserved by
1618:. These two charts provide a second atlas for the circle, with the transition map
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6552:. Although there is no way to do so physically, it is possible (by considering a
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in a manner which varies smoothly from point to point. Given two tangent vectors
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To measure distances and angles on manifolds, the manifold must be Riemannian. A
5560:
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can be sliced open by its 'parallel' and 'meridian' circles, creating a map with
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is a kind of manifold which is discretization of a manifold. It usually means a
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embedded in our common 3D space, were considered by Riemann under the guise of
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3962:
2674:
2455:
2334:
2325:. If a manifold has a fixed dimension, this can be emphasized by calling it a
2008:
1775:
9762:
5567:
to higher dimensions; however, rectifiable sets are not in general manifolds.
4758:
evolved into what is today formalized as a manifold. Riemannian manifolds and
4425:
Before the modern concept of a manifold there were several important results.
4268:. An example of a quotient space of a manifold that is also a manifold is the
1866:
segment, since deleting the center point from the "+" gives a space with four
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for which the above conditions hold, is called a Sikorski differential space.
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for the second copy. Now, glue both copies together by identifying the point
2273:
1908:
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1830:
411:
7988:
Foundational Essays on Topological Manifolds. Smoothings, and Triangulations
7897:
7880:
3950:) plane, an atlas of six charts is obtained which covers the entire sphere.
2583:
to the manifold and then back to another (or perhaps the same) open ball in
1461:
is the opposite of the slope of the line through the points at coordinates (
9822:
9626:
9611:
9576:
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9409:
9088:
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8925:
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8146:
Knots, Groups, and 3-Manifolds. Papers Dedicated to the Memory of R. H. Fox
7983:
7602:
7560:
Differential-Algebraic Systems: Analytical Aspects and Circuit Applications
6956:, a variety is in general not a manifold, though linguistically the French
6924:
6882:
6573:
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6159:
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5721:
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5344:
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4781:
In the first section of Analysis Situs, Poincaré defines a manifold as the
4602:
4265:
1958:
1829:; thus a line segment without its end points is a manifold. They are never
254:
195:
104:
5324:
3166:. This invariance allows to "define" boundary points; see next paragraph.
667:
Together, these parts cover the whole circle, and the four charts form an
190:
for short, is a topological space with the property that each point has a
9710:
9684:
9606:
9295:
9234:
8931:
8920:
8877:
8778:
8379:
8059:
7474:
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6630:
6617:
Just as there are various types of manifolds, there are various types of
6463:, which must intersect itself in its 3-space representation, and (3) the
6118:
5938:
5899:
5728:
the space). Many familiar curves and surfaces, including for example all
5697:
5511:
For most applications, a special kind of topological manifold, namely, a
5328:
5222:
4661:
4443:
first studied such geometries in 1733, but sought only to disprove them.
4070:
2954:{\displaystyle \{(x_{1},x_{2},\dots ,x_{n})\vert \Sigma x_{i}^{2}<1\}}
2704:
1962:
1846:
1691:
369:
316:
132:
6455:
Some illustrative examples of non-orientable manifolds include: (1) the
5307:, who was motivated by the then recent progress in theoretical physics (
9591:
9156:
9114:
8940:
8853:
8485:
8389:
8300:
8212:. W.A. Benjamin Inc. (reprinted by Addison-Wesley and Westview Press).
7947:. Advanced undergraduate / first-year graduate text inspired by Milnor.
7865:
7755:
7728:
7527:
7521:
7515:
7031:
6969:
6810:
6581:
6244:
5807:
5717:
4261:
4036:
2825:
2765:
234:
124:
120:
6684:
5339:. A very pervasive and flexible technique underlying much work on the
4648:
Another important source of manifolds in 19th century mathematics was
4311:
2214:
This implies also that every point has a neighborhood homeomorphic to
9566:
9517:
8970:
8935:
8640:
8527:
8287:(A film explaining and visualizing manifolds up to fourth dimension.)
7848:
6626:
6532:
6515:
6175:
is a kind of manifold which is used to represent the phase spaces in
6010:
is the dimension of the sphere. Further examples can be found in the
5798:
5713:
5410:
5312:
5248:
4782:
4464:
4337:
4028:
3923:
2961:. Every boundary point has a neighborhood homeomorphic to the "half"
2322:
2317:
of the manifold. This is, in particular, the case when manifolds are
2038:
1838:
332:
7857:
7720:
7579:
Introduction to Holomorphic Functions of Several Variables, Volume 2
7171:. Suppose also that the following conditions hold. First: for every
6310:. The most familiar invariants, which are visible for surfaces, are
5814:
which is such that the group operations are defined by smooth maps.
5271:, and rigorously classified in the beginning of the 20th century by
3851:
coordinate (coloured red in the picture on the right). The function
3847:. Consider the northern hemisphere, which is the part with positive
3617:
2473:(see below) are all differentiable, allows us to do calculus on it.
9581:
9134:
9129:
9119:
8510:
7795:
7480:
6908:
6358:
6062:
on the overlaps. These manifolds are the basic objects of study in
5516:
5276:
4778:) which served as a precursor to the modern concept of a manifold.
4502:
4257:
4243:
1834:
1790:
343:
304:
296:
265:
8291:
7483: â Straight path on a curved surface or a Riemannian manifold
6365:
were founded in order to study invariant properties of manifolds.
5810:, are differentiable manifolds that carry also the structure of a
342:
The study of manifolds requires working knowledge of calculus and
9290:
9252:
8034:. Detailed and comprehensive first-year graduate text; sequel to
7076:
be a nonempty set. Suppose that some family of real functions on
6239:
The classification of smooth closed manifolds is well understood
4774:, Henri Poincaré gave a definition of a differentiable manifold (
4310:
Manifolds which can be constructed by identifying points include
4234:= 1, the example simplifies to the circle example given earlier.
281:
7694:; translation in Russian Math. Surveys 53 (1998), no. 1, 229â236
7688:
7671:
6475:
5416:
whose inverse is also continuous) mapping that neighbourhood to
1939:
excludes spaces which are in some sense 'too large' such as the
1822:(all in "one piece"); an example is a pair of separate circles.
1356:{\displaystyle \chi _{\mathrm {minus} }(x,y)=s={\frac {y}{1+x}}}
790:-coordinates are positive. Both map this part into the interval
9616:
9208:
8726:
6911:
is a generalization of manifold allowing for certain kinds of "
5709:
4432:
4390:
2829:
2764:
is a manifold with an edge. For example, a sheet of paper is a
1957:
to a Euclidean space means that every point has a neighborhood
1687:
1436:{\displaystyle \chi _{\mathrm {plus} }(x,y)=t={\frac {y}{1-x}}}
476:
Such functions along with the open regions they map are called
246:
230:
99:
8295:
8164:
Gesammelte mathematische Werke und wissenschaftlicher Nachlass
6564:
For two dimensional manifolds a key invariant property is the
6341:. All invariants of a smooth closed manifold are thus global.
5898:
matrices with non-zero determinant. If the matrix entries are
4272:, identified as a quotient space of the corresponding sphere.
3953:
This can be easily generalized to higher-dimensional spheres.
7217:{\displaystyle H\in C^{\infty }\left(\mathbb {R} ^{n}\right)}
6869:; and it omits finite dimension, allowing structures such as
5701:
4976:'). In this way he introduces a precursor to the notion of a
4582:
4410:
3100:. Any homeomorphism between half-balls must send points with
2747:-manifold without boundary, so the chart with transition map
2703:
These notions are made precise in general through the use of
2510:-axis and the origin. Another example of a chart is the map Ï
1779:
1767:
934:
can be constructed, which takes values from the co-domain of
308:
250:
116:
8191:
Ueber die Hypothesen, welche der Geometrie zu Grunde liegen.
7489: â Subdiscipline of statistics: statistics on manifolds
2725:
A smooth 2-manifold: The interior chart with transition map
7365:{\displaystyle H\circ \left(f_{1},\dots ,f_{n}\right)\in C}
6255:, and in high dimension (5 and above) it is algebraic, via
6162:. Similarly, Fréchet manifolds are locally homeomorphic to
5705:
5217:
has nonzero gradient at every point of the circle. By the
3264:
which have neighborhoods homeomorphic to an open subset of
1449:
is the slope of the line through the point at coordinates (
9177:
4348:
may be obtained by gluing a sphere with a hole in it to a
2458:, invertible maps that are continuous in both directions.
1770:
cannot have a plane representation consisting of a single
391:). Any point of this arc can be uniquely described by its
6295:
that can decide whether two manifolds are diffeomorphic.
4291:
is the group, the resulting quotient space is denoted by
1771:
1670:
Each chart omits a single point, either (â1, 0) for
7833:
7603:
Shigeyuki Morita; Teruko Nagase; Katsumi Nomizu (2001).
5311:), where they serve as a substitute for ordinary 'flat'
4793:. In the third section, he begins by remarking that the
27:
Topological space that locally resembles Euclidean space
7779:"Stratified vector bundles: Examples and constructions"
6247:: in low dimensions (2 and 3) it is geometric, via the
5864:
Other examples of Lie groups include special groups of
5445:. These homeomorphisms are the charts of the manifold.
5225:
of Euclidean space is locally the graph of a function.
2370:
2309:
that appears in the preceding definition is called the
8074:. Classic brief introduction to differential topology.
8017:. Detailed and comprehensive first-year graduate text.
6897:, while infinite-dimensional manifolds are studied in
5538:
Two important classes of differentiable manifolds are
5125:
5082:
5036:
4993:
4902:
depend continuously differentiably on the coordinates
264:
The concept of a manifold is central to many parts of
8232:
A Comprehensive Introduction to Differential Geometry
8100:
7438:
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7378:
7310:
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2337:
of a sphere and a line in three-dimensional space is
2282:
2249:
2220:
2046:
2017:
1974:
1624:
1487:
1457:) and the fixed pivot point (â1, 0); similarly,
1369:
1286:
1052:
1020:
975:
940:
828:
796:
776:
756:
715:
680:
488:
420:
208:
174:
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7538:
Pages displaying wikidata descriptions as a fallback
5258:
4318:(starting with a plane and a sphere, respectively).
4230:, this atlas defines a smooth manifold. In the case
4087:
can be constructed by gluing together two copies of
3621:
The chart maps the part of the sphere with positive
2832:
with interior is also a 2-manifold with boundary. A
7611:. American Mathematical Society Bookstore. p.
4601:, which can be extended to higher dimensions using
4237:
2717:
Topological manifold § Manifolds with boundary
2461:In the case of a differentiable manifold, a set of
1921:that is locally homeomorphic to a Euclidean space.
1862:(a closed loop piece and an open, infinite piece).
8224:advanced undergraduate / first-year graduate text.
8115:
7604:
7456:
7424:
7404:
7384:
7372:. Second: every function, which in every point of
7364:
7296:
7244:
7216:
7163:
7143:
7123:
7088:
7068:
7012:for topological manifolds. Basic examples include
6784:
6747:
6710:
6633:is a central example, and generalizations such as
6438:
6405:
6143:
6122:is a manifold modeled on boundaries of domains in
6105:
6082:
6050:
6002:
5976:
5921:
5890:
5845:
5774:
5688:
5656:
5636:
5616:
5437:
5393:
5209:
5157:
5111:
5068:
5022:
4966:
4941:
4919:
4894:
4870:
4829:
4680:constrain it to more complicated formations, e.g.
4553:
4489:Another, more topological example of an intrinsic
4216:
4108:
3912:
3839:
3808:
3691:
3650:
3593:
3567:
3544:
3524:
3498:
3478:
3455:
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3332:
3309:
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3256:
3236:
3210:
3186:
3158:
3125:
3092:
2973:
2953:
2855:
2812:
2780:
2768:with a 1-dimensional boundary. The boundary of an
2665:
2604:
2575:
2498:
2446:
2294:
2264:
2235:
2206:
2029:
1992:
1643:
1592:
1435:
1355:
1253:
1038:
1002:
969:back to the circle using the inverse, followed by
961:
926:
814:
782:
762:
742:
701:
657:
466:
214:
180:
159:
6805:In geometric topology, most commonly studied are
6066:. A one-complex-dimensional manifold is called a
4341:manifolds, other structures should be preserved.
3976:resulting manifold is a differentiable manifold.
1907:have homeomorphisms on overlapping neighborhoods
9835:
8086:. Addison-Wesley (reprinted by Westview Press)
6274:However, one can determine if two manifolds are
6225:
4474:gives a method for computing the curvature of a
3979:This can be illustrated with the transition map
2037:), or it has a neighborhood homeomorphic to the
1895:There are many different kinds of manifolds. In
467:{\displaystyle \chi _{\mathrm {top} }(x,y)=x.\,}
6852:
5789:Any Riemannian manifold is a Finsler manifold.
5531:-dimensional Euclidean space consisting of the
5519:on a differentiable manifold. Each point of an
4022:
2554:can be defined which goes from an open ball in
8182:The 1851 doctoral thesis in which "manifold" (
5861:1 with multiplication as the group operation.
5563:generalizes the idea of a piecewise smooth or
5263:Two-dimensional manifolds, also known as a 2D
4505:in the three-dimensional Euclidean space with
4394:A finite cylinder is a manifold with boundary.
3575:is a manifold (without boundary) of dimension
3532:is a manifold (without boundary) of dimension
9193:
8316:
6459:, which is a manifold with boundary, (2) the
5617:{\displaystyle \langle \cdot ,\cdot \rangle }
5462:
1469:) and (+1, 0). The inverse mapping from
8296:Max Planck Institute for Mathematics in Bonn
6090:-dimensional complex manifold has dimension
5853:, can be also characterised as the group of
5769:
5763:
5683:
5671:
5611:
5599:
4352:along their respective circular boundaries.
4202:
4195:
4175:
4169:
4148:
4142:
3087:
3039:
2988:
2948:
2921:
2870:
387:is positive (indicated by the yellow arc in
237:. Two-dimensional manifolds are also called
8094:. Undergraduate text treating manifolds in
7124:{\displaystyle C\subseteq \mathbb {R} ^{M}}
6972:. In French an algebraic variety is called
6017:
5585:is a differentiable manifold in which each
5523:-dimensional differentiable manifold has a
5500:
9200:
9186:
8323:
8309:
8064:Topology from the Differentiable Viewpoint
7392:locally coincides with some function from
6785:{\displaystyle f\colon M\to \mathbb {C} ,}
6679:
6187:. A closely related type of manifold is a
6029:is a manifold whose charts take values in
4321:
4061:
3942:) plane and two charts projecting on the (
2477:, for example, form a chart for the plane
1877:
1729:divides the sphere into two half spheres (
8103:
7896:
7847:
7794:
7687:
7656:. Serié 11 (in French). Gauthier-Villars.
7238:
7200:
7151:be equipped with the topology induced by
7111:
6775:
6748:{\displaystyle f\colon M\to \mathbb {R} }
6741:
6426:
6393:
6131:
6038:
5466:
5425:
5381:
5350:
4882:), then he requires that the coordinates
4156:
4129:
4096:
3922:maps the northern hemisphere to the open
3827:
3743:
3679:
3638:
3486:is a manifold with boundary of dimension
3438:
3273:
2710:
2653:
2616:in the circle example above, is called a
2592:
2563:
2514:mentioned above, a chart for the circle.
2486:
2434:
2252:
2223:
2120:
2007:This implies that either the point is an
1977:
463:
87:Learn how and when to remove this message
9557:Covariance and contravariance of vectors
8330:
7878:
7741:
7648:
7635:The notion of a map can formalized as a
6683:
6591:
6531:
6521:
6474:
5929:-dimensional disconnected manifold. The
5361:
5287:proved the Poincaré conjecture (see the
5235:that followed shortly. During the 1930s
4765:
4389:
3616:
3169:
2720:
1914:Formally, a (topological) manifold is a
1789:
1743:), which may both be mapped on the disc
1651:(that is, one has this relation between
1271:
1003:{\displaystyle \chi _{\mathrm {right} }}
743:{\displaystyle \chi _{\mathrm {right} }}
358:
110:
98:
50:This article includes a list of general
7703:
7666:
7575:
7297:{\displaystyle f_{1},\dots ,f_{n}\in C}
6841:methods of studying manifolds, such as
5570:
4871:{\displaystyle \theta '\left(y'\right)}
4609:linked the Euler characteristic to the
2635:
235:self-crossing curves such as a figure 8
14:
9836:
8194:The 1854 Göttingen inaugural lecture (
6833:. This leads to such functions as the
6467:, which arises naturally in geometry.
6314:(a normal invariant, also detected by
1892:that is "modeled on" Euclidean space.
1874:always preserve the number of pieces.
1782:for covering the whole Earth surface.
962:{\displaystyle \chi _{\mathrm {top} }}
822:, though differently. Thus a function
702:{\displaystyle \chi _{\mathrm {top} }}
349:
9181:
8304:
8036:Introduction to Topological Manifolds
8007:Introduction to Topological Manifolds
7596:
7556:
6983:), while a smooth manifold is called
5846:{\displaystyle \operatorname {U} (1)}
4605:. In the mid nineteenth century, the
4355:
4336:Formally, the gluing is defined by a
4116:. The transition map between them is
4031:in some Euclidean space. This is the
3913:{\displaystyle \chi (x,y,z)=(x,y),\ }
3665:
3525:{\displaystyle \operatorname {Int} M}
3363:{\displaystyle \operatorname {Int} M}
3237:{\displaystyle \operatorname {Int} M}
2756:must map to an open Euclidean subset.
119:is decomposed into charts around the
8244:(2nd ed.). New York: Springer.
7872:
7776:
7707:(1936). "Differentiable Manifolds".
6587:
5737:
5492:in the definition). All points in a
5321:analogues of the Poincaré conjecture
4981:
4420:
4054:, but instead there is an intrinsic
4043:to some surface through that point.
3456:{\displaystyle \mathbb {R} _{+}^{n}}
2371:Charts, atlases, and transition maps
147:near each point. More precisely, an
36:
8256:. Concise first-year graduate text.
8046:Algebraic Topology: An Introduction
7986:and Siebenmann, Laurence C. (1977)
7827:
7674:[On Teaching Mathematics].
6821:, an important example of which is
6271:manifold refer to the same object.
6253:solution of the Poincaré conjecture
6058:and whose transition functions are
5689:{\displaystyle \langle u,v\rangle }
5289:Solution of the Poincaré conjecture
4744:n-fach ausgedehnte Mannigfaltigkeit
4692:, one of the founders of topology.
4645:of functions of complex variables.
4413:and surfaces as well as ideas from
2689:, the transition functions must be
107:immersed in three-dimensional space
24:
9420:Tensors in curvilinear coordinates
8237:
7530: â Manifold of dimension five
7189:
6560:Genus and the Euler characteristic
6327:curvature of a Riemannian manifold
6306:, classic algebraic topology, and
6158:which are locally homeomorphic to
6113:as a real differentiable manifold.
5828:
4405:History of manifolds and varieties
4001:on the second copy with the point
3559:
3324:
3042:
2924:
2612:. The resultant map, like the map
2544:
1718:may be covered by an atlas of six
1385:
1382:
1379:
1376:
1305:
1302:
1299:
1296:
1293:
1175:
1172:
1169:
1166:
1163:
1117:
1114:
1111:
1094:
1091:
1088:
1085:
1082:
994:
991:
988:
985:
982:
953:
950:
947:
910:
907:
904:
889:
886:
883:
880:
877:
734:
731:
728:
725:
722:
693:
690:
687:
617:
614:
611:
608:
605:
564:
561:
558:
555:
514:
511:
508:
505:
502:
499:
433:
430:
427:
225:One-dimensional manifolds include
56:it lacks sufficient corresponding
25:
9860:
8260:
7563:, World Scientific, p. 110,
7504:Mathematics of general relativity
7245:{\displaystyle n\in \mathbb {N} }
5868:, which are all subgroups of the
5535:of the curves through the point.
5259:Topology of manifolds: highlights
5158:{\textstyle x=-{\sqrt {1-y^{2}}}}
5069:{\textstyle y=-{\sqrt {1-x^{2}}}}
4719:values. He distinguishes between
4364:of manifolds is also a manifold.
4166:
4139:
3194:be a manifold with boundary. The
1993:{\displaystyle \mathbb {R} ^{n},}
1610: = 1 for all values of
8116:{\displaystyle \mathbb {R} ^{n}}
8023:Introduction to Smooth Manifolds
7654:Journal de l'Ăcole Polytechnique
6817:, one often studies solution to
6439:{\displaystyle \mathbb {R} ^{n}}
6406:{\displaystyle \mathbb {R} ^{n}}
6373:
6144:{\displaystyle \mathbb {C} ^{n}}
6051:{\displaystyle \mathbb {C} ^{n}}
5438:{\displaystyle \mathbb {R} ^{n}}
5394:{\displaystyle \mathbb {R} ^{n}}
5112:{\textstyle x={\sqrt {1-y^{2}}}}
5023:{\textstyle y={\sqrt {1-x^{2}}}}
4715:, because the variable can have
4264:are considered to be relatively
4238:Identifying points of a manifold
4109:{\displaystyle \mathbb {R} ^{n}}
3840:{\displaystyle \mathbb {R} ^{2}}
3692:{\displaystyle \mathbb {R} ^{3}}
3651:{\displaystyle \mathbb {R} ^{2}}
3286:{\displaystyle \mathbb {R} ^{n}}
2666:{\displaystyle \mathbb {R} ^{n}}
2605:{\displaystyle \mathbb {R} ^{n}}
2576:{\displaystyle \mathbb {R} ^{n}}
2499:{\displaystyle \mathbb {R} ^{2}}
2447:{\displaystyle \mathbb {R} ^{n}}
2265:{\displaystyle \mathbb {R} ^{n}}
2236:{\displaystyle \mathbb {R} ^{n}}
2049:
1690:is an example of a surface. The
1644:{\displaystyle t={\frac {1}{s}}}
41:
7881:"Abstract covariant derivative"
7783:Journal of Geometry and Physics
7509:
6930:Algebraic varieties and schemes
6503:
6470:
6333:of a manifold equipped with an
5303:and in a different setting, by
5210:{\displaystyle x^{2}+y^{2}-1=0}
4949:sont fonctions analytiques des
4770:In his very influential paper,
3604:
1811:
1807:
1803:
1799:
1785:
399:onto the first coordinate is a
8363:Differentiable/Smooth manifold
8148:. Princeton University Press.
8066:. Princeton University Press.
7990:. Princeton University Press.
7954:. Princeton University Press.
7921:. Princeton University Press.
7813:10.1016/j.geomphys.2024.105114
7770:
7735:
7697:
7660:
7642:
7629:
7607:Geometry of Differential Forms
7549:
7451:
7439:
7010:topologically stratified space
6858:Infinite dimensional manifolds
6819:partial differential equations
6771:
6737:
6288:under different descriptions.
5963:
5951:
5840:
5834:
4878:. If these manifolds overlap (
4824:
4818:
4699:comes from Riemann's original
4184:
4151:
4011:on the first copy (the points
3901:
3889:
3883:
3865:
3735:
3717:
3416:
3397:
3036:
2991:
2918:
2873:
2807:
2795:
2788:-manifold with boundary is an
2395:, collected in a mathematical
2112:
2067:
1403:
1391:
1323:
1311:
1066:
1060:
1033:
1021:
865:
853:
850:
847:
835:
809:
797:
635:
623:
582:
570:
532:
520:
451:
439:
222:-dimensional Euclidean space.
13:
1:
9473:Exterior covariant derivative
9405:Tensor (intrinsic definition)
7908:
7008:) for smooth manifolds and a
6226:Classification and invariants
5984:dimensional manifolds, where
5792:
4748:n times extended manifoldness
4387: Ă , respectively.
3463:under some coordinate chart.
2000:for some nonnegative integer
9498:Raising and lowering indices
8241:An Introduction to Manifolds
8144:Neuwirth, L. P., ed. (1975)
7500: â Mathematics timeline
6853:Generalizations of manifolds
6649:. Basic results include the
4616:
4023:Intrinsic and extrinsic view
3956:
2276:to any open ball in it (for
1888:Informally, a manifold is a
1263:Such a function is called a
7:
9736:Gluon field strength tensor
9207:
9069:Classification of manifolds
8273:Encyclopedia of Mathematics
7672:"Đ ĐżŃĐ”ĐżĐŸĐŽĐ°ĐČĐ°ĐœĐžĐž ĐŒĐ°ŃĐ”ĐŒĐ°ŃĐžĐșĐž"
7468:
6847:AtiyahâSinger index theorem
6843:hearing the shape of a drum
6368:
6322:(a homological invariant).
6232:Classification of manifolds
5323:, had been done earlier by
4977:
4787:continuously differentiable
3612:
1778:), and therefore one needs
10:
9865:
9547:Cartan formalism (physics)
9367:Penrose graphical notation
7998:. A detailed study of the
7917:, and Quinn, Frank (1990)
7777:Ross, Ethan (2024-04-01).
7652:(1895). "Analysis Situs".
7524: â Mathematical space
7518: â Mathematical space
6610:
6525:
6507:
6496:
6482:
6377:
6361:theory, and the theory of
6265:complete set of invariants
6229:
6179:. They are endowed with a
5796:
5775:{\displaystyle \|\cdot \|}
5741:
5574:
5552:(they can be expressed as
5504:
5365:
5354:
5283:. After nearly a century,
4830:{\displaystyle \theta (y)}
4752:n-dimensional manifoldness
4736:discontinuous manifoldness
4593: = 2 edges, and
4554:{\displaystyle V-E+F=2.\ }
4402:
4398:
4325:
4248:Group action (mathematics)
4241:
3960:
3568:{\displaystyle \partial M}
3333:{\displaystyle \partial M}
3244:, is the set of points in
2714:
2521:
2517:
2406:
2380:
2374:
2272:is homeomorphic, and even
1881:
1774:(also called "chart", see
674:The top and right charts,
410:from the upper arc to the
380: = 1, where the
167:-dimensional manifold, or
29:
9753:
9693:
9642:
9635:
9527:
9458:
9395:
9339:
9286:
9233:
9226:
9219:Glossary of tensor theory
9215:
9145:over commutative algebras
9102:
9061:
8994:
8891:
8787:
8734:
8725:
8561:
8484:
8423:
8343:
8002:of topological manifolds.
7935:and Pollack, Alan (1974)
7582:, CRC Press, p. 73,
7096:was chosen. Denote it by
6813:decompositions, while in
6655:Whitney immersion theorem
6651:Whitney embedding theorem
6202:piecewise linear manifold
5891:{\displaystyle n\times n}
5696:gives a real number. The
5253:Whitney embedding theorem
5239:and others clarified the
5219:implicit function theorem
4791:implicit function theorem
4762:are named after Riemann.
4501:showed that for a convex
4328:Quotient space (topology)
3926:by projecting it on the (
3422:{\displaystyle (x_{n}=0)}
2622:coordinate transformation
2402:
1754:by the projection on the
1681:
1602:It can be confirmed that
1010:back to the interval. If
354:
327:, while four-dimensional
32:Manifold (disambiguation)
9803:Gregorio Ricci-Curbastro
9675:Riemann curvature tensor
9382:Van der Waerden notation
8861:Riemann curvature tensor
7543:
6919:Euclidean space) by the
6863:topological vector space
6672:; a basic result is the
6647:ramified covering spaces
6300:a rich set of invariants
6018:Other types of manifolds
5977:{\displaystyle n(n-1)/2}
5501:Differentiable manifolds
5463:differentiable manifolds
4742:, Riemann constructs an
4721:stetige Mannigfaltigkeit
4709:William Kingdon Clifford
4478:without considering the
3993:for the first copy, and
1905:differentiable manifolds
293:differentiable structure
289:differentiable manifolds
9773:Elwin Bruno Christoffel
9706:Angular momentum tensor
9377:Tetrad (index notation)
9347:Abstract index notation
7919:Topology of 4-Manifolds
7898:10.4064/cm-18-1-251-272
7885:Colloquium Mathematicum
7576:Gunning, R. C. (1990),
7557:Riaza, Ricardo (2008),
6867:non-Hausdorff manifolds
6845:and some proofs of the
6680:Scalar-valued functions
5513:differentiable manifold
5507:Differentiable manifold
5357:Categories of manifolds
4804:Poincaré's notion of a
4799:une chaßne des variétés
4732:continuous manifoldness
4674:generalized coordinates
4589: = 1 vertex,
4581:. On the other hand, a
4431:considers spaces where
4322:Gluing along boundaries
3159:{\displaystyle x_{1}=0}
3126:{\displaystyle x_{1}=0}
2383:Differentiable manifold
2349:has a fixed dimension.
1949:non-Hausdorff manifolds
1884:Categories of manifolds
1878:Mathematical definition
241:. Examples include the
143:that locally resembles
71:more precise citations.
9587:Levi-Civita connection
8653:Manifold with boundary
8368:Differential structure
8238:Tu, Loring W. (2011).
8117:
7487:Directional statistics
7458:
7426:
7406:
7386:
7366:
7298:
7246:
7218:
7165:
7145:
7125:
7090:
7070:
7014:manifold with boundary
6987:variété différentielle
6786:
6749:
6718:
6712:
6674:Nash embedding theorem
6670:Riemannian submersions
6608:
6545:
6480:
6440:
6407:
6363:characteristic classes
6298:Smooth manifolds have
6249:uniformization theorem
6197:combinatorial manifold
6145:
6107:
6084:
6052:
6004:
5978:
5923:
5892:
5847:
5776:
5690:
5658:
5638:
5618:
5439:
5395:
5297:geometrization program
5211:
5159:
5113:
5070:
5024:
4968:
4943:
4921:
4896:
4872:
4831:
4658:William Rowan Hamilton
4555:
4429:Non-Euclidean geometry
4395:
4316:real projective spaces
4218:
4110:
4065:-Sphere as a patchwork
3914:
3841:
3810:
3693:
3652:
3626:
3595:
3569:
3546:
3526:
3500:
3480:
3457:
3423:
3384:
3364:
3334:
3311:
3287:
3258:
3238:
3212:
3188:
3160:
3127:
3094:
2975:
2955:
2857:
2814:
2782:
2762:manifold with boundary
2757:
2711:Manifold with boundary
2673:(that is, if they are
2667:
2606:
2577:
2500:
2448:
2296:
2295:{\displaystyle n>0}
2266:
2237:
2208:
2031:
1994:
1872:topological operations
1825:Manifolds need not be
1818:Manifolds need not be
1815:
1659:for every point where
1645:
1594:
1437:
1357:
1277:
1255:
1040:
1004:
963:
928:
816:
784:
764:
744:
703:
659:
468:
364:
216:
182:
161:
128:
108:
18:Manifold with boundary
9813:Jan Arnoldus Schouten
9768:Augustin-Louis Cauchy
9248:Differential geometry
8118:
8083:Analysis on Manifolds
7970:Differential Topology
7937:Differential Topology
7879:Sikorski, R. (1967).
7836:Annals of Mathematics
7709:Annals of Mathematics
7534:Manifolds of mappings
7498:Timeline of manifolds
7459:
7457:{\displaystyle (M,C)}
7427:
7407:
7387:
7367:
7299:
7247:
7219:
7166:
7146:
7126:
7091:
7071:
6815:mathematical analysis
6787:
6750:
6713:
6688:3D color plot of the
6687:
6595:
6572:, and more generally
6538:real projective plane
6535:
6528:Real projective space
6522:Real projective plane
6478:
6465:real projective plane
6441:
6408:
6339:geometry and topology
6230:Further information:
6146:
6108:
6085:
6053:
6005:
5979:
5924:
5922:{\displaystyle n^{2}}
5893:
5848:
5777:
5691:
5659:
5639:
5619:
5440:
5396:
5362:Topological manifolds
5341:topology of manifolds
5251:theory. Notably, the
5245:differential geometry
5212:
5160:
5114:
5071:
5030:or else the function
5025:
4969:
4944:
4922:
4897:
4873:
4832:
4766:Poincaré's definition
4686:Joseph-Louis Lagrange
4643:analytic continuation
4599:topological invariant
4556:
4493:of a manifold is its
4403:Further information:
4393:
4270:real projective space
4219:
4118:inversion in a sphere
4111:
3961:Further information:
3915:
3842:
3811:
3694:
3653:
3625:coordinate to a disc.
3620:
3596:
3570:
3547:
3527:
3501:
3481:
3458:
3424:
3385:
3365:
3335:
3312:
3288:
3259:
3239:
3213:
3189:
3170:Boundary and interior
3161:
3128:
3095:
2976:
2956:
2858:
2815:
2813:{\displaystyle (n-1)}
2783:
2724:
2683:holomorphic functions
2668:
2618:change of coordinates
2607:
2578:
2501:
2449:
2297:
2267:
2238:
2209:
2032:
1995:
1901:topological manifolds
1897:geometry and topology
1882:Further information:
1793:
1646:
1595:
1438:
1358:
1275:
1256:
1041:
1039:{\displaystyle (0,1)}
1005:
964:
929:
817:
815:{\displaystyle (0,1)}
785:
765:
745:
704:
660:
469:
362:
321:Hamiltonian formalism
303:on a manifold allows
259:real projective plane
217:
183:
162:
114:
102:
9788:Carl Friedrich Gauss
9721:stressâenergy tensor
9716:Cauchy stress tensor
9468:Covariant derivative
9430:Antisymmetric tensor
9362:Multi-index notation
8800:Covariant derivative
8351:Topological manifold
8196:Habilitationsschrift
8098:
8020:Lee, John M. (2003)
8005:Lee, John M. (2000)
7950:Hempel, John (1976)
7915:Freedman, Michael H.
7436:
7416:
7396:
7376:
7308:
7256:
7228:
7175:
7155:
7135:
7100:
7080:
7060:
6992:differential variety
6829:: the kernel of the
6825:, where one studies
6759:
6725:
6696:
6666:isometric immersions
6662:isometric embeddings
6570:Euler characteristic
6421:
6388:
6206:simplicial complexes
6126:
6094:
6074:
6033:
5988:
5945:
5906:
5876:
5870:general linear group
5825:
5760:
5668:
5664:, the inner product
5648:
5628:
5596:
5589:is equipped with an
5571:Riemannian manifolds
5467:Riemannian manifolds
5420:
5403:locally homeomorphic
5376:
5368:topological manifold
5351:Additional structure
5169:
5123:
5080:
5034:
4991:
4953:
4933:
4906:
4886:
4880:a une partie commune
4841:
4812:
4650:analytical mechanics
4607:GaussâBonnet theorem
4579:Euler characteristic
4524:
4495:Euler characteristic
4287:is the manifold and
4124:
4091:
4056:stable normal bundle
3859:
3822:
3703:
3674:
3633:
3579:
3556:
3536:
3510:
3490:
3470:
3433:
3394:
3374:
3348:
3321:
3301:
3268:
3248:
3222:
3202:
3178:
3137:
3104:
2985:
2965:
2867:
2847:
2792:
2772:
2687:symplectic manifolds
2648:
2636:Additional structure
2587:
2558:
2481:
2471:transition functions
2429:
2357:locally ringed space
2280:
2247:
2218:
2044:
2015:
1972:
1955:Locally homeomorphic
1899:, all manifolds are
1794:Four manifolds from
1674:or (+1, 0) for
1622:
1485:
1367:
1284:
1050:
1018:
973:
938:
826:
794:
774:
754:
713:
678:
486:
418:
329:Lorentzian manifolds
313:Symplectic manifolds
274:systems of equations
270:mathematical physics
206:
172:
151:
30:For other uses, see
9849:Geometry processing
9665:Nonmetricity tensor
9520:(2nd-order tensors)
9488:Hodge star operator
9478:Exterior derivative
9327:Transport phenomena
9312:Continuum mechanics
9268:Multilinear algebra
8834:Exterior derivative
8436:AtiyahâSinger index
8385:Riemannian manifold
8285:Dimensions-math.org
8048:. Springer-Verlag.
8026:. Springer-Verlag.
8009:. Springer-Verlag.
7972:. Springer Verlag.
7805:2024JGP...19805114R
7744:Comment. Math. Helv
7053:Differential spaces
6949:instead of atlases.
6899:functional analysis
6835:spherical harmonics
6711:{\displaystyle n=5}
6690:spherical harmonics
6499:Quasitoric manifold
6380:Orientable manifold
6177:classical mechanics
6172:symplectic manifold
6012:table of Lie groups
6003:{\displaystyle n-1}
5583:Riemannian manifold
5577:Riemannian manifold
5414:continuous function
5281:Poincaré conjecture
4457:hyperbolic geometry
3594:{\displaystyle n-1}
3452:
3059:
2941:
2838:Boundary (topology)
2626:transition function
2552:transition function
2506:minus the positive
2353:Sheaf-theoretically
2347:connected component
2189:
2165:
2147:
2030:{\displaystyle n=0}
1667:are both nonzero).
1130:
923:
350:Motivating examples
325:classical mechanics
9798:Tullio Levi-Civita
9741:Metric tensor (GR)
9655:Levi-Civita symbol
9508:Tensor contraction
9322:General relativity
9258:Euclidean geometry
9140:Secondary calculus
9094:Singularity theory
9049:Parallel transport
8817:De Rham cohomology
8456:Generalized Stokes
8166:, SĂ€ndig Reprint.
8113:
8042:Massey, William S.
7756:10.1007/BF02565940
7637:cell decomposition
7454:
7422:
7412:, also belongs to
7402:
7382:
7362:
7304:, the composition
7294:
7242:
7214:
7161:
7141:
7121:
7086:
7066:
7042:Homology manifolds
7018:semialgebraic sets
7006:Whitney conditions
6976:variété algébrique
6827:harmonic functions
6782:
6745:
6719:
6708:
6623:geometric topology
6609:
6546:
6481:
6436:
6403:
6345:Algebraic topology
6308:geometric topology
6304:point-set topology
6141:
6106:{\displaystyle 2n}
6103:
6080:
6048:
6000:
5974:
5937:of the sphere and
5919:
5902:, this will be an
5888:
5843:
5772:
5686:
5654:
5634:
5614:
5545:analytic manifolds
5435:
5391:
5207:
5155:
5109:
5066:
5020:
4967:{\displaystyle y'}
4964:
4939:
4920:{\displaystyle y'}
4917:
4892:
4868:
4827:
4806:chain of manifolds
4652:, as developed by
4631:elliptic integrals
4627:Carl Gustav Jacobi
4621:Investigations of
4611:Gaussian curvature
4551:
4484:intrinsic property
4437:parallel postulate
4396:
4375:, for example, as
4356:Cartesian products
4214:
4106:
3910:
3837:
3806:
3689:
3666:Sphere with charts
3648:
3627:
3591:
3565:
3542:
3522:
3496:
3476:
3453:
3436:
3419:
3380:
3360:
3330:
3307:
3283:
3254:
3234:
3208:
3184:
3156:
3123:
3090:
3045:
2971:
2951:
2927:
2853:
2810:
2778:
2758:
2691:symplectomorphisms
2663:
2602:
2573:
2496:
2444:
2365:algebraic geometry
2359:, whose structure
2355:, a manifold is a
2292:
2262:
2233:
2204:
2175:
2151:
2133:
2027:
1990:
1816:
1641:
1590:
1588:
1433:
1353:
1278:
1251:
1249:
1105:
1036:
1000:
959:
924:
898:
812:
780:
760:
740:
699:
655:
653:
464:
365:
337:general relativity
212:
178:
157:
129:
109:
9831:
9830:
9793:Hermann Grassmann
9749:
9748:
9701:Moment of inertia
9562:Differential form
9537:Affine connection
9352:Einstein notation
9335:
9334:
9263:Exterior calculus
9243:Coordinate system
9175:
9174:
9057:
9056:
8822:Differential form
8476:Whitney embedding
8410:Differential form
8251:978-1-4419-7399-3
8160:Riemann, Bernhard
8154:978-0-691-08170-0
8133:. Prentice Hall.
8127:Munkres, James R.
8078:Munkres, James R.
7939:. Prentice-Hall.
7933:Guillemin, Victor
7838:. Second Series.
7711:. Second Series.
7676:Uspekhi Mat. Nauk
7493:List of manifolds
7425:{\displaystyle C}
7405:{\displaystyle C}
7385:{\displaystyle M}
7164:{\displaystyle C}
7144:{\displaystyle M}
7089:{\displaystyle M}
7069:{\displaystyle M}
7047:homology manifold
6981:algebraic variety
6939:algebraic variety
6889:to be modeled on
6887:Fréchet manifolds
6881:to be modeled on
6873:to be modeled on
6871:Hilbert manifolds
6823:harmonic analysis
6796:regular functions
6794:sometimes called
6625:a basic type are
6619:maps of manifolds
6613:Maps of manifolds
6588:Maps of manifolds
6335:affine connection
6293:no program exists
6183:that defines the
6083:{\displaystyle n}
5931:orthogonal groups
5738:Finsler manifolds
5657:{\displaystyle v}
5637:{\displaystyle u}
5565:rectifiable curve
5317:Andrey Markov Jr.
5309:YangâMills theory
5233:topological space
5153:
5107:
5064:
5018:
4942:{\displaystyle y}
4927:and vice versa ('
4895:{\displaystyle y}
4678:conservation laws
4623:Niels Henrik Abel
4550:
4472:theorema egregium
4461:elliptic geometry
4421:Early development
4362:Cartesian product
3973:equivalence class
3909:
3545:{\displaystyle n}
3499:{\displaystyle n}
3479:{\displaystyle M}
3383:{\displaystyle M}
3310:{\displaystyle M}
3257:{\displaystyle M}
3211:{\displaystyle M}
3187:{\displaystyle M}
3069:
2974:{\displaystyle n}
2856:{\displaystyle n}
2781:{\displaystyle n}
2679:Complex manifolds
2475:Polar coordinates
2393:coordinate charts
2389:mathematical maps
1810: hyperbola,
1696:implicit equation
1639:
1584:
1540:
1431:
1351:
1245:
1210:
1014:is any number in
783:{\displaystyle y}
763:{\displaystyle x}
395:-coordinate. So,
301:Riemannian metric
215:{\displaystyle n}
181:{\displaystyle n}
160:{\displaystyle n}
141:topological space
97:
96:
89:
16:(Redirected from
9856:
9808:Bernhard Riemann
9640:
9639:
9483:Exterior product
9450:Two-point tensor
9435:Symmetric tensor
9317:Electromagnetism
9231:
9230:
9202:
9195:
9188:
9179:
9178:
9167:Stratified space
9125:Fréchet manifold
8839:Interior product
8732:
8731:
8429:
8325:
8318:
8311:
8302:
8301:
8281:
8255:
8186:) first appears.
8184:Mannigfaltigkeit
8122:
8120:
8119:
8114:
8112:
8111:
8106:
7984:Kirby, Robion C.
7903:
7902:
7900:
7876:
7870:
7869:
7851:
7831:
7825:
7824:
7798:
7774:
7768:
7767:
7739:
7733:
7732:
7701:
7695:
7693:
7691:
7682:(319): 229â234.
7664:
7658:
7657:
7646:
7640:
7633:
7627:
7626:
7610:
7600:
7594:
7592:
7573:
7553:
7539:
7463:
7461:
7460:
7455:
7431:
7429:
7428:
7423:
7411:
7409:
7408:
7403:
7391:
7389:
7388:
7383:
7371:
7369:
7368:
7363:
7355:
7351:
7350:
7349:
7331:
7330:
7303:
7301:
7300:
7295:
7287:
7286:
7268:
7267:
7252:, and arbitrary
7251:
7249:
7248:
7243:
7241:
7223:
7221:
7220:
7215:
7213:
7209:
7208:
7203:
7193:
7192:
7170:
7168:
7167:
7162:
7150:
7148:
7147:
7142:
7130:
7128:
7127:
7122:
7120:
7119:
7114:
7095:
7093:
7092:
7087:
7075:
7073:
7072:
7067:
7022:subanalytic sets
6997:Stratified space
6962:Mannigfaltigkeit
6895:general topology
6879:Banach manifolds
6831:Laplace operator
6791:
6789:
6788:
6783:
6778:
6754:
6752:
6751:
6746:
6744:
6717:
6715:
6714:
6709:
6445:
6443:
6442:
6437:
6435:
6434:
6429:
6412:
6410:
6409:
6404:
6402:
6401:
6396:
6350:simply connected
6219:digital topology
6214:digital manifold
6189:contact manifold
6156:Banach manifolds
6150:
6148:
6147:
6142:
6140:
6139:
6134:
6112:
6110:
6109:
6104:
6089:
6087:
6086:
6081:
6064:complex geometry
6057:
6055:
6054:
6049:
6047:
6046:
6041:
6026:complex manifold
6009:
6007:
6006:
6001:
5983:
5981:
5980:
5975:
5970:
5928:
5926:
5925:
5920:
5918:
5917:
5897:
5895:
5894:
5889:
5852:
5850:
5849:
5844:
5781:
5779:
5778:
5773:
5750:Finsler manifold
5744:Finsler manifold
5733:
5695:
5693:
5692:
5687:
5663:
5661:
5660:
5655:
5643:
5641:
5640:
5635:
5623:
5621:
5620:
5615:
5479:second countable
5444:
5442:
5441:
5436:
5434:
5433:
5428:
5400:
5398:
5397:
5392:
5390:
5389:
5384:
5301:Michael Freedman
5293:William Thurston
5285:Grigori Perelman
5269:Riemann surfaces
5216:
5214:
5213:
5208:
5194:
5193:
5181:
5180:
5164:
5162:
5161:
5156:
5154:
5152:
5151:
5136:
5118:
5116:
5115:
5110:
5108:
5106:
5105:
5090:
5075:
5073:
5072:
5067:
5065:
5063:
5062:
5047:
5029:
5027:
5026:
5021:
5019:
5017:
5016:
5001:
4973:
4971:
4970:
4965:
4963:
4948:
4946:
4945:
4940:
4926:
4924:
4923:
4918:
4916:
4901:
4899:
4898:
4893:
4877:
4875:
4874:
4869:
4867:
4863:
4851:
4836:
4834:
4833:
4828:
4760:Riemann surfaces
4756:Mannigfaltigkeit
4728:Mannigfaltigkeit
4713:Mannigfaltigkeit
4705:Mannigfaltigkeit
4639:Bernhard Riemann
4629:on inversion of
4560:
4558:
4557:
4552:
4548:
4467:, respectively.
4369:product topology
4346:projective plane
4223:
4221:
4220:
4215:
4210:
4209:
4194:
4165:
4164:
4159:
4138:
4137:
4132:
4115:
4113:
4112:
4107:
4105:
4104:
4099:
3919:
3917:
3916:
3911:
3907:
3854:
3846:
3844:
3843:
3838:
3836:
3835:
3830:
3815:
3813:
3812:
3807:
3802:
3798:
3791:
3790:
3778:
3777:
3765:
3764:
3752:
3751:
3746:
3698:
3696:
3695:
3690:
3688:
3687:
3682:
3657:
3655:
3654:
3649:
3647:
3646:
3641:
3600:
3598:
3597:
3592:
3574:
3572:
3571:
3566:
3551:
3549:
3548:
3543:
3531:
3529:
3528:
3523:
3505:
3503:
3502:
3497:
3485:
3483:
3482:
3477:
3462:
3460:
3459:
3454:
3451:
3446:
3441:
3428:
3426:
3425:
3420:
3409:
3408:
3389:
3387:
3386:
3381:
3369:
3367:
3366:
3361:
3339:
3337:
3336:
3331:
3316:
3314:
3313:
3308:
3292:
3290:
3289:
3284:
3282:
3281:
3276:
3263:
3261:
3260:
3255:
3243:
3241:
3240:
3235:
3217:
3215:
3214:
3209:
3193:
3191:
3190:
3185:
3165:
3163:
3162:
3157:
3149:
3148:
3132:
3130:
3129:
3124:
3116:
3115:
3099:
3097:
3096:
3091:
3080:
3079:
3070:
3067:
3058:
3053:
3035:
3034:
3016:
3015:
3003:
3002:
2980:
2978:
2977:
2972:
2960:
2958:
2957:
2952:
2940:
2935:
2917:
2916:
2898:
2897:
2885:
2884:
2862:
2860:
2859:
2854:
2819:
2817:
2816:
2811:
2787:
2785:
2784:
2779:
2755:
2746:
2742:
2733:
2672:
2670:
2669:
2664:
2662:
2661:
2656:
2611:
2609:
2608:
2603:
2601:
2600:
2595:
2582:
2580:
2579:
2574:
2572:
2571:
2566:
2524:Atlas (topology)
2505:
2503:
2502:
2497:
2495:
2494:
2489:
2453:
2451:
2450:
2445:
2443:
2442:
2437:
2419:coordinate chart
2409:Coordinate chart
2377:Atlas (topology)
2343:locally constant
2331:
2330:
2308:
2301:
2299:
2298:
2293:
2271:
2269:
2268:
2263:
2261:
2260:
2255:
2242:
2240:
2239:
2234:
2232:
2231:
2226:
2213:
2211:
2210:
2205:
2200:
2196:
2188:
2183:
2164:
2159:
2146:
2141:
2129:
2128:
2123:
2111:
2110:
2092:
2091:
2079:
2078:
2058:
2057:
2052:
2036:
2034:
2033:
2028:
2003:
1999:
1997:
1996:
1991:
1986:
1985:
1980:
1937:second countable
1925:Second countable
1916:second countable
1861:
1813:
1809:
1806: parabola,
1805:
1801:
1796:algebraic curves
1759:
1753:
1742:
1735:
1728:
1714:
1650:
1648:
1647:
1642:
1640:
1632:
1599:
1597:
1596:
1591:
1589:
1585:
1583:
1582:
1581:
1565:
1557:
1541:
1539:
1538:
1537:
1521:
1520:
1519:
1503:
1442:
1440:
1439:
1434:
1432:
1430:
1416:
1390:
1389:
1388:
1362:
1360:
1359:
1354:
1352:
1350:
1336:
1310:
1309:
1308:
1260:
1258:
1257:
1252:
1250:
1246:
1244:
1243:
1228:
1220:
1216:
1212:
1211:
1209:
1208:
1193:
1180:
1179:
1178:
1150:
1146:
1142:
1141:
1129:
1121:
1120:
1099:
1098:
1097:
1045:
1043:
1042:
1037:
1009:
1007:
1006:
1001:
999:
998:
997:
968:
966:
965:
960:
958:
957:
956:
933:
931:
930:
925:
922:
914:
913:
894:
893:
892:
821:
819:
818:
813:
789:
787:
786:
781:
769:
767:
766:
761:
749:
747:
746:
741:
739:
738:
737:
708:
706:
705:
700:
698:
697:
696:
671:for the circle.
664:
662:
661:
656:
654:
622:
621:
620:
569:
568:
567:
519:
518:
517:
473:
471:
470:
465:
438:
437:
436:
311:to be measured.
221:
219:
218:
213:
187:
185:
184:
179:
166:
164:
163:
158:
92:
85:
81:
78:
72:
67:this article by
58:inline citations
45:
44:
37:
21:
9864:
9863:
9859:
9858:
9857:
9855:
9854:
9853:
9834:
9833:
9832:
9827:
9778:Albert Einstein
9745:
9726:Einstein tensor
9689:
9670:Ricci curvature
9650:Kronecker delta
9636:Notable tensors
9631:
9552:Connection form
9529:
9523:
9454:
9440:Tensor operator
9397:
9391:
9331:
9307:Computer vision
9300:
9282:
9278:Tensor calculus
9222:
9211:
9206:
9176:
9171:
9110:Banach manifold
9103:Generalizations
9098:
9053:
8990:
8887:
8849:Ricci curvature
8805:Cotangent space
8783:
8721:
8563:
8557:
8516:Exponential map
8480:
8425:
8419:
8339:
8329:
8294:project of the
8266:
8263:
8252:
8228:Spivak, Michael
8204:Spivak, Michael
8107:
8102:
8101:
8099:
8096:
8095:
7911:
7906:
7877:
7873:
7858:10.2307/2118532
7832:
7828:
7775:
7771:
7740:
7736:
7721:10.2307/1968482
7702:
7698:
7665:
7661:
7647:
7643:
7634:
7630:
7623:
7601:
7597:
7590:
7571:
7554:
7550:
7546:
7537:
7512:
7471:
7437:
7434:
7433:
7417:
7414:
7413:
7397:
7394:
7393:
7377:
7374:
7373:
7345:
7341:
7326:
7322:
7321:
7317:
7309:
7306:
7305:
7282:
7278:
7263:
7259:
7257:
7254:
7253:
7237:
7229:
7226:
7225:
7204:
7199:
7198:
7194:
7188:
7184:
7176:
7173:
7172:
7156:
7153:
7152:
7136:
7133:
7132:
7115:
7110:
7109:
7101:
7098:
7097:
7081:
7078:
7077:
7061:
7058:
7057:
7037:homotopy theory
6954:singular points
6855:
6807:Morse functions
6774:
6760:
6757:
6756:
6740:
6726:
6723:
6722:
6697:
6694:
6693:
6682:
6643:covering spaces
6615:
6606:sphere eversion
6590:
6562:
6530:
6524:
6512:
6506:
6501:
6487:
6473:
6430:
6425:
6424:
6422:
6419:
6418:
6397:
6392:
6391:
6389:
6386:
6385:
6382:
6376:
6371:
6234:
6228:
6185:Poisson bracket
6135:
6130:
6129:
6127:
6124:
6123:
6095:
6092:
6091:
6075:
6072:
6071:
6068:Riemann surface
6042:
6037:
6036:
6034:
6031:
6030:
6020:
5989:
5986:
5985:
5966:
5946:
5943:
5942:
5935:symmetry groups
5913:
5909:
5907:
5904:
5903:
5877:
5874:
5873:
5872:, the group of
5855:complex numbers
5826:
5823:
5822:
5801:
5795:
5761:
5758:
5757:
5746:
5740:
5729:
5669:
5666:
5665:
5649:
5646:
5645:
5629:
5626:
5625:
5597:
5594:
5593:
5579:
5573:
5561:rectifiable set
5533:tangent vectors
5509:
5503:
5429:
5424:
5423:
5421:
5418:
5417:
5385:
5380:
5379:
5377:
5374:
5373:
5370:
5364:
5359:
5353:
5305:Simon Donaldson
5261:
5237:Hassler Whitney
5189:
5185:
5176:
5172:
5170:
5167:
5166:
5147:
5143:
5135:
5124:
5121:
5120:
5101:
5097:
5089:
5081:
5078:
5077:
5058:
5054:
5046:
5035:
5032:
5031:
5012:
5008:
5000:
4992:
4989:
4988:
4956:
4954:
4951:
4950:
4934:
4931:
4930:
4909:
4907:
4904:
4903:
4887:
4884:
4883:
4856:
4852:
4844:
4842:
4839:
4838:
4813:
4810:
4809:
4768:
4619:
4563:topological map
4525:
4522:
4521:
4423:
4407:
4401:
4358:
4330:
4324:
4250:
4242:Main articles:
4240:
4228:smooth function
4205:
4201:
4190:
4160:
4155:
4154:
4133:
4128:
4127:
4125:
4122:
4121:
4100:
4095:
4094:
4092:
4089:
4088:
4067:
4025:
4010:
3988:
3965:
3959:
3860:
3857:
3856:
3852:
3831:
3826:
3825:
3823:
3820:
3819:
3786:
3782:
3773:
3769:
3760:
3756:
3747:
3742:
3741:
3716:
3712:
3704:
3701:
3700:
3683:
3678:
3677:
3675:
3672:
3671:
3668:
3642:
3637:
3636:
3634:
3631:
3630:
3615:
3607:
3580:
3577:
3576:
3557:
3554:
3553:
3537:
3534:
3533:
3511:
3508:
3507:
3491:
3488:
3487:
3471:
3468:
3467:
3447:
3442:
3437:
3434:
3431:
3430:
3404:
3400:
3395:
3392:
3391:
3375:
3372:
3371:
3349:
3346:
3345:
3322:
3319:
3318:
3302:
3299:
3298:
3277:
3272:
3271:
3269:
3266:
3265:
3249:
3246:
3245:
3223:
3220:
3219:
3203:
3200:
3199:
3179:
3176:
3175:
3172:
3144:
3140:
3138:
3135:
3134:
3133:to points with
3111:
3107:
3105:
3102:
3101:
3075:
3071:
3068: and
3066:
3054:
3049:
3030:
3026:
3011:
3007:
2998:
2994:
2986:
2983:
2982:
2966:
2963:
2962:
2936:
2931:
2912:
2908:
2893:
2889:
2880:
2876:
2868:
2865:
2864:
2848:
2845:
2844:
2793:
2790:
2789:
2773:
2770:
2769:
2754:
2748:
2744:
2741:
2735:
2732:
2726:
2719:
2713:
2675:diffeomorphisms
2657:
2652:
2651:
2649:
2646:
2645:
2638:
2596:
2591:
2590:
2588:
2585:
2584:
2567:
2562:
2561:
2559:
2556:
2555:
2547:
2545:Transition maps
2526:
2520:
2513:
2490:
2485:
2484:
2482:
2479:
2478:
2438:
2433:
2432:
2430:
2427:
2426:
2411:
2405:
2385:
2379:
2373:
2328:
2327:
2311:local dimension
2306:
2281:
2278:
2277:
2256:
2251:
2250:
2248:
2245:
2244:
2227:
2222:
2221:
2219:
2216:
2215:
2184:
2179:
2160:
2155:
2142:
2137:
2124:
2119:
2118:
2106:
2102:
2087:
2083:
2074:
2070:
2066:
2062:
2053:
2048:
2047:
2045:
2042:
2041:
2016:
2013:
2012:
2001:
1981:
1976:
1975:
1973:
1970:
1969:
1967:Euclidean space
1919:Hausdorff space
1886:
1880:
1849:
1845:of points on a
1802: circles,
1788:
1755:
1744:
1737:
1730:
1723:
1701:
1684:
1631:
1623:
1620:
1619:
1587:
1586:
1577:
1573:
1566:
1558:
1556:
1549:
1543:
1542:
1533:
1529:
1522:
1515:
1511:
1504:
1502:
1495:
1488:
1486:
1483:
1482:
1420:
1415:
1375:
1374:
1370:
1368:
1365:
1364:
1340:
1335:
1292:
1291:
1287:
1285:
1282:
1281:
1248:
1247:
1239:
1235:
1227:
1218:
1217:
1204:
1200:
1192:
1185:
1181:
1162:
1161:
1157:
1148:
1147:
1131:
1122:
1110:
1109:
1104:
1100:
1081:
1080:
1076:
1069:
1053:
1051:
1048:
1047:
1019:
1016:
1015:
981:
980:
976:
974:
971:
970:
946:
945:
941:
939:
936:
935:
915:
903:
902:
876:
875:
871:
827:
824:
823:
795:
792:
791:
775:
772:
771:
755:
752:
751:
721:
720:
716:
714:
711:
710:
686:
685:
681:
679:
676:
675:
652:
651:
638:
604:
603:
599:
596:
595:
585:
554:
553:
549:
546:
545:
535:
498:
497:
493:
489:
487:
484:
483:
426:
425:
421:
419:
416:
415:
357:
352:
253:, and also the
207:
204:
203:
173:
170:
169:
152:
149:
148:
145:Euclidean space
93:
82:
76:
73:
63:Please help to
62:
46:
42:
35:
28:
23:
22:
15:
12:
11:
5:
9862:
9852:
9851:
9846:
9829:
9828:
9826:
9825:
9820:
9818:Woldemar Voigt
9815:
9810:
9805:
9800:
9795:
9790:
9785:
9783:Leonhard Euler
9780:
9775:
9770:
9765:
9759:
9757:
9755:Mathematicians
9751:
9750:
9747:
9746:
9744:
9743:
9738:
9733:
9728:
9723:
9718:
9713:
9708:
9703:
9697:
9695:
9691:
9690:
9688:
9687:
9682:
9680:Torsion tensor
9677:
9672:
9667:
9662:
9657:
9652:
9646:
9644:
9637:
9633:
9632:
9630:
9629:
9624:
9619:
9614:
9609:
9604:
9599:
9594:
9589:
9584:
9579:
9574:
9569:
9564:
9559:
9554:
9549:
9544:
9539:
9533:
9531:
9525:
9524:
9522:
9521:
9515:
9513:Tensor product
9510:
9505:
9503:Symmetrization
9500:
9495:
9493:Lie derivative
9490:
9485:
9480:
9475:
9470:
9464:
9462:
9456:
9455:
9453:
9452:
9447:
9442:
9437:
9432:
9427:
9422:
9417:
9415:Tensor density
9412:
9407:
9401:
9399:
9393:
9392:
9390:
9389:
9387:Voigt notation
9384:
9379:
9374:
9372:Ricci calculus
9369:
9364:
9359:
9357:Index notation
9354:
9349:
9343:
9341:
9337:
9336:
9333:
9332:
9330:
9329:
9324:
9319:
9314:
9309:
9303:
9301:
9299:
9298:
9293:
9287:
9284:
9283:
9281:
9280:
9275:
9273:Tensor algebra
9270:
9265:
9260:
9255:
9253:Dyadic algebra
9250:
9245:
9239:
9237:
9228:
9224:
9223:
9216:
9213:
9212:
9205:
9204:
9197:
9190:
9182:
9173:
9172:
9170:
9169:
9164:
9159:
9154:
9149:
9148:
9147:
9137:
9132:
9127:
9122:
9117:
9112:
9106:
9104:
9100:
9099:
9097:
9096:
9091:
9086:
9081:
9076:
9071:
9065:
9063:
9059:
9058:
9055:
9054:
9052:
9051:
9046:
9041:
9036:
9031:
9026:
9021:
9016:
9011:
9006:
9000:
8998:
8992:
8991:
8989:
8988:
8983:
8978:
8973:
8968:
8963:
8958:
8948:
8943:
8938:
8928:
8923:
8918:
8913:
8908:
8903:
8897:
8895:
8889:
8888:
8886:
8885:
8880:
8875:
8874:
8873:
8863:
8858:
8857:
8856:
8846:
8841:
8836:
8831:
8830:
8829:
8819:
8814:
8813:
8812:
8802:
8797:
8791:
8789:
8785:
8784:
8782:
8781:
8776:
8771:
8766:
8765:
8764:
8754:
8749:
8744:
8738:
8736:
8729:
8723:
8722:
8720:
8719:
8714:
8704:
8699:
8685:
8680:
8675:
8670:
8665:
8663:Parallelizable
8660:
8655:
8650:
8649:
8648:
8638:
8633:
8628:
8623:
8618:
8613:
8608:
8603:
8598:
8593:
8583:
8573:
8567:
8565:
8559:
8558:
8556:
8555:
8550:
8545:
8543:Lie derivative
8540:
8538:Integral curve
8535:
8530:
8525:
8524:
8523:
8513:
8508:
8507:
8506:
8499:Diffeomorphism
8496:
8490:
8488:
8482:
8481:
8479:
8478:
8473:
8468:
8463:
8458:
8453:
8448:
8443:
8438:
8432:
8430:
8421:
8420:
8418:
8417:
8412:
8407:
8402:
8397:
8392:
8387:
8382:
8377:
8376:
8375:
8370:
8360:
8359:
8358:
8347:
8345:
8344:Basic concepts
8341:
8340:
8328:
8327:
8320:
8313:
8305:
8299:
8298:
8292:manifold atlas
8288:
8282:
8262:
8261:External links
8259:
8258:
8257:
8250:
8235:
8225:
8222:Famously terse
8201:
8200:
8199:
8187:
8157:
8142:
8124:
8110:
8105:
8075:
8057:
8039:
8018:
8003:
7981:
7966:Hirsch, Morris
7963:
7948:
7930:
7910:
7907:
7905:
7904:
7871:
7842:(3): 435â467.
7826:
7769:
7734:
7715:(3): 645â680.
7696:
7678:(in Russian).
7668:ArnolÊčd, V. I.
7659:
7641:
7628:
7621:
7595:
7588:
7569:
7547:
7545:
7542:
7541:
7540:
7531:
7525:
7519:
7511:
7508:
7507:
7506:
7501:
7495:
7490:
7484:
7478:
7470:
7467:
7466:
7465:
7453:
7450:
7447:
7444:
7441:
7421:
7401:
7381:
7361:
7358:
7354:
7348:
7344:
7340:
7337:
7334:
7329:
7325:
7320:
7316:
7313:
7293:
7290:
7285:
7281:
7277:
7274:
7271:
7266:
7262:
7240:
7236:
7233:
7212:
7207:
7202:
7197:
7191:
7187:
7183:
7180:
7160:
7140:
7118:
7113:
7108:
7105:
7085:
7065:
7054:
7051:
7043:
7040:
7028:
7025:
6998:
6995:
6950:
6931:
6928:
6905:
6902:
6891:Fréchet spaces
6875:Hilbert spaces
6859:
6854:
6851:
6809:, which yield
6781:
6777:
6773:
6770:
6767:
6764:
6743:
6739:
6736:
6733:
6730:
6707:
6704:
6701:
6681:
6678:
6611:Main article:
6589:
6586:
6561:
6558:
6554:quotient space
6526:Main article:
6523:
6520:
6508:Main article:
6505:
6502:
6483:Main article:
6472:
6469:
6433:
6428:
6400:
6395:
6378:Main article:
6375:
6372:
6370:
6367:
6302:, coming from
6257:surgery theory
6227:
6224:
6223:
6222:
6209:
6192:
6167:
6164:Fréchet spaces
6152:
6138:
6133:
6114:
6102:
6099:
6079:
6045:
6040:
6019:
6016:
5999:
5996:
5993:
5973:
5969:
5965:
5962:
5959:
5956:
5953:
5950:
5916:
5912:
5887:
5884:
5881:
5842:
5839:
5836:
5833:
5830:
5806:, named after
5797:Main article:
5794:
5791:
5771:
5768:
5765:
5742:Main article:
5739:
5736:
5685:
5682:
5679:
5676:
5673:
5653:
5633:
5613:
5610:
5607:
5604:
5601:
5575:Main article:
5572:
5569:
5505:Main article:
5502:
5499:
5432:
5427:
5388:
5383:
5366:Main article:
5363:
5360:
5355:Main article:
5352:
5349:
5337:Sergei Novikov
5260:
5257:
5206:
5203:
5200:
5197:
5192:
5188:
5184:
5179:
5175:
5150:
5146:
5142:
5139:
5134:
5131:
5128:
5104:
5100:
5096:
5093:
5088:
5085:
5061:
5057:
5053:
5050:
5045:
5042:
5039:
5015:
5011:
5007:
5004:
4999:
4996:
4982:transition map
4974:et inversement
4962:
4959:
4938:
4915:
4912:
4891:
4866:
4862:
4859:
4855:
4850:
4847:
4826:
4823:
4820:
4817:
4772:Analysis Situs
4767:
4764:
4690:Henri Poincaré
4682:Liouville tori
4656:, Jacobi, and
4654:Siméon Poisson
4618:
4615:
4547:
4544:
4541:
4538:
4535:
4532:
4529:
4512:(or corners),
4499:Leonhard Euler
4422:
4419:
4417:and topology.
4415:linear algebra
4400:
4397:
4357:
4354:
4326:Main article:
4323:
4320:
4254:quotient space
4239:
4236:
4213:
4208:
4204:
4200:
4197:
4193:
4189:
4186:
4183:
4180:
4177:
4174:
4171:
4168:
4163:
4158:
4153:
4150:
4147:
4144:
4141:
4136:
4131:
4103:
4098:
4066:
4060:
4048:intrinsic view
4033:extrinsic view
4024:
4021:
4006:
3984:
3963:Surgery theory
3958:
3955:
3906:
3903:
3900:
3897:
3894:
3891:
3888:
3885:
3882:
3879:
3876:
3873:
3870:
3867:
3864:
3834:
3829:
3805:
3801:
3797:
3794:
3789:
3785:
3781:
3776:
3772:
3768:
3763:
3759:
3755:
3750:
3745:
3740:
3737:
3734:
3731:
3728:
3725:
3722:
3719:
3715:
3711:
3708:
3686:
3681:
3667:
3664:
3645:
3640:
3614:
3611:
3606:
3603:
3590:
3587:
3584:
3564:
3561:
3541:
3521:
3518:
3515:
3495:
3475:
3450:
3445:
3440:
3418:
3415:
3412:
3407:
3403:
3399:
3379:
3359:
3356:
3353:
3329:
3326:
3306:
3280:
3275:
3253:
3233:
3230:
3227:
3207:
3183:
3171:
3168:
3155:
3152:
3147:
3143:
3122:
3119:
3114:
3110:
3089:
3086:
3083:
3078:
3074:
3065:
3062:
3057:
3052:
3048:
3044:
3041:
3038:
3033:
3029:
3025:
3022:
3019:
3014:
3010:
3006:
3001:
2997:
2993:
2990:
2970:
2950:
2947:
2944:
2939:
2934:
2930:
2926:
2923:
2920:
2915:
2911:
2907:
2904:
2901:
2896:
2892:
2888:
2883:
2879:
2875:
2872:
2852:
2809:
2806:
2803:
2800:
2797:
2777:
2752:
2739:
2730:
2712:
2709:
2660:
2655:
2637:
2634:
2630:transition map
2599:
2594:
2570:
2565:
2546:
2543:
2522:Main article:
2519:
2516:
2511:
2493:
2488:
2456:homeomorphisms
2441:
2436:
2421:, or simply a
2415:coordinate map
2407:Main article:
2404:
2401:
2375:Main article:
2372:
2369:
2335:disjoint union
2291:
2288:
2285:
2259:
2254:
2230:
2225:
2203:
2199:
2195:
2192:
2187:
2182:
2178:
2174:
2171:
2168:
2163:
2158:
2154:
2150:
2145:
2140:
2136:
2132:
2127:
2122:
2117:
2114:
2109:
2105:
2101:
2098:
2095:
2090:
2086:
2082:
2077:
2073:
2069:
2065:
2061:
2056:
2051:
2026:
2023:
2020:
2009:isolated point
1989:
1984:
1979:
1879:
1876:
1787:
1784:
1776:nautical chart
1716:
1715:
1683:
1680:
1638:
1635:
1630:
1627:
1580:
1576:
1572:
1569:
1564:
1561:
1555:
1552:
1550:
1548:
1545:
1544:
1536:
1532:
1528:
1525:
1518:
1514:
1510:
1507:
1501:
1498:
1496:
1494:
1491:
1490:
1481:) is given by
1429:
1426:
1423:
1419:
1414:
1411:
1408:
1405:
1402:
1399:
1396:
1393:
1387:
1384:
1381:
1378:
1373:
1349:
1346:
1343:
1339:
1334:
1331:
1328:
1325:
1322:
1319:
1316:
1313:
1307:
1304:
1301:
1298:
1295:
1290:
1266:transition map
1242:
1238:
1234:
1231:
1226:
1223:
1221:
1219:
1215:
1207:
1203:
1199:
1196:
1191:
1188:
1184:
1177:
1174:
1171:
1168:
1165:
1160:
1156:
1153:
1151:
1149:
1145:
1140:
1137:
1134:
1128:
1125:
1119:
1116:
1113:
1108:
1103:
1096:
1093:
1090:
1087:
1084:
1079:
1075:
1072:
1070:
1068:
1065:
1062:
1059:
1056:
1055:
1035:
1032:
1029:
1026:
1023:
996:
993:
990:
987:
984:
979:
955:
952:
949:
944:
921:
918:
912:
909:
906:
901:
897:
891:
888:
885:
882:
879:
874:
870:
867:
864:
861:
858:
855:
852:
849:
846:
843:
840:
837:
834:
831:
811:
808:
805:
802:
799:
779:
759:
736:
733:
730:
727:
724:
719:
695:
692:
689:
684:
650:
647:
644:
641:
639:
637:
634:
631:
628:
625:
619:
616:
613:
610:
607:
602:
598:
597:
594:
591:
588:
586:
584:
581:
578:
575:
572:
566:
563:
560:
557:
552:
548:
547:
544:
541:
538:
536:
534:
531:
528:
525:
522:
516:
513:
510:
507:
504:
501:
496:
492:
491:
462:
459:
456:
453:
450:
447:
444:
441:
435:
432:
429:
424:
356:
353:
351:
348:
299:to be done. A
211:
177:
156:
95:
94:
49:
47:
40:
26:
9:
6:
4:
3:
2:
9861:
9850:
9847:
9845:
9842:
9841:
9839:
9824:
9821:
9819:
9816:
9814:
9811:
9809:
9806:
9804:
9801:
9799:
9796:
9794:
9791:
9789:
9786:
9784:
9781:
9779:
9776:
9774:
9771:
9769:
9766:
9764:
9761:
9760:
9758:
9756:
9752:
9742:
9739:
9737:
9734:
9732:
9729:
9727:
9724:
9722:
9719:
9717:
9714:
9712:
9709:
9707:
9704:
9702:
9699:
9698:
9696:
9692:
9686:
9683:
9681:
9678:
9676:
9673:
9671:
9668:
9666:
9663:
9661:
9660:Metric tensor
9658:
9656:
9653:
9651:
9648:
9647:
9645:
9641:
9638:
9634:
9628:
9625:
9623:
9620:
9618:
9615:
9613:
9610:
9608:
9605:
9603:
9600:
9598:
9595:
9593:
9590:
9588:
9585:
9583:
9580:
9578:
9575:
9573:
9572:Exterior form
9570:
9568:
9565:
9563:
9560:
9558:
9555:
9553:
9550:
9548:
9545:
9543:
9540:
9538:
9535:
9534:
9532:
9526:
9519:
9516:
9514:
9511:
9509:
9506:
9504:
9501:
9499:
9496:
9494:
9491:
9489:
9486:
9484:
9481:
9479:
9476:
9474:
9471:
9469:
9466:
9465:
9463:
9461:
9457:
9451:
9448:
9446:
9445:Tensor bundle
9443:
9441:
9438:
9436:
9433:
9431:
9428:
9426:
9423:
9421:
9418:
9416:
9413:
9411:
9408:
9406:
9403:
9402:
9400:
9394:
9388:
9385:
9383:
9380:
9378:
9375:
9373:
9370:
9368:
9365:
9363:
9360:
9358:
9355:
9353:
9350:
9348:
9345:
9344:
9342:
9338:
9328:
9325:
9323:
9320:
9318:
9315:
9313:
9310:
9308:
9305:
9304:
9302:
9297:
9294:
9292:
9289:
9288:
9285:
9279:
9276:
9274:
9271:
9269:
9266:
9264:
9261:
9259:
9256:
9254:
9251:
9249:
9246:
9244:
9241:
9240:
9238:
9236:
9232:
9229:
9225:
9221:
9220:
9214:
9210:
9203:
9198:
9196:
9191:
9189:
9184:
9183:
9180:
9168:
9165:
9163:
9162:Supermanifold
9160:
9158:
9155:
9153:
9150:
9146:
9143:
9142:
9141:
9138:
9136:
9133:
9131:
9128:
9126:
9123:
9121:
9118:
9116:
9113:
9111:
9108:
9107:
9105:
9101:
9095:
9092:
9090:
9087:
9085:
9082:
9080:
9077:
9075:
9072:
9070:
9067:
9066:
9064:
9060:
9050:
9047:
9045:
9042:
9040:
9037:
9035:
9032:
9030:
9027:
9025:
9022:
9020:
9017:
9015:
9012:
9010:
9007:
9005:
9002:
9001:
8999:
8997:
8993:
8987:
8984:
8982:
8979:
8977:
8974:
8972:
8969:
8967:
8964:
8962:
8959:
8957:
8953:
8949:
8947:
8944:
8942:
8939:
8937:
8933:
8929:
8927:
8924:
8922:
8919:
8917:
8914:
8912:
8909:
8907:
8904:
8902:
8899:
8898:
8896:
8894:
8890:
8884:
8883:Wedge product
8881:
8879:
8876:
8872:
8869:
8868:
8867:
8864:
8862:
8859:
8855:
8852:
8851:
8850:
8847:
8845:
8842:
8840:
8837:
8835:
8832:
8828:
8827:Vector-valued
8825:
8824:
8823:
8820:
8818:
8815:
8811:
8808:
8807:
8806:
8803:
8801:
8798:
8796:
8793:
8792:
8790:
8786:
8780:
8777:
8775:
8772:
8770:
8767:
8763:
8760:
8759:
8758:
8757:Tangent space
8755:
8753:
8750:
8748:
8745:
8743:
8740:
8739:
8737:
8733:
8730:
8728:
8724:
8718:
8715:
8713:
8709:
8705:
8703:
8700:
8698:
8694:
8690:
8686:
8684:
8681:
8679:
8676:
8674:
8671:
8669:
8666:
8664:
8661:
8659:
8656:
8654:
8651:
8647:
8644:
8643:
8642:
8639:
8637:
8634:
8632:
8629:
8627:
8624:
8622:
8619:
8617:
8614:
8612:
8609:
8607:
8604:
8602:
8599:
8597:
8594:
8592:
8588:
8584:
8582:
8578:
8574:
8572:
8569:
8568:
8566:
8560:
8554:
8551:
8549:
8546:
8544:
8541:
8539:
8536:
8534:
8531:
8529:
8526:
8522:
8521:in Lie theory
8519:
8518:
8517:
8514:
8512:
8509:
8505:
8502:
8501:
8500:
8497:
8495:
8492:
8491:
8489:
8487:
8483:
8477:
8474:
8472:
8469:
8467:
8464:
8462:
8459:
8457:
8454:
8452:
8449:
8447:
8444:
8442:
8439:
8437:
8434:
8433:
8431:
8428:
8424:Main results
8422:
8416:
8413:
8411:
8408:
8406:
8405:Tangent space
8403:
8401:
8398:
8396:
8393:
8391:
8388:
8386:
8383:
8381:
8378:
8374:
8371:
8369:
8366:
8365:
8364:
8361:
8357:
8354:
8353:
8352:
8349:
8348:
8346:
8342:
8337:
8333:
8326:
8321:
8319:
8314:
8312:
8307:
8306:
8303:
8297:
8293:
8289:
8286:
8283:
8279:
8275:
8274:
8269:
8265:
8264:
8253:
8247:
8243:
8242:
8236:
8233:
8229:
8226:
8223:
8219:
8218:0-8053-9021-9
8215:
8211:
8210:
8205:
8202:
8197:
8193:
8192:
8188:
8185:
8181:
8180:
8176:
8175:
8173:
8172:3-253-03059-8
8169:
8165:
8161:
8158:
8155:
8151:
8147:
8143:
8140:
8139:0-13-181629-2
8136:
8132:
8128:
8125:
8108:
8093:
8092:0-201-51035-9
8089:
8085:
8084:
8079:
8076:
8073:
8072:0-691-04833-9
8069:
8065:
8061:
8058:
8055:
8054:0-387-90271-6
8051:
8047:
8043:
8040:
8037:
8033:
8032:0-387-95495-3
8029:
8025:
8024:
8019:
8016:
8015:0-387-98759-2
8012:
8008:
8004:
8001:
7997:
7996:0-691-08190-5
7993:
7989:
7985:
7982:
7979:
7978:0-387-90148-5
7975:
7971:
7967:
7964:
7961:
7960:0-8218-3695-1
7957:
7953:
7949:
7946:
7945:0-13-212605-2
7942:
7938:
7934:
7931:
7928:
7927:0-691-08577-3
7924:
7920:
7916:
7913:
7912:
7899:
7894:
7890:
7886:
7882:
7875:
7867:
7863:
7859:
7855:
7850:
7845:
7841:
7837:
7830:
7822:
7818:
7814:
7810:
7806:
7802:
7797:
7792:
7788:
7784:
7780:
7773:
7765:
7761:
7757:
7753:
7749:
7745:
7738:
7730:
7726:
7722:
7718:
7714:
7710:
7706:
7700:
7690:
7685:
7681:
7677:
7673:
7669:
7663:
7655:
7651:
7645:
7638:
7632:
7624:
7622:0-8218-1045-6
7618:
7614:
7609:
7608:
7599:
7591:
7589:9780534133092
7585:
7581:
7580:
7572:
7570:9789812791818
7566:
7562:
7561:
7552:
7548:
7535:
7532:
7529:
7526:
7523:
7520:
7517:
7514:
7513:
7505:
7502:
7499:
7496:
7494:
7491:
7488:
7485:
7482:
7479:
7476:
7473:
7472:
7448:
7445:
7442:
7419:
7399:
7379:
7359:
7356:
7352:
7346:
7342:
7338:
7335:
7332:
7327:
7323:
7318:
7314:
7311:
7291:
7288:
7283:
7279:
7275:
7272:
7269:
7264:
7260:
7234:
7231:
7210:
7205:
7195:
7185:
7181:
7178:
7158:
7138:
7116:
7106:
7103:
7083:
7063:
7055:
7052:
7048:
7044:
7041:
7038:
7033:
7029:
7026:
7023:
7019:
7015:
7011:
7007:
7003:
6999:
6996:
6993:
6989:
6988:
6982:
6978:
6977:
6971:
6967:
6963:
6959:
6955:
6951:
6948:
6944:
6940:
6935:
6932:
6929:
6926:
6925:finite groups
6922:
6918:
6914:
6913:singularities
6910:
6906:
6903:
6900:
6896:
6892:
6888:
6884:
6883:Banach spaces
6880:
6876:
6872:
6868:
6864:
6860:
6857:
6856:
6850:
6848:
6844:
6840:
6836:
6832:
6828:
6824:
6820:
6816:
6812:
6808:
6803:
6801:
6797:
6792:
6779:
6768:
6765:
6762:
6734:
6731:
6728:
6705:
6702:
6699:
6691:
6686:
6677:
6675:
6671:
6667:
6663:
6658:
6656:
6652:
6648:
6644:
6640:
6636:
6632:
6628:
6624:
6620:
6614:
6607:
6603:
6599:
6598:Morin surface
6594:
6585:
6583:
6579:
6575:
6574:Betti numbers
6571:
6567:
6557:
6555:
6551:
6543:
6542:Boy's surface
6539:
6534:
6529:
6519:
6517:
6511:
6500:
6495:
6493:
6486:
6477:
6468:
6466:
6462:
6458:
6453:
6451:
6450:
6431:
6416:
6415:ordered basis
6398:
6381:
6374:Orientability
6366:
6364:
6360:
6356:
6352:
6351:
6346:
6342:
6340:
6336:
6332:
6328:
6323:
6321:
6317:
6313:
6312:orientability
6309:
6305:
6301:
6296:
6294:
6289:
6287:
6283:
6282:
6277:
6272:
6268:
6266:
6260:
6258:
6254:
6250:
6246:
6242:
6237:
6233:
6220:
6216:
6215:
6210:
6207:
6203:
6199:
6198:
6193:
6190:
6186:
6182:
6178:
6174:
6173:
6168:
6165:
6161:
6160:Banach spaces
6157:
6153:
6136:
6121:
6120:
6115:
6100:
6097:
6077:
6069:
6065:
6061:
6043:
6028:
6027:
6022:
6021:
6015:
6013:
5997:
5994:
5991:
5971:
5967:
5960:
5957:
5954:
5948:
5940:
5936:
5932:
5914:
5910:
5901:
5885:
5882:
5879:
5871:
5867:
5862:
5860:
5856:
5837:
5831:
5820:
5815:
5813:
5809:
5805:
5800:
5790:
5787:
5785:
5766:
5755:
5751:
5745:
5735:
5732:
5725:
5723:
5722:vector fields
5719:
5715:
5711:
5707:
5703:
5699:
5680:
5677:
5674:
5651:
5631:
5608:
5605:
5602:
5592:
5591:inner product
5588:
5587:tangent space
5584:
5578:
5568:
5566:
5562:
5557:
5555:
5551:
5547:
5546:
5541:
5536:
5534:
5530:
5527:. This is an
5526:
5525:tangent space
5522:
5518:
5514:
5508:
5498:
5495:
5491:
5487:
5482:
5480:
5476:
5471:
5468:
5464:
5460:
5456:
5451:
5446:
5430:
5415:
5412:
5408:
5407:homeomorphism
5404:
5386:
5369:
5358:
5348:
5346:
5342:
5338:
5334:
5333:Stephen Smale
5330:
5326:
5322:
5318:
5314:
5310:
5306:
5302:
5298:
5294:
5290:
5286:
5282:
5278:
5274:
5273:Poul Heegaard
5270:
5266:
5256:
5254:
5250:
5246:
5242:
5238:
5234:
5230:
5226:
5224:
5220:
5204:
5201:
5198:
5195:
5190:
5186:
5182:
5177:
5173:
5148:
5144:
5140:
5137:
5132:
5129:
5126:
5102:
5098:
5094:
5091:
5086:
5083:
5059:
5055:
5051:
5048:
5043:
5040:
5037:
5013:
5009:
5005:
5002:
4997:
4994:
4985:
4983:
4979:
4975:
4960:
4957:
4936:
4913:
4910:
4889:
4881:
4864:
4860:
4857:
4853:
4848:
4845:
4821:
4815:
4807:
4802:
4800:
4796:
4792:
4788:
4784:
4779:
4777:
4773:
4763:
4761:
4757:
4753:
4749:
4745:
4741:
4737:
4733:
4729:
4726:
4722:
4718:
4714:
4710:
4706:
4702:
4698:
4693:
4691:
4687:
4683:
4679:
4675:
4671:
4667:
4663:
4659:
4655:
4651:
4646:
4644:
4640:
4636:
4632:
4628:
4624:
4614:
4612:
4608:
4604:
4603:Betti numbers
4600:
4596:
4592:
4588:
4584:
4580:
4576:
4572:
4568:
4564:
4545:
4542:
4539:
4536:
4533:
4530:
4527:
4519:
4515:
4511:
4508:
4504:
4500:
4496:
4492:
4487:
4485:
4481:
4480:ambient space
4477:
4473:
4468:
4466:
4462:
4458:
4454:
4450:
4446:
4442:
4438:
4434:
4430:
4426:
4418:
4416:
4412:
4406:
4392:
4388:
4386:
4382:
4379: Ă
4378:
4374:
4370:
4365:
4363:
4353:
4351:
4347:
4342:
4339:
4334:
4329:
4319:
4317:
4313:
4308:
4306:
4302:
4298:
4294:
4290:
4286:
4282:
4278:
4273:
4271:
4267:
4263:
4259:
4255:
4249:
4245:
4235:
4233:
4229:
4224:
4211:
4206:
4198:
4191:
4187:
4181:
4178:
4172:
4161:
4145:
4134:
4120:, defined as
4119:
4101:
4086:
4082:
4078:
4075:
4073:
4064:
4059:
4057:
4053:
4052:normal bundle
4049:
4044:
4042:
4038:
4034:
4030:
4020:
4018:
4014:
4009:
4004:
4000:
3996:
3992:
3987:
3982:
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3969:
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3954:
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3933:
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3898:
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3868:
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3850:
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3803:
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3783:
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3757:
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3748:
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3729:
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3713:
3709:
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3663:
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3610:
3602:
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3585:
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3539:
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3516:
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3493:
3473:
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3443:
3413:
3410:
3405:
3401:
3377:
3357:
3354:
3351:
3343:
3327:
3304:
3296:
3278:
3251:
3231:
3228:
3225:
3205:
3197:
3181:
3167:
3153:
3150:
3145:
3141:
3120:
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3112:
3108:
3084:
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3076:
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3063:
3060:
3055:
3050:
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3027:
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3017:
3012:
3008:
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2999:
2995:
2968:
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2913:
2909:
2905:
2902:
2899:
2894:
2890:
2886:
2881:
2877:
2850:
2841:
2839:
2835:
2831:
2827:
2823:
2820:-manifold. A
2804:
2801:
2798:
2775:
2767:
2763:
2751:
2738:
2729:
2723:
2718:
2708:
2706:
2701:
2699:
2694:
2692:
2688:
2684:
2680:
2676:
2658:
2642:
2633:
2631:
2627:
2623:
2619:
2615:
2597:
2568:
2553:
2542:
2540:
2539:maximal atlas
2535:
2533:
2532:
2525:
2515:
2509:
2491:
2476:
2472:
2468:
2464:
2459:
2457:
2439:
2424:
2420:
2416:
2410:
2400:
2398:
2394:
2390:
2384:
2378:
2368:
2366:
2362:
2358:
2354:
2350:
2348:
2344:
2340:
2336:
2332:
2329:pure manifold
2324:
2320:
2316:
2312:
2303:
2289:
2286:
2283:
2275:
2274:diffeomorphic
2257:
2228:
2201:
2197:
2193:
2190:
2185:
2180:
2176:
2172:
2169:
2166:
2161:
2156:
2152:
2148:
2143:
2138:
2134:
2130:
2125:
2115:
2107:
2103:
2099:
2096:
2093:
2088:
2084:
2080:
2075:
2071:
2063:
2059:
2054:
2040:
2024:
2021:
2018:
2010:
2005:
1987:
1982:
1968:
1964:
1960:
1956:
1952:
1950:
1946:
1942:
1938:
1934:
1930:
1926:
1922:
1920:
1917:
1912:
1910:
1909:diffeomorphic
1906:
1902:
1898:
1893:
1891:
1885:
1875:
1873:
1869:
1863:
1860:
1856:
1852:
1848:
1844:
1840:
1836:
1832:
1828:
1823:
1821:
1797:
1792:
1783:
1781:
1777:
1773:
1769:
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1761:
1758:
1751:
1747:
1740:
1733:
1726:
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1712:
1708:
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1700:
1699:
1698:
1697:
1693:
1689:
1679:
1677:
1673:
1668:
1666:
1662:
1658:
1654:
1636:
1633:
1628:
1625:
1617:
1613:
1609:
1606: +
1605:
1600:
1578:
1574:
1570:
1567:
1562:
1559:
1553:
1551:
1546:
1534:
1530:
1526:
1523:
1516:
1512:
1508:
1505:
1499:
1497:
1492:
1480:
1476:
1472:
1468:
1464:
1460:
1456:
1452:
1448:
1443:
1427:
1424:
1421:
1417:
1412:
1409:
1406:
1400:
1397:
1394:
1371:
1347:
1344:
1341:
1337:
1332:
1329:
1326:
1320:
1317:
1314:
1288:
1274:
1270:
1268:
1267:
1261:
1240:
1236:
1232:
1229:
1224:
1222:
1213:
1205:
1201:
1197:
1194:
1189:
1186:
1182:
1158:
1154:
1152:
1143:
1138:
1135:
1132:
1126:
1123:
1106:
1101:
1077:
1073:
1071:
1063:
1057:
1030:
1027:
1024:
1013:
977:
942:
919:
916:
899:
895:
872:
868:
862:
859:
856:
844:
841:
838:
832:
829:
806:
803:
800:
777:
757:
717:
682:
672:
670:
665:
648:
645:
642:
640:
632:
629:
626:
600:
592:
589:
587:
579:
576:
573:
550:
542:
539:
537:
529:
526:
523:
494:
481:
480:
474:
460:
457:
454:
448:
445:
442:
422:
413:
412:open interval
409:
406:
402:
398:
394:
390:
386:
384:
379:
376: +
375:
371:
361:
347:
345:
340:
338:
334:
330:
326:
322:
318:
315:serve as the
314:
310:
306:
302:
298:
294:
290:
285:
283:
279:
275:
271:
267:
262:
260:
256:
252:
248:
244:
240:
236:
232:
228:
223:
209:
201:
197:
193:
189:
175:
154:
146:
142:
138:
134:
126:
122:
118:
113:
106:
101:
91:
88:
80:
70:
66:
60:
59:
53:
48:
39:
38:
33:
19:
9823:Hermann Weyl
9627:Vector space
9612:Pseudotensor
9596:
9577:Fiber bundle
9530:abstractions
9425:Mixed tensor
9410:Tensor field
9217:
9089:Moving frame
9084:Morse theory
9074:Gauge theory
8866:Tensor field
8795:Closed/Exact
8774:Vector field
8742:Distribution
8683:Hypercomplex
8678:Quaternionic
8415:Vector field
8373:Smooth atlas
8331:
8271:
8240:
8231:
8207:
8195:
8189:
8183:
8177:
8163:
8145:
8130:
8081:
8063:
8060:Milnor, John
8045:
8035:
8021:
8006:
7987:
7969:
7951:
7936:
7918:
7888:
7884:
7874:
7849:math/9304210
7839:
7835:
7829:
7786:
7782:
7772:
7747:
7743:
7737:
7712:
7708:
7699:
7679:
7675:
7662:
7653:
7650:Poincaré, H.
7644:
7631:
7606:
7598:
7578:
7559:
7551:
7510:By dimension
7027:CW-complexes
6991:
6984:
6980:
6973:
6968:are largely
6965:
6964:and English
6961:
6957:
6934:Non-singular
6916:
6804:
6793:
6720:
6659:
6616:
6563:
6549:
6547:
6513:
6510:Klein bottle
6504:Klein bottle
6491:
6488:
6485:Möbius strip
6479:Möbius strip
6471:Möbius strip
6461:Klein bottle
6457:Möbius strip
6454:
6447:
6383:
6348:
6343:
6324:
6297:
6290:
6285:
6279:
6275:
6273:
6269:
6261:
6243:, except in
6241:in principle
6240:
6238:
6235:
6212:
6195:
6170:
6117:
6024:
5939:hyperspheres
5900:real numbers
5863:
5816:
5803:
5802:
5788:
5749:
5747:
5730:
5726:
5582:
5580:
5558:
5554:power series
5543:
5539:
5537:
5528:
5520:
5512:
5510:
5489:
5485:
5483:
5472:
5458:
5454:
5449:
5447:
5371:
5345:Morse theory
5264:
5262:
5241:foundational
5229:Hermann Weyl
5227:
4986:
4928:
4879:
4805:
4803:
4798:
4780:
4775:
4769:
4755:
4751:
4747:
4743:
4735:
4731:
4727:
4724:
4720:
4716:
4712:
4704:
4696:
4694:
4647:
4620:
4594:
4590:
4586:
4578:
4574:
4570:
4566:
4517:
4513:
4506:
4488:
4469:
4427:
4424:
4408:
4384:
4380:
4376:
4366:
4359:
4350:Möbius strip
4343:
4335:
4331:
4309:
4304:
4300:
4296:
4292:
4288:
4284:
4274:
4266:well-behaved
4262:CW complexes
4251:
4231:
4225:
4084:
4080:
4076:
4071:
4068:
4062:
4047:
4045:
4032:
4026:
4016:
4012:
4007:
4002:
3998:
3994:
3990:
3985:
3980:
3978:
3970:
3966:
3952:
3947:
3943:
3939:
3935:
3931:
3927:
3921:
3855:defined by
3848:
3817:
3669:
3659:
3628:
3622:
3608:
3605:Construction
3465:
3294:
3195:
3173:
2842:
2761:
2759:
2749:
2736:
2727:
2705:pseudogroups
2702:
2697:
2695:
2643:
2639:
2629:
2625:
2621:
2617:
2613:
2551:
2548:
2538:
2536:
2529:
2527:
2507:
2470:
2466:
2462:
2460:
2422:
2418:
2414:
2412:
2396:
2392:
2386:
2351:
2338:
2326:
2314:
2310:
2304:
2006:
1959:homeomorphic
1954:
1953:
1944:
1936:
1935:conditions;
1928:
1924:
1923:
1913:
1894:
1887:
1864:
1858:
1854:
1850:
1824:
1817:
1814: cubic.
1786:Other curves
1765:
1762:
1756:
1749:
1745:
1738:
1731:
1724:
1722:: the plane
1717:
1710:
1706:
1702:
1685:
1675:
1671:
1669:
1664:
1660:
1656:
1652:
1615:
1611:
1607:
1603:
1601:
1478:
1474:
1470:
1466:
1462:
1458:
1454:
1450:
1446:
1444:
1279:
1265:
1262:
1011:
673:
666:
477:
475:
392:
388:
382:
377:
373:
366:
341:
317:phase spaces
286:
263:
255:Klein bottle
224:
196:homeomorphic
192:neighborhood
168:
136:
130:
105:Klein bottle
83:
74:
55:
9763:Ălie Cartan
9711:Spin tensor
9685:Weyl tensor
9643:Mathematics
9607:Multivector
9398:definitions
9296:Engineering
9235:Mathematics
9034:Levi-Civita
9024:Generalized
8996:Connections
8946:Lie algebra
8878:Volume form
8779:Vector flow
8752:Pushforward
8747:Lie bracket
8646:Lie algebra
8611:G-structure
8400:Pushforward
8380:Submanifold
7952:3-Manifolds
7891:: 251â272.
7750:(1): 1â14.
7705:Whitney, H.
7689:10.4213/rm5
7475:Submanifold
6952:Because of
6923:of various
6839:heat kernel
6800:functionals
6639:submersions
6631:knot theory
6629:, of which
6413:. Given an
6245:dimension 4
6119:CR manifold
6060:holomorphic
5450:topological
5329:John Milnor
5223:submanifold
4670:Hamiltonian
4662:phase space
4573:edges, and
4516:edges, and
4453:Lobachevsky
1963:open subset
1847:cubic curve
1692:unit sphere
385:-coordinate
370:unit circle
268:and modern
200:open subset
133:mathematics
125:South Poles
69:introducing
9838:Categories
9592:Linear map
9460:Operations
9157:Stratifold
9115:Diffeology
8911:Associated
8712:Symplectic
8697:Riemannian
8626:Hyperbolic
8553:Submersion
8461:HopfâRinow
8395:Submersion
8390:Smooth map
8268:"Manifold"
7909:References
7796:2303.04200
7789:: 105114.
7528:5-manifold
7522:4-manifold
7516:3-manifold
7032:CW complex
7002:filtration
6970:synonymous
6811:handlebody
6692:of degree
6635:immersions
6627:embeddings
6582:cohomology
6516:cross-caps
6497:See also:
6449:orientable
6281:invariants
5808:Sophus Lie
5804:Lie groups
5793:Lie groups
5718:divergence
5459:consistent
5455:particular
4666:Lagrangian
4569:vertices,
4037:tangential
3342:complement
3317:, denoted
3218:, denoted
2826:1-manifold
2766:2-manifold
2715:See also:
2698:compatible
2465:called an
2381:See also:
2323:dimensions
1868:components
1841:, and the
405:invertible
401:continuous
397:projection
249:, and the
233:, but not
52:references
9844:Manifolds
9731:EM tensor
9567:Dimension
9518:Transpose
9039:Principal
9014:Ehresmann
8971:Subbundle
8961:Principal
8936:Fibration
8916:Cotangent
8788:Covectors
8641:Lie group
8621:Hermitian
8564:manifolds
8533:Immersion
8528:Foliation
8466:Noether's
8451:Frobenius
8446:De Rham's
8441:Darboux's
8332:Manifolds
8278:EMS Press
7968:, (1997)
7821:0393-0440
7764:120977898
7555:E.g. see
7432:. A pair
7357:∈
7336:…
7315:∘
7289:∈
7273:…
7235:∈
7190:∞
7182:∈
7107:⊆
6960:, German
6904:Orbifolds
6837:, and to
6772:→
6766::
6738:→
6732::
6602:immersion
6550:antipodes
6286:invariant
6276:different
5995:−
5958:−
5883:×
5832:
5799:Lie group
5770:‖
5767:⋅
5764:‖
5714:curvature
5684:⟩
5672:⟨
5612:⟩
5609:⋅
5603:⋅
5600:⟨
5494:connected
5486:dimension
5475:Hausdorff
5411:bijective
5325:René Thom
5313:spacetime
5249:Lie group
5196:−
5141:−
5133:−
5095:−
5052:−
5044:−
5006:−
4980:and of a
4846:θ
4816:θ
4783:level set
4740:induction
4635:Jacobians
4617:Synthesis
4531:−
4465:curvature
4373:cylinders
4338:bijection
4258:orbifolds
4203:‖
4196:‖
4185:↦
4167:∖
4152:→
4140:∖
3957:Patchwork
3924:unit disc
3863:χ
3754:∣
3739:∈
3586:−
3560:∂
3517:
3355:
3340:, is the
3325:∂
3229:
3082:≥
3043:Σ
3021:…
2925:Σ
2903:…
2802:−
2391:, called
2319:connected
2315:dimension
2170:⋯
2116:∈
2097:…
2039:open ball
1945:Hausdorff
1941:long line
1933:point-set
1929:Hausdorff
1839:hyperbola
1831:countable
1820:connected
1509:−
1425:−
1372:χ
1289:χ
1233:−
1198:−
1159:χ
1124:−
1107:χ
1078:χ
978:χ
943:χ
917:−
900:χ
896:∘
873:χ
851:→
718:χ
683:χ
601:χ
551:χ
495:χ
423:χ
414:(â1, 1):
333:spacetime
305:distances
188:-manifold
77:July 2021
9597:Manifold
9582:Geodesic
9340:Notation
9135:Orbifold
9130:K-theory
9120:Diffiety
8844:Pullback
8658:Oriented
8636:Kenmotsu
8616:Hadamard
8562:Types of
8511:Geodesic
8336:Glossary
8131:Topology
8000:category
7670:(1998).
7481:Geodesic
7469:See also
7224:, where
6966:manifold
6909:orbifold
6604:used in
6578:homology
6369:Surfaces
6359:homotopy
6355:homology
6329:and the
6316:homology
6251:and the
6204:made by
5866:matrices
5550:analytic
5517:calculus
5277:Max Dehn
5265:surfaces
5221:, every
4961:′
4914:′
4861:′
4849:′
4725:diskrete
4707:, which
4697:manifold
4510:vertices
4503:polytope
4491:property
4441:Saccheri
4279:, which
4244:Orbifold
4083:-sphere
4029:embedded
4015:= 0 and
3660:manifold
3295:boundary
3196:interior
2469:, whose
2345:), each
1943:, while
1835:parabola
1046:, then:
389:Figure 1
344:topology
297:calculus
291:; their
282:CT scans
266:geometry
239:surfaces
194:that is
137:manifold
9694:Physics
9528:Related
9291:Physics
9209:Tensors
9079:History
9062:Related
8976:Tangent
8954:)
8934:)
8901:Adjoint
8893:Bundles
8871:density
8769:Torsion
8735:Vectors
8727:Tensors
8710:)
8695:)
8691:,
8689:Pseudoâ
8668:Poisson
8601:Finsler
8596:Fibered
8591:Contact
8589:)
8581:Complex
8579:)
8548:Section
8280:, 2001
8230:(1999)
8206:(1965)
8129:(2000)
8080:(1991)
8062:(1997)
8044:(1977)
7866:2118532
7801:Bibcode
7729:1968482
7050:theory.
6958:variété
6947:sheaves
6943:Schemes
6921:actions
6331:torsion
5859:modulus
5819:compact
5710:volumes
4929:...les
4776:variété
4476:surface
4439:fails.
4399:History
4074:-sphere
3506:, then
2628:, or a
2518:Atlases
1965:of the
1780:atlases
1713:â 1 = 0
1477:,
1465:,
1453:,
408:mapping
319:in the
295:allows
276:and as
231:circles
65:improve
9622:Vector
9617:Spinor
9602:Matrix
9396:Tensor
9044:Vector
9029:Koszul
9009:Cartan
9004:Affine
8986:Vector
8981:Tensor
8966:Spinor
8956:Normal
8952:Stable
8906:Affine
8810:bundle
8762:bundle
8708:Almost
8631:KĂ€hler
8587:Almost
8577:Almost
8571:Closed
8471:Sard's
8427:(list)
8248:
8216:
8170:
8152:
8137:
8090:
8070:
8052:
8030:
8013:
7994:
7976:
7958:
7943:
7925:
7864:
7819:
7762:
7727:
7619:
7586:
7567:
7020:, and
6885:, and
6668:, and
6645:, and
6492:single
6318:) and
6181:2-form
5941:, are
5933:, the
5784:metric
5702:angles
5540:smooth
4703:term,
4701:German
4549:
4520:faces,
4449:Bolyai
4433:Euclid
4411:curves
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355:Circle
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