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In the mathematical field of algebraic topology, the homotopy groups of spheres describe how spheres of various dimensions can wrap around each other. They are examples of topological invariants, which reflect, in algebraic terms, the structure of spheres viewed as topological spaces, forgetting about their precise geometry. Unlike homology groups, which are also topological invariants, the homotopy groups are surprisingly complex and difficult to compute.
The n-dimensional unit sphere — called the n-sphere for brevity, and denoted as S^{n} — generalizes the familiar circle (S^{1}) and the ordinary sphere (S^{2}). The n-sphere may be defined geometrically as the set of points in a Euclidean space of dimension n + 1 located at a unit distance from the origin. The i-th homotopy group π_{i}(S^{n}) summarizes the different ways in which the i-dimensional sphere S^{i} can be mapped continuously into the n-dimensional sphere S^{n}. This summary does not distinguish between two mappings if one can be continuously deformed to the other; thus, only equivalence classes of mappings are summarized. An "addition" operation defined on these equivalence classes makes the set of equivalence classes into an abelian group.
The problem of determining π_{i}(S^{n}) falls into three regimes, depending on whether i is less than, equal to, or greater than n:
The question of computing the homotopy group π_{n+k}(S^{n}) for positive k turned out to be a central question in algebraic topology that has contributed to development of many of its fundamental techniques and has served as a stimulating focus of research. One of the main discoveries is that the homotopy groups π_{n+k}(S^{n}) are independent of n for n ≥ k + 2. These are called the stable homotopy groups of spheres and have been computed for values of k up to 64. The stable homotopy groups form the coefficient ring of an extraordinary cohomology theory, called stable cohomotopy theory. The unstable homotopy groups (for n < k + 2) are more erratic; nevertheless, they have been tabulated for k < 20. Most modern computations use spectral sequences, a technique first applied to homotopy groups of spheres by Jean-Pierre Serre. Several important patterns have been established, yet much remains unknown and unexplained.
The study of homotopy groups of spheres builds on a great deal of background material, here briefly reviewed. Algebraic topology provides the larger context, itself built on topology and abstract algebra, with homotopy groups as a basic example.
An ordinary sphere in three-dimensional space — the surface, not the solid ball — is just one example of what a sphere means in topology. Geometry defines a sphere rigidly, as a shape. Here are some alternatives.
Some theory requires selecting a fixed point on the sphere, calling the pair (sphere, point) a pointed sphere. For some spaces the choice matters, but for a sphere all points are equivalent so the choice is a matter of convenience.^{ [4]} For spheres constructed as a repeated suspension, the point (1, 0, 0, ..., 0), which is on the equator of all the levels of suspension, works well; for the disk with collapsed rim, the point resulting from the collapse of the rim is another obvious choice.
The distinguishing feature of a topological space is its continuity structure, formalized in terms of open sets or neighborhoods. A continuous map is a function between spaces that preserves continuity. A homotopy is a continuous path between continuous maps; two maps connected by a homotopy are said to be homotopic.^{ [5]} The idea common to all these concepts is to discard variations that do not affect outcomes of interest. An important practical example is the residue theorem of complex analysis, where "closed curves" are continuous maps from the circle into the complex plane, and where two closed curves produce the same integral result if they are homotopic in the topological space consisting of the plane minus the points of singularity.^{ [6]}
The first homotopy group, or fundamental group, π_{1}(X) of a ( path connected) topological space X thus begins with continuous maps from a pointed circle (S^{1},s) to the pointed space (X,x), where maps from one pair to another map s into x. These maps (or equivalently, closed curves) are grouped together into equivalence classes based on homotopy (keeping the "base point" x fixed), so that two maps are in the same class if they are homotopic. Just as one point is distinguished, so one class is distinguished: all maps (or curves) homotopic to the constant map S^{1}↦x are called null homotopic. The classes become an abstract algebraic group with the introduction of addition, defined via an "equator pinch". This pinch maps the equator of a pointed sphere (here a circle) to the distinguished point, producing a " bouquet of spheres" — two pointed spheres joined at their distinguished point. The two maps to be added map the upper and lower spheres separately, agreeing on the distinguished point, and composition with the pinch gives the sum map.^{ [7]}
More generally, the i-th homotopy group, π_{i}(X) begins with the pointed i-sphere (S^{i}, s), and otherwise follows the same procedure. The null homotopic class acts as the identity of the group addition, and for X equal to S^{n} (for positive n) — the homotopy groups of spheres — the groups are abelian and finitely generated. If for some i all maps are null homotopic, then the group π_{i} consists of one element, and is called the trivial group.^{[ citation needed]}
A continuous map between two topological spaces induces a group homomorphism between the associated homotopy groups. In particular, if the map is a continuous bijection (a homeomorphism), so that the two spaces have the same topology, then their i-th homotopy groups are isomorphic for all i. However, the real plane has exactly the same homotopy groups as a solitary point (as does a Euclidean space of any dimension), and the real plane with a point removed has the same groups as a circle, so groups alone are not enough to distinguish spaces. Although the loss of discrimination power is unfortunate, it can also make certain computations easier.^{[ citation needed]}
The low-dimensional examples of homotopy groups of spheres provide a sense of the subject, because these special cases can be visualized in ordinary 3-dimensional space.^{ [8]} However, such visualizations are not mathematical proofs, and do not capture the possible complexity of maps between spheres.^{[ citation needed]}
The simplest case concerns the ways that a circle (1-sphere) can be wrapped around another circle. This can be visualized by wrapping a rubber band around one's finger: it can be wrapped once, twice, three times and so on. The wrapping can be in either of two directions, and wrappings in opposite directions will cancel out after a deformation. The homotopy group π_{1}(S^{1}) is therefore an infinite cyclic group, and is isomorphic to the group Z of integers under addition: a homotopy class is identified with an integer by counting the number of times a mapping in the homotopy class wraps around the circle. This integer can also be thought of as the winding number of a loop around the origin in the plane.^{ [8]}
The identification (a group isomorphism) of the homotopy group with the integers is often written as an equality: thus π_{1}(S^{1}) = Z.^{ [9]}
Mappings from a 2-sphere to a 2-sphere can be visualized as wrapping a plastic bag around a ball and then sealing it. The sealed bag is topologically equivalent to a 2-sphere, as is the surface of the ball. The bag can be wrapped more than once by twisting it and wrapping it back over the ball. (There is no requirement for the continuous map to be injective and so the bag is allowed to pass through itself.) The twist can be in one of two directions and opposite twists can cancel out by deformation. The total number of twists after cancellation is an integer, called the degree of the mapping. As in the case mappings from the circle to the circle, this degree identifies the homotopy group with the group of integers, Z.
These two results generalize: for all n > 0, π_{n}(S^{n}) = Z (see below).
Any continuous mapping from a circle to an ordinary sphere can be continuously deformed to a one-point mapping, and so its homotopy class is trivial. One way to visualize this is to imagine a rubber-band wrapped around a frictionless ball: the band can always be slid off the ball. The homotopy group is therefore a trivial group, with only one element, the identity element, and so it can be identified with the subgroup of Z consisting only of the number zero. This group is often denoted by 0. Showing this rigorously requires more care, however, due to the existence of space-filling curves.^{ [10]}
This result generalizes to higher dimensions. All mappings from a lower-dimensional sphere into a sphere of higher dimension are similarly trivial: if i < n, then π_{i}(S^{n}) = 0. This can be shown as a consequence of the cellular approximation theorem.^{ [11]}
All the interesting cases of homotopy groups of spheres involve mappings from a higher-dimensional sphere onto one of lower dimension. Unfortunately, the only example which can easily be visualized is not interesting: there are no nontrivial mappings from the ordinary sphere to the circle. Hence, π_{2}(S^{1}) = 0. This is because S^{1} has the real line as its universal cover which is contractible (it has the homotopy type of a point). In addition, because S^{2} is simply connected, by the lifting criterion^{[ citation needed]}, any map from S^{2} to S^{1} can be lifted to a map into the real line and the nullhomotopy descends to the downstairs space.^{[ citation needed]}
The first nontrivial example with i > n concerns mappings from the 3-sphere to the ordinary 2-sphere, and was discovered by Heinz Hopf, who constructed a nontrivial map from S^{3} to S^{2}, now known as the Hopf fibration.^{ [12]} This map generates the homotopy group π_{3}(S^{2}) = Z.^{ [13]}
In the late 19th century Camille Jordan introduced the notion of homotopy and used the notion of a homotopy group, without using the language of group theory.^{ [14]} A more rigorous approach was adopted by Henri Poincaré in his 1895 set of papers Analysis situs where the related concepts of homology and the fundamental group were also introduced.^{ [15]}
Higher homotopy groups were first defined by Eduard Čech in 1932.^{ [16]} (His first paper was withdrawn on the advice of Pavel Sergeyevich Alexandrov and Heinz Hopf, on the grounds that the groups were commutative so could not be the right generalizations of the fundamental group.) Witold Hurewicz is also credited with the introduction of homotopy groups in his 1935 paper and also for the Hurewicz theorem which can be used to calculate some of the groups.^{ [17]} An important method for calculating the various groups is the concept of stable algebraic topology, which finds properties that are independent of the dimensions. Typically these only hold for larger dimensions. The first such result was Hans Freudenthal's suspension theorem, published in 1937. Stable algebraic topology flourished between 1945 and 1966 with many important results.^{ [17]} In 1953 George W. Whitehead showed that there is a metastable range for the homotopy groups of spheres. Jean-Pierre Serre used spectral sequences to show that most of these groups are finite, the exceptions being π_{n}(S^{n}) and π_{4n−1}(S^{2n}). Others who worked in this area included José Adem, Hiroshi Toda, Frank Adams, J. Peter May, Mark Mahowald, Daniel Isaksen, Guozhen Wang, and Zhouli Xu. The stable homotopy groups π_{n+k}(S^{n}) are known for k up to 90, and, as of 2023, unknown for larger k.^{ [18]}
As noted already, when i is less than n, π_{i}(S^{n}) = 0, the trivial group. The reason is that a continuous mapping from an i-sphere to an n-sphere with i < n can always be deformed so that it is not surjective. Consequently, its image is contained in S^{n} with a point removed; this is a contractible space, and any mapping to such a space can be deformed into a one-point mapping.^{ [11]}
The case i = n has also been noted already, and is an easy consequence of the Hurewicz theorem: this theorem links homotopy groups with homology groups, which are generally easier to calculate; in particular, it shows that for a simply-connected space X, the first nonzero homotopy group π_{k}(X), with k > 0, is isomorphic to the first nonzero homology group H_{k}(X). For the n-sphere, this immediately implies that for n ≥ 2, π_{n}(S^{n}) = H_{n}(S^{n}) = Z.^{[ citation needed]}
The homology groups H_{i}(S^{n}), with i > n, are all trivial. It therefore came as a great surprise historically that the corresponding homotopy groups are not trivial in general. This is the case that is of real importance: the higher homotopy groups π_{i}(S^{n}), for i > n, are surprisingly complex and difficult to compute, and the effort to compute them has generated a significant amount of new mathematics.^{[ citation needed]}
The following table gives an idea of the complexity of the higher homotopy groups even for spheres of dimension 8 or less. In this table, the entries are either the
trivial group 0, the infinite cyclic group Z, finite
cyclic groups of order n (written as Z_{n}), or
direct products of such groups (written, for example, as Z_{24}×Z_{3} or Z^{2}
_{2} = Z_{2}×Z_{2}). Extended tables of homotopy groups of spheres are given
at the end of the article.
π_{1} | π_{2} | π_{3} | π_{4} | π_{5} | π_{6} | π_{7} | π_{8} | π_{9} | π_{10} | π_{11} | π_{12} | π_{13} | π_{14} | π_{15} | |
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
S^{0} | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 |
S^{1} | Z | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 |
S^{2} | 0 | Z | Z | Z_{2} | Z_{2} | Z_{12} | Z_{2} | Z_{2} | Z_{3} | Z_{15} | Z_{2} | Z^{2} _{2} |
Z_{12}×Z_{2} | Z_{84}×Z^{2} _{2} |
Z^{2} _{2} |
S^{3} | 0 | 0 | Z | Z_{2} | Z_{2} | Z_{12} | Z_{2} | Z_{2} | Z_{3} | Z_{15} | Z_{2} | Z^{2} _{2} |
Z_{12}×Z_{2} | Z_{84}×Z^{2} _{2} |
Z^{2} _{2} |
S^{4} | 0 | 0 | 0 | Z | Z_{2} | Z_{2} | Z×Z_{12} | Z^{2} _{2} |
Z^{2} _{2} |
Z_{24}×Z_{3} | Z_{15} | Z_{2} | Z^{3} _{2} |
^{Z120×} _{Z12×Z2} |
Z_{84}×Z^{5} _{2} |
S^{5} | 0 | 0 | 0 | 0 | Z | Z_{2} | Z_{2} | Z_{24} | Z_{2} | Z_{2} | Z_{2} | Z_{30} | Z_{2} | Z^{3} _{2} |
Z_{72}×Z_{2} |
S^{6} | 0 | 0 | 0 | 0 | 0 | Z | Z_{2} | Z_{2} | Z_{24} | 0 | Z | Z_{2} | Z_{60} | Z_{24}×Z_{2} | Z^{3} _{2} |
S^{7} | 0 | 0 | 0 | 0 | 0 | 0 | Z | Z_{2} | Z_{2} | Z_{24} | 0 | 0 | Z_{2} | Z_{120} | Z^{3} _{2} |
S^{8} | 0 | 0 | 0 | 0 | 0 | 0 | 0 | Z | Z_{2} | Z_{2} | Z_{24} | 0 | 0 | Z_{2} | Z×Z_{120} |
The first two rows of this table are straightforward. The homotopy groups π_{i}(S^{0}) of the 0-dimensional sphere are trivial for i > 0, because any base point preserving map from an i-sphere to a 0-sphere is a one-point mapping. Similarly, the homotopy groups π_{i}(S^{1}) of the 1-sphere are trivial for i > 1, because the universal covering space, , which has the same higher homotopy groups, is contractible.^{[ citation needed]}
Beyond these two rows, the higher homotopy groups (i > n) appear to be chaotic, but in fact there are many patterns, some obvious and some very subtle.
These patterns follow from many different theoretical results.^{[ citation needed]}
The fact that the groups below the jagged line in the table above are constant along the diagonals is explained by the
suspension theorem of
Hans Freudenthal, which implies that the suspension homomorphism from π_{n+k}(S^{n}) to π_{n+k+1}(S^{n+1}) is an isomorphism for n > k + 1. The groups π_{n+k}(S^{n}) with n > k + 1 are called the stable homotopy groups of spheres, and are denoted π^{S}
_{k}: they are finite abelian groups for k ≠ 0, and have been computed in numerous cases, although the general pattern is still elusive.^{
[19]} For n ≤ k+1, the groups are called the unstable homotopy groups of spheres.^{[
citation needed]}
The classical Hopf fibration is a fiber bundle:
The general theory of fiber bundles F → E → B shows that there is a long exact sequence of homotopy groups
For this specific bundle, each group homomorphism π_{i}(S^{1}) → π_{i}(S^{3}), induced by the inclusion S^{1} → S^{3}, maps all of π_{i}(S^{1}) to zero, since the lower-dimensional sphere S^{1} can be deformed to a point inside the higher-dimensional one S^{3}. This corresponds to the vanishing of π_{1}(S^{3}). Thus the long exact sequence breaks into short exact sequences,
Since S^{n+1} is a suspension of S^{n}, these sequences are split by the suspension homomorphism π_{i−1}(S^{1}) → π_{i}(S^{2}), giving isomorphisms
Since π_{i−1}(S^{1}) vanishes for i at least 3, the first row shows that π_{i}(S^{2}) and π_{i}(S^{3}) are isomorphic whenever i is at least 3, as observed above.
The Hopf fibration may be constructed as follows: pairs of complex numbers (z_{0},z_{1}) with |z_{0}|^{2} + |z_{1}|^{2} = 1 form a 3-sphere, and their ratios z_{0}/z_{1} cover the complex plane plus infinity, a 2-sphere. The Hopf map S^{3} → S^{2} sends any such pair to its ratio.^{[ citation needed]}
Similarly, there are generalized Hopf fibrations
constructed using pairs of quaternions or octonions instead of complex numbers.^{ [20]} Here, too, π_{3}(S^{7}) and π_{7}(S^{15}) are zero. Thus the long exact sequences again break into families of split short exact sequences, implying two families of relations.
The three fibrations have base space S^{n} with n = 2^{m}, for m = 1, 2, 3. A fibration does exist for S^{1} (m = 0), but not for S^{16} (m = 4) and beyond. Although generalizations of the relations to S^{16} are often true, they sometimes fail; for example,
Thus there can be no fibration
the first non-trivial case of the Hopf invariant one problem, because such a fibration would imply that the failed relation is true.^{[ citation needed]}
Homotopy groups of spheres are closely related to
cobordism classes of manifolds.
In 1938
Lev Pontryagin established an isomorphism between the homotopy group π_{n+k}(S^{n}) and the group Ω^{framed}
_{k}(S^{n+k}) of cobordism classes of
differentiable k-submanifolds of S^{n+k} which are "framed", i.e. have a trivialized
normal bundle. Every map f : S^{n+k} → S^{n} is homotopic to a differentiable map with M^{k} = f^{−1}(1, 0, ..., 0) ⊂ S^{n+k} a framed k-dimensional submanifold. For example, π_{n}(S^{n}) = Z is the cobordism group of framed 0-dimensional submanifolds of S^{n}, computed by the algebraic sum of their points, corresponding to the
degree of maps f : S^{n} → S^{n}. The projection of the
Hopf fibration S^{3} → S^{2} represents a generator of π_{3}(S^{2}) = Ω^{framed}
_{1}(S^{3}) = Z which corresponds to the framed 1-dimensional submanifold of S^{3} defined by the standard embedding S^{1} ⊂ S^{3} with a nonstandard trivialization of the normal 2-plane bundle. Until the advent of more sophisticated algebraic methods in the early 1950s (Serre) the Pontrjagin isomorphism was the main tool for computing the homotopy groups of spheres. In 1954 the Pontrjagin isomorphism was generalized by
René Thom to an isomorphism expressing other groups of cobordism classes (e.g. of all manifolds) as
homotopy groups of spaces and
spectra. In more recent work the argument is usually reversed, with cobordism groups computed in terms of homotopy groups.^{
[21]}
In 1951, Jean-Pierre Serre showed that homotopy groups of spheres are all finite except for those of the form π_{n}(S^{n}) or π_{4n−1}(S^{2n}) (for positive n), when the group is the product of the infinite cyclic group with a finite abelian group.^{ [22]} In particular the homotopy groups are determined by their p-components for all primes p. The 2-components are hardest to calculate, and in several ways behave differently from the p-components for odd primes.^{[ citation needed]}
In the same paper, Serre found the first place that p-torsion occurs in the homotopy groups of n dimensional spheres, by showing that π_{n+k}(S^{n}) has no p- torsion if k < 2p − 3, and has a unique subgroup of order p if n ≥ 3 and k = 2p − 3. The case of 2-dimensional spheres is slightly different: the first p-torsion occurs for k = 2p − 3 + 1. In the case of odd torsion there are more precise results; in this case there is a big difference between odd and even dimensional spheres. If p is an odd prime and n = 2i + 1, then elements of the p- component of π_{n+k}(S^{n}) have order at most p^{i}.^{ [23]} This is in some sense the best possible result, as these groups are known to have elements of this order for some values of k.^{ [24]} Furthermore, the stable range can be extended in this case: if n is odd then the double suspension from π_{k}(S^{n}) to π_{k+2}(S^{n+2}) is an isomorphism of p-components if k < p(n + 1) − 3, and an epimorphism if equality holds.^{ [25]} The p-torsion of the intermediate group π_{k+1}(S^{n+1}) can be strictly larger.^{[ citation needed]}
The results above about odd torsion only hold for odd-dimensional spheres: for even-dimensional spheres, the James fibration gives the torsion at odd primes p in terms of that of odd-dimensional spheres,
(where (p) means take the p-component).^{ [26]} This exact sequence is similar to the ones coming from the Hopf fibration; the difference is that it works for all even-dimensional spheres, albeit at the expense of ignoring 2-torsion. Combining the results for odd and even dimensional spheres shows that much of the odd torsion of unstable homotopy groups is determined by the odd torsion of the stable homotopy groups.^{[ citation needed]}
For stable homotopy groups there are more precise results about p-torsion. For example, if k < 2p(p − 1) − 2 for a prime p then the p-primary component of the stable homotopy group π^{S}
_{k} vanishes unless k + 1 is divisible by 2(p − 1), in which case it is cyclic of order p.^{
[27]}
An important subgroup of π_{n+k}(S^{n}), for k ≥ 2, is the image of the J-homomorphism J : π_{k}(SO(n)) → π_{n+k}(S^{n}), where SO(n) denotes the special orthogonal group.^{ [28]} In the stable range n ≥ k + 2, the homotopy groups π_{k}(SO(n)) only depend on k (mod 8). This period 8 pattern is known as Bott periodicity, and it is reflected in the stable homotopy groups of spheres via the image of the J-homomorphism which is:
This last case accounts for the elements of unusually large finite order in π_{n+k}(S^{n}) for such values of k. For example, the stable groups π_{n+11}(S^{n}) have a cyclic subgroup of order 504, the denominator of B_{6}/12 = 1/504.^{[ citation needed]}
The stable homotopy groups of spheres are the direct sum of the image of the J-homomorphism, and the kernel of the Adams e-invariant, a homomorphism from these groups to . Roughly speaking, the image of the J-homomorphism is the subgroup of "well understood" or "easy" elements of the stable homotopy groups. These well understood elements account for most elements of the stable homotopy groups of spheres in small dimensions. The quotient of π^{S}
_{n} by the image of the J-homomorphism is considered to be the "hard" part of the stable homotopy groups of spheres (
Adams 1966). (Adams also introduced certain order 2 elements μ_{n} of π^{S}
_{n} for n ≡ 1 or 2 (mod 8), and these are also considered to be "well understood".) Tables of homotopy groups of spheres sometimes omit the "easy" part im(J) to save space.^{[
citation needed]}
The direct sum
of the stable homotopy groups of spheres is a supercommutative graded ring, where multiplication is given by composition of representing maps, and any element of non-zero degree is nilpotent;^{ [29]} the nilpotence theorem on complex cobordism implies Nishida's theorem.^{[ citation needed]}
Example: If η is the generator of π^{S}
_{1} (of order 2),
then η^{2} is nonzero and generates π^{S}
_{2}, and η^{3} is nonzero and 12 times a generator of π^{S}
_{3}, while η^{4} is zero because the group π^{S}
_{4} is trivial.^{[
citation needed]}
If f and g and h are elements of π^{S}
_{*} with f g = 0 and g⋅h = 0, there is a
Toda bracket ⟨f, g, h⟩ of these elements.^{
[30]} The Toda bracket is not quite an element of a stable homotopy group, because it is only defined up to addition of products of certain other elements.
Hiroshi Toda used the composition product and Toda brackets to label many of the elements of homotopy groups. There are also higher Toda brackets of several elements, defined when suitable lower Toda brackets vanish. This parallels the theory of
Massey products in
cohomology.^{[
citation needed]}
Every element of the stable homotopy groups of spheres can be expressed using composition products and higher Toda brackets in terms of certain well known elements, called Hopf elements.^{
[31]}
If X is any finite simplicial complex with finite fundamental group, in particular if X is a sphere of dimension at least 2, then its homotopy groups are all finitely generated abelian groups. To compute these groups, they are often factored into their p-components for each prime p, and calculating each of these p-groups separately. The first few homotopy groups of spheres can be computed using ad hoc variations of the ideas above; beyond this point, most methods for computing homotopy groups of spheres are based on spectral sequences.^{ [32]} This is usually done by constructing suitable fibrations and taking the associated long exact sequences of homotopy groups; spectral sequences are a systematic way of organizing the complicated information that this process generates.^{[ citation needed]}
The computation of the homotopy groups of S^{2} has been reduced to a combinatorial group theory question. Berrick et al. (2006) identify these homotopy groups as certain quotients of the Brunnian braid groups of S^{2}. Under this correspondence, every nontrivial element in π_{n}(S^{2}) for n > 2 may be represented by a Brunnian braid over S^{2} that is not Brunnian over the disk D^{2}. For example, the Hopf map S^{3} → S^{2} corresponds to the Borromean rings.^{ [40]}
Tables of homotopy groups of spheres are most conveniently organized by showing π_{n+k}(S^{n}).
The following table shows many of the groups π_{n+k}(S^{n}). The stable homotopy groups are highlighted in blue, the unstable ones in red. Each homotopy group is the product of the cyclic groups of the orders given in the table, using the following conventions:^{ [46]}
Example: π_{19}(S^{10}) = π_{9+10}(S^{10}) = Z×Z_{2}×Z_{2}×Z_{2}, which is denoted by ∞⋅2^{3} in the table.
S^{n} → | S^{0} | S^{1} | S^{2} | S^{3} | S^{4} | S^{5} | S^{6} | S^{7} | S^{8} | S^{9} | S^{10} | S^{11} | S^{12} | S^{≥13} |
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
π_{<n}(S^{n}) | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ | |
π_{0+n}(S^{n}) | 2 | ∞ | ∞ | ∞ | ∞ | ∞ | ∞ | ∞ | ∞ | ∞ | ∞ | ∞ | ∞ | ∞ |
π_{1+n}(S^{n}) | ⋅ | ⋅ | ∞ | 2 | 2 | 2 | 2 | 2 | 2 | 2 | 2 | 2 | 2 | 2 |
π_{2+n}(S^{n}) | ⋅ | ⋅ | 2 | 2 | 2 | 2 | 2 | 2 | 2 | 2 | 2 | 2 | 2 | 2 |
π_{3+n}(S^{n}) | ⋅ | ⋅ | 2 | 12 | ∞⋅12 | 24 | 24 | 24 | 24 | 24 | 24 | 24 | 24 | 24 |
π_{4+n}(S^{n}) | ⋅ | ⋅ | 12 | 2 | 2^{2} | 2 | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ |
π_{5+n}(S^{n}) | ⋅ | ⋅ | 2 | 2 | 2^{2} | 2 | ∞ | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ |
π_{6+n}(S^{n}) | ⋅ | ⋅ | 2 | 3 | 24⋅3 | 2 | 2 | 2 | 2 | 2 | 2 | 2 | 2 | 2 |
π_{7+n}(S^{n}) | ⋅ | ⋅ | 3 | 15 | 15 | 30 | 60 | 120 | ∞⋅120 | 240 | 240 | 240 | 240 | 240 |
π_{8+n}(S^{n}) | ⋅ | ⋅ | 15 | 2 | 2 | 2 | 24⋅2 | 2^{3} | 2^{4} | 2^{3} | 2^{2} | 2^{2} | 2^{2} | 2^{2} |
π_{9+n}(S^{n}) | ⋅ | ⋅ | 2 | 2^{2} | 2^{3} | 2^{3} | 2^{3} | 2^{4} | 2^{5} | 2^{4} | ∞⋅2^{3} | 2^{3} | 2^{3} | 2^{3} |
π_{10+n}(S^{n}) | ⋅ | ⋅ | 2^{2} | 12⋅2 | 120⋅12⋅2 | 72⋅2 | 72⋅2 | 24⋅2 | 24^{2}⋅2 | 24⋅2 | 12⋅2 | 6⋅2 | 6 | 6 |
π_{11+n}(S^{n}) | ⋅ | ⋅ | 12⋅2 | 84⋅2^{2} | 84⋅2^{5} | 504⋅2^{2} | 504⋅4 | 504⋅2 | 504⋅2 | 504⋅2 | 504 | 504 | ∞⋅504 | 504 |
π_{12+n}(S^{n}) | ⋅ | ⋅ | 84⋅2^{2} | 2^{2} | 2^{6} | 2^{3} | 240 | ⋅ | ⋅ | ⋅ | 12 | 2 | 2^{2} | See below |
π_{13+n}(S^{n}) | ⋅ | ⋅ | 2^{2} | 6 | 24⋅6⋅2 | 6⋅2 | 6 | 6 | 6⋅2 | 6 | 6 | 6⋅2 | 6⋅2 | |
π_{14+n}(S^{n}) | ⋅ | ⋅ | 6 | 30 | 2520⋅6⋅2 | 6⋅2 | 12⋅2 | 24⋅4 | 240⋅24⋅4 | 16⋅4 | 16⋅2 | 16⋅2 | 48⋅4⋅2 | |
π_{15+n}(S^{n}) | ⋅ | ⋅ | 30 | 30 | 30 | 30⋅2 | 60⋅6 | 120⋅2^{3} | 120⋅2^{5} | 240⋅2^{3} | 240⋅2^{2} | 240⋅2 | 240⋅2 | |
π_{16+n}(S^{n}) | ⋅ | ⋅ | 30 | 6⋅2 | 6^{2}⋅2 | 2^{2} | 504⋅2^{2} | 2^{4} | 2^{7} | 2^{4} | 240⋅2 | 2 | 2 | |
π_{17+n}(S^{n}) | ⋅ | ⋅ | 6⋅2 | 12⋅2^{2} | 24⋅12⋅4⋅2^{2} | 4⋅2^{2} | 2^{4} | 2^{4} | 6⋅2^{4} | 2^{4} | 2^{3} | 2^{3} | 2^{4} | |
π_{18+n}(S^{n}) | ⋅ | ⋅ | 12⋅2^{2} | 12⋅2^{2} | 120⋅12⋅2^{5} | 24⋅2^{2} | 24⋅6⋅2 | 24⋅2 | 504⋅24⋅2 | 24⋅2 | 24⋅2^{2} | 8⋅4⋅2 | 480⋅4^{2}⋅2 | |
π_{19+n}(S^{n}) | ⋅ | ⋅ | 12⋅2^{2} | 132⋅2 | 132⋅2^{5} | 264⋅2 | 1056⋅8 | 264⋅2 | 264⋅2 | 264⋅2 | 264⋅6 | 264⋅2^{3} | 264⋅2^{5} |
S^{n} → | S^{13} | S^{14} | S^{15} | S^{16} | S^{17} | S^{18} | S^{19} | S^{20} | S^{≥21} |
---|---|---|---|---|---|---|---|---|---|
π_{12+n}(S^{n}) | 2 | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ | ⋅ |
π_{13+n}(S^{n}) | 6 | ∞⋅3 | 3 | 3 | 3 | 3 | 3 | 3 | 3 |
π_{14+n}(S^{n}) | 16⋅2 | 8⋅2 | 4⋅2 | 2^{2} | 2^{2} | 2^{2} | 2^{2} | 2^{2} | 2^{2} |
π_{15+n}(S^{n}) | 480⋅2 | 480⋅2 | 480⋅2 | ∞⋅480⋅2 | 480⋅2 | 480⋅2 | 480⋅2 | 480⋅2 | 480⋅2 |
π_{16+n}(S^{n}) | 2 | 24⋅2 | 2^{3} | 2^{4} | 2^{3} | 2^{2} | 2^{2} | 2^{2} | 2^{2} |
π_{17+n}(S^{n}) | 2^{4} | 2^{4} | 2^{5} | 2^{6} | 2^{5} | ∞⋅2^{4} | 2^{4} | 2^{4} | 2^{4} |
π_{18+n}(S^{n}) | 8^{2}⋅2 | 8^{2}⋅2 | 8^{2}⋅2 | 24⋅8^{2}⋅2 | 8^{2}⋅2 | 8⋅4⋅2 | 8⋅2^{2} | 8⋅2 | 8⋅2 |
π_{19+n}(S^{n}) | 264⋅2^{3} | 264⋅4⋅2 | 264⋅2^{2} | 264⋅2^{2} | 264⋅2^{2} | 264⋅2 | 264⋅2 | ∞⋅264⋅2 | 264⋅2 |
The stable homotopy groups π^{S}
_{k} are the products of cyclic groups of the infinite or prime power orders shown in the table. (For largely historical reasons, stable homotopy groups are usually given as products of cyclic groups of prime power order, while tables of unstable homotopy groups often give them as products of the smallest number of cyclic groups.) The main complexity is in the 2-, 3-, and 5-components: For p > 5, the p-components in the range of the table are accounted for by the J-homomorphism and are cyclic of order p if 2(p − 1) divides k + 1 and 0 otherwise.^{
[47]} The mod 8 behavior of the table comes from
Bott periodicity via the
J-homomorphism, whose image is underlined.
n → | 0 | 1 | 2 | 3 | 4 | 5 | 6 | 7 |
---|---|---|---|---|---|---|---|---|
π_{0+n}^{S} | ∞ | 2 | 2 | 8⋅3 | ⋅ | ⋅ | 2 | 16⋅3⋅5 |
π_{8+n}^{S} | 2⋅2 | 2⋅2^{2} | 2⋅3 | 8⋅9⋅7 | ⋅ | 3 | 2^{2} | 32⋅2⋅3⋅5 |
π_{16+n}^{S} | 2⋅2 | 2⋅2^{3} | 8⋅2 | 8⋅2⋅3⋅11 | 8⋅3 | 2^{2} | 2⋅2 | 16⋅8⋅2⋅9⋅3⋅5⋅7⋅13 |
π_{24+n}^{S} | 2⋅2 | 2⋅2 | 2^{2}⋅3 | 8⋅3 | 2 | 3 | 2⋅3 | 64⋅2^{2}⋅3⋅5⋅17 |
π_{32+n}^{S} | 2⋅2^{3} | 2⋅2^{4} | 4⋅2^{3} | 8⋅2^{2}⋅27⋅7⋅19 | 2⋅3 | 2^{2}⋅3 | 4⋅2⋅3⋅5 | 16⋅2^{5}⋅3⋅3⋅25⋅11 |
π_{40+n}^{S} | 2⋅4⋅2^{4}⋅3 | 2⋅2^{4} | 8⋅2^{2}⋅3 | 8⋅3⋅23 | 8 | 16⋅2^{3}⋅9⋅5 | 2^{4}⋅3 | 32⋅4⋅2^{3}⋅9⋅3⋅5⋅7⋅13 |
π_{48+n}^{S} | 2⋅4⋅2^{3} | 2⋅2⋅3 | 2^{3}⋅3 | 8⋅8⋅2⋅3 | 2^{3}⋅3 | 2^{4} | 4⋅2 | 16⋅3⋅3⋅5⋅29 |
π_{56+n}^{S} | 2 | 2⋅2^{2} | 2^{2} | 8⋅2^{2}⋅9⋅7⋅11⋅31 | 4 | ⋅ | 2^{4}⋅3 | 128⋅4⋅2^{2}⋅3⋅5⋅17 |
π_{64+n}^{S} | 2⋅4⋅2^{5} | 2⋅4⋅2^{8}⋅3 | 8⋅2^{6} | 8⋅4⋅2^{3}⋅3 | 2^{3}⋅3 | 2^{4} | 4^{2}⋅2^{5} | 16⋅8⋅4⋅2^{6}⋅27⋅5⋅7⋅13⋅19⋅37 |
π_{72+n}^{S} | 2⋅2^{7}⋅3 | 2⋅2^{6} | 4^{3}⋅2⋅3 | 8⋅2⋅9⋅3 | 4⋅2^{2}⋅5 | 4⋅2^{5} | 4^{2}⋅2^{3}⋅3 | 32⋅4⋅2^{6}⋅3⋅25⋅11⋅41 |