Postnikov system

{{Short description|In mathematics, a topological construction}}

In homotopy theory, a branch of algebraic topology, a Postnikov system (or Postnikov tower) is a way of decomposing a topological space by filtering its homotopy type. What this looks like is for a space X there is a list of spaces \{X_n\}_{n \geq 0} where

\pi_k(X_n) = \begin{cases}

\pi_k(X) & \text{ for } k \leq n \\

0 & \text{ for } k > n

\end{cases}

and there is a series of maps \phi_n: X_n \to X_{n-1} that are fibrations with fibers Eilenberg-MacLane spaces K(\pi_n(X),n). In short, we are decomposing the homotopy type of X using an inverse system of topological spaces whose homotopy type at degree k agrees with the truncated homotopy type of the original space X. Postnikov systems were introduced by, and are named after, Mikhail Postnikov.

There is a similar construction called the Whitehead tower (defined below) where instead of having spaces X_n with the homotopy type of X for degrees \leq n, these spaces have null homotopy groups \pi_{k}(X_n) =0 for 1 < k < n.

Definition

A Postnikov system of a path-connected space X is an inverse system of spaces

: \cdots \to X_n \xrightarrow{p_n} X_{n-1}\xrightarrow{p_{n-1}} \cdots \xrightarrow{p_3} X_2 \xrightarrow{p_2} X_1 \xrightarrow{p_1} *

with a sequence of maps \phi_n : X \to X_n compatible with the inverse system such that

  1. The map \phi_n : X \to X_n induces an isomorphism \pi_i(X) \to \pi_i(X_n) for every i\leq n.
  2. \pi_i(X_n) = 0 for i > n.{{Cite book|last=Hatcher|first=Allen|author-link=Allen Hatcher|url=https://pi.math.cornell.edu/~hatcher/AT/AT.pdf|title=Algebraic Topology}}{{rp|410}}
  3. Each map p_n : X_n \to X_{n-1} is a fibration, and so the fiber F_n is an Eilenberg–MacLane space, K(\pi_n(X),n).

The first two conditions imply that X_1 is also a K(\pi_1(X),1)-space. More generally, if X is (n-1)-connected, then X_n is a K(\pi_n(X),n)-space and all X_{i} for i < n are contractible. Note the third condition is only included optionally by some authors.

= Existence =

Postnikov systems exist on connected CW complexes,{{rp|354}} and there is a weak homotopy-equivalence between X and its inverse limit, so

: X\simeq\varprojlim{}X_n,

showing that X is a CW approximation of its inverse limit. They can be constructed on a CW complex by iteratively killing off homotopy groups. If we have a map f : S^{n} \to X representing a homotopy class [f]\in\pi_n(X), we can take the pushout along the boundary map S^{n} \to e_{n+1}, killing off the homotopy class. For X_{m} this process can be repeated for all n > m , giving a space which has vanishing homotopy groups \pi_n(X_m) . Using the fact that X_{n-1} can be constructed from X_n by killing off all homotopy maps S^n \to X_{n}, we obtain a map X_n \to X_{n-1}.

= Main property =

One of the main properties of the Postnikov tower, which makes it so powerful to study while computing cohomology, is the fact the spaces X_n are homotopic to a CW complex \mathfrak{X}_n which differs from X only by cells of dimension \geq n+2.

= Homotopy classification of fibrations =

The sequence of fibrations p_n:X_n \to X_{n-1}{{Cite journal|last=Kahn|first=Donald W.|date=1963-03-01|title=Induced maps for Postnikov systems|url=https://www.ams.org/journals/tran/1963-107-03/S0002-9947-1963-0150777-X/S0002-9947-1963-0150777-X.pdf|journal=Transactions of the American Mathematical Society| volume=107|issue=3|pages=432–450|doi=10.1090/s0002-9947-1963-0150777-x|issn=0002-9947|doi-access=free}} have homotopically defined invariants, meaning the homotopy classes of maps p_n, give a well defined homotopy type [X] \in \operatorname{Ob}(hTop). The homotopy class of p_n comes from looking at the homotopy class of the classifying map for the fiber K(\pi_n(X), n). The associated classifying map is

:X_{n-1} \to B(K(\pi_n(X),n)) \simeq K(\pi_n(X),n+1),

hence the homotopy class [p_n] is classified by a homotopy class

:[p_n] \in [X_{n-1},K(\pi_n(X), n+1)] \cong H^{n+1}(X_{n-1}, \pi_n(X))

called the nth Postnikov invariant of X, since the homotopy classes of maps to Eilenberg-Maclane spaces gives cohomology with coefficients in the associated abelian group.

== Fiber sequence for spaces with two nontrivial homotopy groups ==

One of the special cases of the homotopy classification is the homotopy class of spaces X such that there exists a fibration

:K(A,n) \to X \to \pi_1(X)

giving a homotopy type with two non-trivial homotopy groups, \pi_1(X) = G, and \pi_n(X) = A. Then, from the previous discussion, the fibration map BG \to K(A,n+1) gives a cohomology class in

:H^{n+1}(BG, A),

which can also be interpreted as a group cohomology class. This space X can be considered a higher local system.

Examples of Postnikov towers

= Postnikov tower of a ''K''(''G'', ''n'') =

One of the conceptually simplest cases of a Postnikov tower is that of the Eilenberg–Maclane space K(G,n). This gives a tower with

:\begin{matrix}

X_i \simeq * &\text{for } i < n \\

X_i \simeq K(G,n) & \text{for } i \geq n

\end{matrix}

= Postnikov tower of ''S''<sup>2</sup> =

The Postnikov tower for the sphere S^2 is a special case whose first few terms can be understood explicitly. Since we have the first few homotopy groups from the simply connectedness of S^2, degree theory of spheres, and the Hopf fibration, giving \pi_k(S^2) \simeq \pi_k(S^3) for k \geq 3, hence

: \begin{matrix}

\pi_1(S^2) =& 0 \\

\pi_2(S^2) =& \Z \\

\pi_3(S^2) =& \Z \\

\pi_4(S^2) =& \Z/2.

\end{matrix}

Then, X_2 = S^2_2 = K(\Z,2), and X_3 comes from a pullback sequence

: \begin{matrix}

X_3 & \to & * \\

\downarrow & & \downarrow \\

X_2 & \to & K(\Z,4) ,

\end{matrix}

which is an element in

: [p_3] \in [K(\Z,2), K(\Z,4)] \cong H^4(\mathbb{CP}^\infty) = \Z.

If this was trivial it would imply X_3 \simeq K(\Z,2)\times K(\Z,3). But, this is not the case! In fact, this is responsible for why strict infinity groupoids don't model homotopy types.{{cite arXiv|last=Simpson|first=Carlos|author-link=Carlos Simpson|date=1998-10-09|title=Homotopy types of strict 3-groupoids|eprint=math/9810059}} Computing this invariant requires more work, but can be explicitly found.{{Cite journal|last1=Eilenberg|first1=Samuel|author1-link=Samuel Eilenberg|last2=MacLane|first2=Saunders|author2-link=Saunders MacLane|date=1954|title=On the Groups H(\Pi, n), III: Operations and Obstructions|jstor=1969849|journal=Annals of Mathematics|volume=60|issue=3|pages=513–557|doi=10.2307/1969849|issn=0003-486X}} This is the quadratic form x \mapsto x^2 on \Z \to \Z coming from the Hopf fibration S^3 \to S^2. Note that each element in H^4(\mathbb{CP}^\infty) gives a different homotopy 3-type.

Homotopy groups of spheres

One application of the Postnikov tower is the computation of homotopy groups of spheres.{{Cite web|last=Laurențiu-George|first=Maxim|title=Spectral sequences and homotopy groups of spheres|url=https://www.math.wisc.edu/~maxim/753f13w7.pdf|url-status=live|archive-url=https://web.archive.org/web/20170519125745/https://www.math.wisc.edu/~maxim/753f13w7.pdf|archive-date=19 May 2017}} For an n-dimensional sphere S^n we can use the Hurewicz theorem to show each S^n_i is contractible for i < n, since the theorem implies that the lower homotopy groups are trivial. Recall there is a spectral sequence for any Serre fibration, such as the fibration

: K(\pi_{n+1}(X), n + 1) \simeq F_{n+1} \to S^n_{n+1} \to S^n_n \simeq K(\Z, n).

We can then form a homological spectral sequence with E^2-terms

: E^2_{p,q} = H_p\left(K(\Z, n), H_q\left(K\left(\pi_{n+1}\left(S^n\right), n + 1\right)\right)\right).

And the first non-trivial map to \pi_{n+1}\left(S^n\right),

: d^{n+1}_{0,n+1} : H_{n+2}(K(\Z, n)) \to H_0\left(K(\Z, n), H_{n+1}\left(K\left(\pi_{n+1}\left(S^n\right), n + 1\right)\right)\right),

equivalently written as

: d^{n+1}_{0,n+1} : H_{n+2}(K(\Z, n)) \to \pi_{n+1}\left(S^n\right).

If it's easy to compute H_{n+1}\left(S^n_{n+1}\right) and H_{n+2}\left(S^n_{n+2}\right), then we can get information about what this map looks like. In particular, if it's an isomorphism, we obtain a computation of \pi_{n+1}\left(S^n\right). For the case n = 3, this can be computed explicitly using the path fibration for K(\Z, 3), the main property of the Postnikov tower for \mathfrak{X}_4 \simeq S^3 \cup \{\text{cells of dimension} \geq 6\} (giving H_4(X_4) = H_5(X_4) = 0, and the universal coefficient theorem giving \pi_4\left(S^3\right) = \Z/2. Moreover, because of the Freudenthal suspension theorem this actually gives the stable homotopy group \pi_1^\mathbb{S} since \pi_{n+k}\left(S^n\right) is stable for n \geq k + 2.

Note that similar techniques can be applied using the Whitehead tower (below) for computing \pi_4\left(S^3\right) and \pi_5\left(S^3\right), giving the first two non-trivial stable homotopy groups of spheres.

Postnikov towers of spectra

In addition to the classical Postnikov tower, there is a notion of Postnikov towers in stable homotopy theory constructed on spectra{{Cite book|url=http://link.springer.com/10.1007/978-3-540-77751-9|title=On Thom Spectra, Orientability, and Cobordism|date=1998|publisher=Springer|isbn=978-3-540-62043-3|series=Springer Monographs in Mathematics|location=Berlin, Heidelberg|language=en|doi=10.1007/978-3-540-77751-9}}pg 85-86.

= Definition =

For a spectrum E a postnikov tower of E is a diagram in the homotopy category of spectra, \text{Ho}(\textbf{Spectra}), given by

: \cdots \to E_{(2)} \xrightarrow{p_2} E_{(1)} \xrightarrow{p_1} E_{(0)} ,

with maps

: \tau_n : E \to E_{(n)}

commuting with the p_n maps. Then, this tower is a Postnikov tower if the following two conditions are satisfied:

  1. \pi_i^{\mathbb{S}}\left(E_{(n)}\right) = 0 for i > n,
  2. \left(\tau_n\right)_* : \pi_i^{\mathbb{S}}(E) \to \pi_i^{\mathbb{S}}\left(E_{(n)}\right) is an isomorphism for i \leq n,

where \pi_i^{\mathbb{S}} are stable homotopy groups of a spectrum. It turns out every spectrum has a Postnikov tower and this tower can be constructed using a similar kind of inductive procedure as the one given above.

Whitehead tower

Given a CW complex X, there is a dual construction to the Postnikov tower called the Whitehead tower. Instead of killing off all higher homotopy groups, the Whitehead tower iteratively kills off lower homotopy groups. This is given by a tower of CW complexes,

: \cdots \to X_3 \to X_2 \to X_1 \to X,

where

  1. The lower homotopy groups are zero, so \pi_i(X_n) = 0 for i \leq n.
  2. The induced map \pi_i : \pi_i(X_n) \to \pi_i(X) is an isomorphism for i > n.
  3. The maps X_n \to X_{n-1} are fibrations with fiber K(\pi_n(X), n-1).

= Implications =

Notice X_1 \to X is the universal cover of X since it is a covering space with a simply connected cover. Furthermore, each X_n \to X is the universal n-connected cover of X.

= Construction =

The spaces X_n in the Whitehead tower are constructed inductively. If we construct a K\left(\pi_{n+1}(X), n + 1\right) by killing off the higher homotopy groups in X_n,{{Cite web|url=https://www.math.wisc.edu/~maxim/754notes.pdf|title=Lecture Notes on Homotopy Theory and Applications|first=Laurențiu|last=Maxim|page=66|url-status=live|archive-url=https://web.archive.org/web/20200216062602/https://www.math.wisc.edu/~maxim/754notes.pdf|archive-date=16 February 2020}} we get an embedding X_n \to K(\pi_{n+1}(X), n + 1). If we let

: X_{n+1} = \left\{f\colon I \to K\left(\pi_{n+1}(X), n + 1\right) : f(0) = p \text{ and } f(1) \in X_{n} \right\}

for some fixed basepoint p, then the induced map X_{n+1} \to X_n is a fiber bundle with fiber homeomorphic to

: \Omega K\left(\pi_{n+1}(X), n + 1\right) \simeq K\left(\pi_{n+1}(X), n\right),

and so we have a Serre fibration

: K\left(\pi_{n+1}(X), n\right) \to X_n \to X_{n-1}.

Using the long exact sequence in homotopy theory, we have that \pi_i(X_n) = \pi_i\left(X_{n-1}\right) for i \geq n + 1, \pi_i(X_n) = \pi_i(X_{n-1}) = 0 for i < n-1, and finally, there is an exact sequence

: 0 \to \pi_{n+1}\left(X_{n+1}) \to \pi_{n+1}(X_{n}\right) \mathrel{\overset{\partial}{\rightarrow}} \pi_{n}K\left(\pi_{n+1}(X), n\right) \to \pi_{n}\left(X_{n+1}\right) \to 0,

where if the middle morphism is an isomorphism, the other two groups are zero. This can be checked by looking at the inclusion X_n \to K(\pi_{n+1}(X), n + 1) and noting that the Eilenberg–Maclane space has a cellular decomposition

: X_{n-1} \cup \{\text{cells of dimension} \geq n + 2\}; thus,

: \pi_{n+1}\left(X_n\right) \cong \pi_{n+1}\left(K\left(\pi_{n+1}(X), n + 1\right)\right) \cong \pi_n\left(K\left(\pi_{n+1}(X), n\right)\right),

giving the desired result.

= As a homotopy fiber =

Another way to view the components in the Whitehead tower is as a homotopy fiber. If we take

: \text{Hofiber}(\phi_n: X \to X_n)

from the Postnikov tower, we get a space X^n which has

: \pi_k(X^n) = \begin{cases}

\pi_k(X) & k > n \\

0 & k \leq n

\end{cases}

Whitehead tower of spectra

The dual notion of the Whitehead tower can be defined in a similar manner using homotopy fibers in the category of spectra. If we let

: E\langle n \rangle = \operatorname{Hofiber}\left(\tau_n: E \to E_{(n)}\right)

then this can be organized in a tower giving connected covers of a spectrum. This is a widely used construction{{Cite journal|last=Hill|first=Michael A.|date=2009|title=The string bordism of BE8 and BE8 × BE8 through dimension 14|url=https://projecteuclid.org/euclid.ijm/1264170845|journal=Illinois Journal of Mathematics|language=EN|volume=53|issue=1|pages=183–196|doi=10.1215/ijm/1264170845|issn=0019-2082|doi-access=free}}{{Cite journal|date=2014-12-01|title=Secondary invariants for string bordism and topological modular forms|journal=Bulletin des Sciences Mathématiques|language=en|volume=138|issue=8|pages=912–970|doi=10.1016/j.bulsci.2014.05.002|issn=0007-4497|doi-access=free|last1=Bunke|first1=Ulrich|last2=Naumann|first2=Niko}}{{cite book|last=Szymik|first=Markus|year=2019|chapter=String bordism and chromatic characteristics|editor1=Daniel G. Davis|editor2=Hans-Werner Henn|editor3=J. F. Jardine|editor4=Mark W. Johnson|editor5=Charles Rezk|title=Homotopy Theory: Tools and Applications|series=Contemporary Mathematics|volume=729|pages=239–254|doi=10.1090/conm/729/14698|arxiv=1312.4658|isbn=9781470442446|s2cid=56461325}} in bordism theory because the coverings of the unoriented cobordism spectrum M\text{O} gives other bordism theories

: \begin{align}

M\text{String} &= M\text{O}\langle 8 \rangle \\

M\text{Spin} &= M\text{O}\langle 4 \rangle \\

M\text{SO} &= M\text{O}\langle 2 \rangle

\end{align}

such as string bordism.

Whitehead tower and string theory

In Spin geometry the \operatorname{Spin}(n) group is constructed as the universal cover of the Special orthogonal group \operatorname{SO}(n), so \Z/2 \to \operatorname{Spin}(n) \to SO(n) is a fibration, giving the first term in the Whitehead tower. There are physically relevant interpretations for the higher parts in this tower, which can be read as

\cdots \to \operatorname{Fivebrane}(n) \to \operatorname{String}(n) \to \operatorname{Spin}(n) \to \operatorname{SO}(n)
where \operatorname{String}(n) is the 3-connected cover of \operatorname{SO}(n) called the string group, and \operatorname{Fivebrane}(n) is the 7-connected cover called the fivebrane group.{{Cite web|url=https://physics.stackexchange.com/questions/359741/physical-application-of-postnikov-tower-stringn-and-fivebranen|title=Mathematical physics – Physical application of Postnikov tower, String(n) and Fivebrane(n)|website=Physics Stack Exchange|access-date=2020-02-16}}{{Cite web|url=https://mathoverflow.net/questions/59772/what-do-whitehead-towers-have-to-do-with-physics|title=at.algebraic topology – What do Whitehead towers have to do with physics?|website=MathOverflow|access-date=2020-02-16}}

See also

References

{{reflist}}

  • {{cite journal | last=Postnikov | first=Mikhail M. | author-link=Mikhail Postnikov | title=Determination of the homology groups of a space by means of the homotopy invariants | journal=Doklady Akademii Nauk SSSR | volume=76 | year=1951 | pages=359–362}}
  • {{cite web|last=Maxim|first=Laurențiu|url=https://web.archive.org/web/20200216062602/https://www.math.wisc.edu/~maxim/754notes.pdf| title=Lecture Notes on Homotopy Theory and Applications|website=www.math.wisc.edu}}
  • [https://www.pnas.org/content/32/11/277 Determination of the Second Homology and Cohomology Groups of a Space by Means of Homotopy Invariants] - gives accessible examples of Postnikov invariants
  • {{Cite book | last=Hatcher | first=Allen | author-link=Allen Hatcher|title=Algebraic topology | url=http://pi.math.cornell.edu/~hatcher/AT/ATpage.html | publisher=Cambridge University Press | isbn=978-0-521-79540-1 | year=2002}}
  • {{cite web|author=Zhang|title=Postnikov towers, Whitehead towers and their applications (handwritten notes)|url=https://www.math.purdue.edu/~zhang24/towers.pdf |archive-url=https://web.archive.org/web/20200213180540/https://www.math.purdue.edu/~zhang24/towers.pdf |website=www.math.purdue.edu|url-status=dead |archive-date=2020-02-13 }}

Category:Homotopy theory