# Mapping cylinder

{{ safesubst:#invoke:Unsubst||$N=Refimprove |date=__DATE__ |$B= {{#invoke:Message box|ambox}} }} In mathematics, specifically algebraic topology, the mapping cylinder of a function ${\displaystyle f}$ between topological spaces ${\displaystyle X}$ and ${\displaystyle Y}$ is the quotient

${\displaystyle M_{f}=(([0,1]\times X)\amalg Y)\,/\,\sim }$

where the union is disjoint, and ∼ is the equivalence relation generated by

${\displaystyle (0,x)\sim f(x)\quad {\text{for each }}x\in X.}$

That is, the mapping cylinder ${\displaystyle M_{f}}$ is obtained by gluing one end of ${\displaystyle X\times [0,1]}$ to ${\displaystyle Y}$ via the map ${\displaystyle f}$. Notice that the "top" of the cylinder ${\displaystyle \{1\}\times X}$ is homeomorphic to ${\displaystyle X}$, while the "bottom" is the space ${\displaystyle f(X)\subset Y}$.

See [1] for more details.

## Basic properties

The bottom Y is a deformation retract of ${\displaystyle M_{f}}$. The projection ${\displaystyle M_{f}\to Y}$ splits (via ${\displaystyle Y\ni y\mapsto y\in Y\subset M_{f}}$), and a deformation retraction ${\displaystyle R}$ is given by:

${\displaystyle R:M_{f}\times I\rightarrow M_{f}}$
${\displaystyle ([t,x],s)\mapsto [s\cdot t,x]}$

(where points in ${\displaystyle Y}$ stay fixed, which is well-defined, because ${\displaystyle [0,x]=[s\cdot 0,x]}$ for all ${\displaystyle s}$).

The map ${\displaystyle f:X\to Y}$ is a homotopy equivalence if and only if the "top" ${\displaystyle \{1\}\times X}$ is a strong deformation retract of ${\displaystyle M_{f}}$. A proof can be found in.[2] An explicit formula for the strong deformation retraction is produced in.[3]

## Interpretation

The mapping cylinder may be viewed as a way to replace an arbitrary map by an equivalent cofibration, in the following sense:

Given a map ${\displaystyle f\colon X\to Y}$, the mapping cylinder is a space ${\displaystyle M_{f}}$, together with a cofibration ${\displaystyle {\tilde {f}}\colon X\to M_{f}}$ and a surjective homotopy equivalence ${\displaystyle M_{f}\to Y}$ (indeed, Y is a deformation retract of ${\displaystyle M_{f}}$), such that the composition ${\displaystyle X\to M_{f}\to Y}$ equals f.

Thus the space Y gets replaced with a homotopy equivalent space ${\displaystyle M_{f}}$, and the map f with a lifted map ${\displaystyle {\tilde {f}}}$. Equivalently, the diagram

${\displaystyle f\colon X\to Y}$

gets replaced with a diagram

${\displaystyle {\tilde {f}}\colon X\to M_{f}}$

together with a homotopy equivalence between them.

The construction serves to replace any map of topological spaces by a homotopy equivalent cofibration.

Note that pointwise, a cofibration is a closed inclusion.

## Applications

Mapping cylinders are quite common homotopical tools. One use of mapping cylinders is to apply theorems concerning inclusions of spaces to general maps, which might not be injective.

Consequently, theorems or techniques (such as homology, cohomology or homotopy theory) which are only dependent on the homotopy class of spaces and maps involved may be applied to ${\displaystyle f\colon X\rightarrow Y}$ with the assumption that ${\displaystyle X\subset Y}$ and that ${\displaystyle f}$ is actually the inclusion of a subspace.

Another, more intuitive appeal of the construction is that it accords with the usual mental image of a function as "sending" points of ${\displaystyle X}$ to points of ${\displaystyle Y,}$ and hence of embedding ${\displaystyle X}$ within ${\displaystyle Y,}$ despite the fact that the function need not be one-to-one.

### Categorical application and interpretation

One can use the mapping cylinder to construct homotopy limits{{ safesubst:#invoke:Unsubst||date=__DATE__ |\$B= {{#invoke:Category handler|main}}{{#invoke:Category handler|main}}[citation needed] }}: given a diagram, replace the maps by cofibrations (using the mapping cylinder) and then take the ordinary pointwise limit (one must take a bit more care, but mapping cylinders are a component).

Conversely, the mapping cylinder is the homotopy pushout of the diagram where ${\displaystyle f\colon X\to Y}$ and ${\displaystyle {\text{id}}_{X}\colon X\to X}$.

### Mapping telescope

Given a sequence of maps

${\displaystyle X_{1}\to _{f_{1}}X_{2}\to _{f_{2}}X_{3}\to \cdots }$

the mapping telescope is the homotopical direct limit. If the maps are all already cofibrations (such as for the orthogonal groups ${\displaystyle O(n)\subset O(n+1)}$), then the direct limit is the union, but in general one must use the mapping telescope. The mapping telescope is a sequence of mapping cylinders, joined end-to-end. The picture of the construction looks like a stack of increasingly large cylinders, like a telescope.

Formally, one defines it as

${\displaystyle {\Bigl (}\coprod _{i}[0,1]\times X_{i}{\Bigr )}/((0,x_{i})\sim (1,f(x_{i})))}$

## References

1. Algebraic Topology by Allen Hatcher. Page 2
2. Algebraic Topology by Allen Hatcher. Corollary 0.16
3. A Short Note on Mapping Cylinders by A. Aguado
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