Exact sequence

An exact sequence is a concept in mathematics, especially in group theory, ring and module theory, homological algebra, as well as in differential geometry. An exact sequence is a sequence, either finite or infinite, of objects and morphisms between them such that the image of one morphism equals the kernel of the next.

Definition

In the context of group theory, a sequence

${\displaystyle G_{0}\;{\xrightarrow {\ f_{1}\ }}\;G_{1}\;{\xrightarrow {\ f_{2}\ }}\;G_{2}\;{\xrightarrow {\ f_{3}\ }}\;\cdots \;{\xrightarrow {\ f_{n}\ }}\;G_{n}}$

of groups and group homomorphisms is called exact if the image of each homomorphism is equal to the kernel of the next:

${\displaystyle \operatorname {im} (f_{k})=\ker(f_{k+1})}$

The sequence of groups and homomorphisms may be either finite or infinite.

A similar definition can be made for other algebraic structures. For example, one could have an exact sequence of vector spaces and linear maps, or of modules and module homomorphisms. More generally, the notion of an exact sequence makes sense in any category with kernels and cokernels.

Simple cases

To understand the definition, it is helpful to consider relatively simple cases where the sequence is finite and begins or ends with the trivial group. Traditionally, this, along with the single identity element, is denoted 0 (additive notation, usually when the groups are abelian), or denoted 1 (multiplicative notation).

• Consider the sequence 0 → A → B. The image of the leftmost map is 0. Therefore the sequence is exact if and only if the rightmost map (from A to B) has kernel {0}; i.e., if and only if that map is a monomorphism (injective, or one-to-one).
• Consider the dual sequence B → C → 0. The kernel of the rightmost map is C. Therefore the sequence is exact if and only if the image of the leftmost map (from B to C) is all of C; i.e., if and only if that map is an epimorphism (surjective, or onto).
• Therefore, the sequence 0 → X → Y → 0 is exact if and only if the map from X to Y is both a monomorphism and epimorphism (that is, a bimorphism), and thus, in many cases, an isomorphism from X to Y.

Short exact sequence

Important are short exact sequences, which are exact sequences of the form

${\displaystyle 0\to A\;{\xrightarrow {\ f\ }}\;B\;{\xrightarrow {\ g\ }}\;C\to 0}$

As established above, for any such short exact sequence, f is a monomorphism and g is an epimorphism. Furthermore, the image of f is equal to the kernel of g. It is helpful to think of A as a subobject of B with f embedding A into B, and of C as the corresponding factor object (or quotient), B/A, with g inducing an isomorphism

${\displaystyle C\cong B/\operatorname {im} (f)}$

The short exact sequence

${\displaystyle 0\to A\;{\xrightarrow {\ f\ }}\;B\;{\xrightarrow {\ g\ }}\;C\to 0}$

is called split if there exists a homomorphism h : C → B such that the composition g ∘ h is the identity map on C. It follows that if these are abelian groups, B is isomorphic to the direct sum of A and C (see Splitting lemma):

${\displaystyle B\cong A\oplus C.}$

Long exact sequence

A long exact sequence is an exact sequence consisting of more than three nonzero terms, often an infinite exact sequence.

A long exact sequence

${\displaystyle A_{0}\;{\xrightarrow {\ f_{1}\ }}\;A_{1}\;{\xrightarrow {\ f_{2}\ }}\;A_{2}\;{\xrightarrow {\ f_{3}\ }}\;\cdots \;{\xrightarrow {\ f_{n}\ }}\;A_{n}}$

is equivalent to a sequence of short exact sequences

${\displaystyle {\begin{aligned}&A_{0}\;\rightarrow \;K_{1}\;\rightarrow \;0\;,\\0\;\rightarrow \;K_{1}\rightarrow {}&A_{1}\;\rightarrow \;K_{2}\;\rightarrow \;0\;,\\\vdots \,\,\,\,\\0\;\rightarrow \;K_{n-1}\rightarrow {}&A_{n-1}\rightarrow \;K_{n}\;\rightarrow \;0\;,\\0\;\rightarrow K_{n}\rightarrow {}&A_{n}\end{aligned}}}$

where ${\displaystyle K_{i}=\operatorname {im} (f_{i})=\ker(f_{i+1})}$ for every ${\displaystyle i}$.

Examples

Integers modulo two

Consider the following sequence of abelian groups:

${\displaystyle \mathbf {Z} \;\;{\overset {2\times }{\hookrightarrow }}\;\;\mathbf {Z} \twoheadrightarrow \mathbf {Z} /2\mathbf {Z} }$

The first homomorphism maps each element i in the set of integers Z to the element 2i in Z. The second homomorphism maps each element i in Z to an element j in the quotient group, i.e., j = i mod 2. Here the hook arrow ${\displaystyle \hookrightarrow }$ indicates that the map 2× from Z to Z is a monomorphism, and the two-headed arrow ${\displaystyle \twoheadrightarrow }$ indicates an epimorphism (the map mod 2). This is an exact sequence because the image 2Z of the monomorphism is the kernel of the epimorphism. Essentially "the same" sequence can also be written as

${\displaystyle 2\mathbf {Z} \;\;{\hookrightarrow }\;\;\mathbf {Z} \twoheadrightarrow \mathbf {Z} /2\mathbf {Z} }$

In this case the monomorphism is 2n ↦ 2n and although it looks like an identity function, it is not onto (i.e. not an epimorphism) because the odd numbers don't belong to 2Z. The image of 2Z through this monomorphism is however exactly the same subset of Z as the image of Z through n ↦ 2n used in the previous sequence. This latter sequence does differ in the concrete nature of its first object from the previous one as 2Z is not the same set as Z even though the two are isomorphic as groups.

The first sequence may also be written without using special symbols for monomorphism and epimorphism:

${\displaystyle 0\;\to \;\mathbf {Z} \;\;{\overset {2\times }{\longrightarrow }}\;\;\mathbf {Z} \;\longrightarrow \;\mathbf {Z} /2\mathbf {Z} \;\to \;\ 0}$

Here 0 denotes the trivial group, the map from Z to Z is multiplication by 2, and the map from Z to the factor group Z/2Z is given by reducing integers modulo 2. This is indeed an exact sequence:

• the image of the map 0 → Z is {0}, and the kernel of multiplication by 2 is also {0}, so the sequence is exact at the first Z.
• the image of multiplication by 2 is 2Z, and the kernel of reducing modulo 2 is also 2Z, so the sequence is exact at the second Z.
• the image of reducing modulo 2 is Z/2Z, and the kernel of the zero map is also Z/2Z, so the sequence is exact at the position Z/2Z.

The first and third sequences are somewhat of a special case owing to the infinite nature of Z. It is not possible for a finite group to be mapped by inclusion (i.e. by a monomorphism) as a proper subgroup of itself. Instead the sequence that emerges from the first isomorphism theorem is

${\displaystyle 1\to N\to G\to G/N\to 1}$

As a more concrete example of an exact sequence on finite groups:

${\displaystyle 1\to C_{n}\to D_{2n}\to C_{2}\to 1}$

where ${\displaystyle C_{n}}$ is the cyclic group of order n and ${\displaystyle D_{2n}}$ is the dihedral group of order 2n, which is a non-abelian group.

Intersection and sum of modules

Let I and J be two ideals of a ring R. Then

${\displaystyle 0\to I\cap J\to I\oplus J\to I+J\to 0}$

is an exact sequence of R-modules, where the module homomorphism ${\displaystyle I\cap J\to I\oplus J}$ maps each element x of ${\displaystyle I\cap J}$ to the element ${\displaystyle (x,x)}$ of the direct sum ${\displaystyle I\oplus J}$, and the homomorphsim ${\displaystyle I\oplus J\to I+J}$ maps each element ${\displaystyle (x,y)}$ of ${\displaystyle I\oplus J}$ to ${\displaystyle x-y}$.

These homomorphisms are restrictions of similarly defined homomorphisms that form the short exact sequence

${\displaystyle 0\to R\to R\oplus R\to R\to 0}$

Passing to quotient modules yield another exact sequence

${\displaystyle 0\to R/(I\cap J)\to R/I\oplus R/J\to R/(I+J)\to 0}$

Grad, curl and div in differential geometry

Another example can be derived from differential geometry, especially relevant for work on the Maxwell equations.

Consider the Hilbert space ${\displaystyle L^{2}}$ of scalar-valued square-integrable functions on three dimensions ${\displaystyle \left\lbrace f:\mathbb {R} ^{3}\to \mathbb {R} \right\rbrace }$. Taking the gradient of a function ${\displaystyle f\in \mathbb {H} _{1}}$ moves us to a subset of ${\displaystyle \mathbb {H} _{3}}$, the space of vector valued, still square-integrable functions on the same domain ${\displaystyle \left\lbrace f:\mathbb {R} ^{3}\to \mathbb {R} ^{3}\right\rbrace }$ -- specifically, the set of such functions that represent conservative vector fields. (The generalized Stokes' theorem has preserved integrability.)

First, note the curl of all such fields is zero -- since

${\displaystyle {\begin{aligned}\operatorname {curl} (\operatorname {grad} f)&\equiv \nabla \times (\nabla f)=0\end{aligned}}}$

for all such f. However, this only proves that the image of the gradient is a subset of the kernel of the curl. To prove that they are in fact the same set, prove the converse: that if the curl of a vector field ${\displaystyle {\vec {F}}}$ is 0, then ${\displaystyle {\vec {F}}}$ is the gradient of some scalar function. This follows almost immediately from Stokes' theorem (see the proof at conservative force.) The image of the gradient is then precisely the kernel of the curl, and so we can then take the curl to be our next morphism, taking us again to a (different) subset of ${\displaystyle \mathbb {H} _{3}}$.

Similarly, we note that

${\displaystyle {\begin{aligned}\operatorname {div} (\operatorname {curl} {\vec {v}})&\equiv \nabla \cdot \nabla \times {\vec {v}}=0,\end{aligned}}}$

so the image of the curl is a subset of the kernel of the divergence. The converse is somewhat involved:

Proof that ${\displaystyle \operatorname {div} {\vec {F}}}$ = 0 implies ${\displaystyle {\vec {F}}=\operatorname {curl} {\vec {A}}}$ for some ${\displaystyle {\vec {A}}}$

We shall proceed by construction: given a vector field ${\displaystyle {\vec {F}}=F_{x}{\hat {i}}+F_{y}{\hat {j}}+F_{z}{\hat {k}}}$ such that ${\displaystyle \nabla \cdot {\vec {F}}=0}$, we produce a field ${\displaystyle {\vec {A}}}$ such that ${\displaystyle {\begin{aligned}\nabla \times {\vec {A}}&=\left(\partial _{y}A_{z}-\partial _{z}A_{y}\right){\hat {i}}+\left(\partial _{z}A_{x}-\partial _{x}A_{z}\right){\hat {j}}+\left(\partial _{x}A_{y}-\partial _{y}A_{x}\right){\hat {k}}\\&=F_{x}{\hat {i}}+F_{y}{\hat {j}}+F_{z}{\hat {k}}={\vec {F}}\end{aligned}}}$ First, note that since as proved above ${\displaystyle \operatorname {curl} (\operatorname {grad} f)=0}$, we can add the gradient of any scalar function to ${\displaystyle {\vec {A}}}$ without changing the curl. We can use this gauge freedom to set any one component of ${\displaystyle {\vec {A}}}$ to zero without changing its curl; choosing arbitrarily the z-component, we thus require simply that ${\displaystyle -\partial _{z}A_{y}{\hat {i}}+\partial _{z}A_{x}{\hat {j}}+\left(\partial _{x}A_{y}-\partial _{y}A_{x}\right){\hat {k}}=F_{x}{\hat {i}}+F_{y}{\hat {j}}+F_{z}{\hat {k}}}$ Then by simply integrating the first two components, and noting that the 'constant' of integration may still depend on any variable not integrated over, we find that ${\displaystyle {\begin{aligned}A_{x}&=\int F_{y}dz+{\vec {C_{1}}}(x,y)\\A_{y}&=-\int F_{x}dz+{\vec {C_{2}}}(x,y)\end{aligned}}}$ Note that since the two integration terms ${\displaystyle {\vec {C_{1}}},{\vec {C_{2}}}}$ both depend only on x and y and not on z, then we can add another gradient of some function ${\displaystyle f(x,y)}$ that also does not depend on z. This permits us to eliminate either of the terms in favor of the other, without spoiling our earlier work that set ${\displaystyle A_{z}}$ to zero. Choosing to eliminate ${\displaystyle {\vec {C_{2}}}}$ and applying the last component as a constraint, we have ${\displaystyle {\begin{aligned}-\partial _{x}\int F_{x}dz+\partial _{x}{\vec {C_{1}}}(x,y)-\partial _{y}\int F_{y}dz&=F_{z}\\-\int \left(\partial _{x}F_{x}+\partial _{y}F_{y}\right)dz+\partial _{x}{\vec {C_{1}}}(x,y)&=F_{z}\end{aligned}}}$ By assumption, ${\displaystyle \operatorname {div} {\vec {F}}=\partial _{x}F_{x}+\partial _{y}F_{y}+\partial _{z}F_{z}=0}$, and so ${\displaystyle \int \partial _{z}F_{z}dz+\partial _{x}{\vec {C_{1}}}(x,y)=F_{z}}$ Since the fundamental theorem of calculus requires that the first term above be precisely ${\displaystyle F_{z}}$ plus a constant in z, a solution to the above system of equations is guaranteed to exist.

Having thus proved that the image of the curl is precisely the kernel of the divergence, this morphism in turn takes us back to the space we started from ${\displaystyle L^{2}}$. Since definitionally we have landed on a space of integrable functions, any such function can (at least formally) be integrated in order to produce a vector field which divergence is that function -- so the image of the divergence is the entirety of ${\displaystyle L^{2}}$, and we can complete our sequence:

${\displaystyle 0\to L^{2}\;\;{\xrightarrow {\operatorname {grad} }}\;\;\mathbb {H} _{3}\;\;{\xrightarrow {\operatorname {curl} }}\;\;\mathbb {H} _{3}\;\;{\xrightarrow {\operatorname {div} }}\;\;L^{2}\to 0}$

Equivalently, we could have reasoned in reverse: in a simply connected space, a curl-free vector field (a field in the kernel of the curl) can always be written as a gradient of a scalar function (and thus is in the image of the gradient). Similarly, a divergenceless field can be written as a curl of another field.[1] (Reasoning in this direction thus makes use of the fact that 3-dimensional space is topologically trivial.)

This short exact sequence also permits a much shorter proof of the validity of the Helmholtz decomposition that does not rely on brute-force vector calculus. Consider the subsequence

${\displaystyle 0\to L^{2}\;\;{\xrightarrow {\operatorname {grad} }}\;\;\mathbb {H} _{3}\;\;{\xrightarrow {\operatorname {curl} }}\;\;\operatorname {im} (\operatorname {curl} )\to 0.}$

Since the divergence of the gradient is the Laplacian, and since the Hilbert space of square-integrable functions can be spanned by the eigenfunctions of the Laplacian, we already see that some inverse mapping ${\displaystyle \nabla ^{-1}:\mathbb {H} _{3}\to L^{2}}$ must exist. To explicitly construct such an inverse, we can start from the definition of the vector Laplacian

${\displaystyle \nabla ^{2}{\vec {A}}=\nabla (\nabla \cdot {\vec {A}})+\nabla \times (\nabla \times {\vec {A}})}$

Since we are trying to construct an identity mapping by composing some function with the gradient, we know that in our case ${\displaystyle \nabla \times {\vec {A}}=\operatorname {curl} ({\vec {A}})=0}$. Then if we take the divergence of both sides

${\displaystyle {\begin{aligned}\nabla \cdot \nabla ^{2}{\vec {A}}&=\nabla \cdot \nabla (\nabla \cdot {\vec {A}})\\&=\nabla ^{2}(\nabla \cdot {\vec {A}})\\\end{aligned}}}$

we see that if a function is an eigenfunction of the vector Laplacian, its divergence must be an eigenfunction of the scalar Laplacian with the same eigenvalue. Then we can build our inverse function ${\displaystyle \nabla ^{-1}}$ simply by breaking any function in ${\displaystyle \mathbb {H} _{3}}$ into the vector-Laplacian eigenbasis, scaling each by the inverse of their eigenvalue, and taking the divergence; the action of ${\displaystyle \nabla ^{-1}\circ \nabla }$ is thus clearly the identity. Thus by the splitting lemma,

${\displaystyle \mathbb {H} _{3}\cong L^{2}\oplus \operatorname {im} (\operatorname {curl} )}$,

or equivalently, any square-integrable vector field on ${\displaystyle \mathbb {R} ^{3}}$ can be broken into the sum of a gradient and a curl -- which is what we set out to prove.

Properties

The splitting lemma states that if the short exact sequence

${\displaystyle 0\to A\;{\xrightarrow {\ f\ }}\;B\;{\xrightarrow {\ g\ }}\;C\to 0}$

admits a morphism t : B → A such that t ∘ f is the identity on A or a morphism u: C → B such that g ∘ u is the identity on C, then B is a direct sum of A and C (for non-commutative groups, this is a semidirect product). One says that such a short exact sequence splits.

The snake lemma shows how a commutative diagram with two exact rows gives rise to a longer exact sequence. The nine lemma is a special case.

The five lemma gives conditions under which the middle map in a commutative diagram with exact rows of length 5 is an isomorphism; the short five lemma is a special case thereof applying to short exact sequences.

The importance of short exact sequences is underlined by the fact that every exact sequence results from "weaving together" several overlapping short exact sequences. Consider for instance the exact sequence

${\displaystyle A_{1}\to A_{2}\to A_{3}\to A_{4}\to A_{5}\to A_{6}}$

which implies that there exist objects C_k in the category such that

${\displaystyle C_{k}\cong \ker(A_{k}\to A_{k+1})\cong \operatorname {im} (A_{k-1}\to A_{k})}$.

Suppose in addition that the cokernel of each morphism exists, and is isomorphic to the image of the next morphism in the sequence:

${\displaystyle C_{k}\cong \operatorname {coker} (A_{k-2}\to A_{k-1})}$

(This is true for a number of interesting categories, including any abelian category such as the abelian groups; but it is not true for all categories that allow exact sequences, and in particular is not true for the category of groups, in which coker(f) : G → H is not H/im(f) but ${\displaystyle H/{\left\langle \operatorname {im} f\right\rangle }^{H}}$, the quotient of H by the conjugate closure of im(f).) Then we obtain a commutative diagram in which all the diagonals are short exact sequences:

The only portion of this diagram that depends on the cokernel condition is the object ${\textstyle C_{7}}$ and the final pair of morphisms ${\textstyle A_{6}\to C_{7}\to 0}$. If there exists any object ${\displaystyle A_{k+1}}$ and morphism ${\displaystyle A_{k}\to A_{k+1}}$ such that ${\displaystyle A_{k-1}\to A_{k}\to A_{k+1}}$ is exact, then the exactness of ${\displaystyle 0\to C_{k}\to A_{k}\to C_{k+1}\to 0}$ is ensured. Again taking the example of the category of groups, the fact that im(f) is the kernel of some homomorphism on H implies that it is a normal subgroup, which coincides with its conjugate closure; thus coker(f) is isomorphic to the image H/im(f) of the next morphism.

Conversely, given any list of overlapping short exact sequences, their middle terms form an exact sequence in the same manner.

Applications of exact sequences

In the theory of abelian categories, short exact sequences are often used as a convenient language to talk about sub- and factor objects.

The extension problem is essentially the question "Given the end terms A and C of a short exact sequence, what possibilities exist for the middle term B?" In the category of groups, this is equivalent to the question, what groups B have A as a normal subgroup and C as the corresponding factor group? This problem is important in the classification of groups. See also Outer automorphism group.

Notice that in an exact sequence, the composition f_i+1 ∘ f_i maps A_i to 0 in A_i+2, so every exact sequence is a chain complex. Furthermore, only f_i-images of elements of A_i are mapped to 0 by f_i+1, so the homology of this chain complex is trivial. More succinctly:

Exact sequences are precisely those chain complexes which are acyclic.

Given any chain complex, its homology can therefore be thought of as a measure of the degree to which it fails to be exact.

If we take a series of short exact sequences linked by chain complexes (that is, a short exact sequence of chain complexes, or from another point of view, a chain complex of short exact sequences), then we can derive from this a long exact sequence (i.e. an exact sequence indexed by the natural numbers) on homology by application of the zig-zag lemma. It comes up in algebraic topology in the study of relative homology; the Mayer–Vietoris sequence is another example. Long exact sequences induced by short exact sequences are also characteristic of derived functors.

Exact functors are functors that transform exact sequences into exact sequences.

References

General

• Spanier, Edwin Henry (1995). Algebraic Topology. Berlin: Springer. p. 179. ISBN 0-387-94426-5.
• Eisenbud, David (1995). Commutative Algebra: with a View Toward Algebraic Geometry. Springer-Verlag New York. p. 785. ISBN 0-387-94269-6.

Citations

1. "Divergenceless field". December 6, 2009.

External links

• "Exact sequence". PlanetMath.