An exact sequence is a sequence of morphisms between objects (for example, groups, rings, modules, and, more generally, objects of an abelian category) such that the image of one morphism equals the kernel of the next.
In the context of group theory, a sequence
G0 \xrightarrow{ f1 } G1 \xrightarrow{ f2 } G2 \xrightarrow{ f3 } … \xrightarrow{ fn } Gn
Gi
\operatorname{im}(fi)=\ker(fi+1)
Gi
1\leqi<n
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, and more specially in abelian categories, where it is widely used.
To understand the definition, it is helpful to consider relatively simple cases where the sequence is of group homomorphisms, 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).
Short exact sequences are exact sequences of the form
0\toA\xrightarrow{f}B\xrightarrow{g}C\to0.
C\congB/\operatorname{im}(f)=B/\operatorname{ker}(g)
The short exact sequence
0\toA\xrightarrow{f}B\xrightarrow{g}C\to0
B\congA ⊕ C.
A general exact sequence is sometimes called a long exact sequence, to distinguish from the special case of a short exact sequence.[1]
A long exact sequence is equivalent to a family of short exact sequences in the following sense: Given a long sequence
with n ≥ 2, we can split it up into the short sequences
where
Ki=\operatorname{im}(fi)
i
Ki
Consider the following sequence of abelian groups:
Zl{\overset{2 x }{\hookrightarrow}}Z\twoheadrightarrowZ/2Z
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; that is, . Here the hook arrow
\hookrightarrow
\twoheadrightarrow
2Zl{\hookrightarrow}Z\twoheadrightarrowZ/2Z
In this case the monomorphism is 2n ↦ 2n and although it looks like an identity function, it is not onto (that is, 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:
0\toZl{\overset{2 x }{\longrightarrow}}Z\longrightarrowZ/2Z\to0
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 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 (that is, by a monomorphism) as a proper subgroup of itself. Instead the sequence that emerges from the first isomorphism theorem is
1\toN\toG\toG/N\to1
1,
As a more concrete example of an exact sequence on finite groups:
1\toCn\toD2n\toC2\to1
where
Cn
D2n
Let and be two ideals of a ring .Then
0\toI\capJ\toI ⊕ J\toI+J\to0
I\capJ\toI ⊕ J
I\capJ
I ⊕ J
I ⊕ J\toI+J
I ⊕ J
These homomorphisms are restrictions of similarly defined homomorphisms that form the short exact sequence
0\toR\toR ⊕ R\toR\to0
Passing to quotient modules yields another exact sequence
0\toR/(I\capJ)\toR/I ⊕ R/J\toR/(I+J)\to0
Another example can be derived from differential geometry, especially relevant for work on the Maxwell equations.
L2
\left\lbracef:R3\toR\right\rbrace
f\inH1
H3
\left\lbracef:R3\toR3\right\rbrace
First, note the curl of all such fields is zero — since
\operatorname{curl}(\operatorname{grad}f)\equiv\nabla x (\nablaf)=0
for all such . 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
\vec{F}
\vec{F}
H3
Similarly, we note that
\operatorname{div}\left(\operatorname{curl}\vec{v}\right)\equiv\nabla ⋅ \nabla x \vec{v}=0,
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
L2
L2
0\toL2l{\xrightarrow{\operatorname{grad}}}H3l{\xrightarrow{\operatorname{curl}}}H3l{\xrightarrow{\operatorname{div}}}L2\to0
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 solenoidal vector field can be written as a curl of another field.[2] (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
0\toL2l{\xrightarrow{\operatorname{grad}}}H3l{\xrightarrow{\operatorname{curl}}}\operatorname{im}(\operatorname{curl})\to0.
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
\nabla-1:H3\toL2
\nabla2\vec{A}=\nabla\left(\nabla ⋅ \vec{A}\right)+\nabla x \left(\nabla x \vec{A}\right)
Since we are trying to construct an identity mapping by composing some function with the gradient, we know that in our case
\nabla x \vec{A}=\operatorname{curl}\left(\vec{A}\right)=0
\begin{align} \nabla ⋅ \nabla2\vec{A} &=\nabla ⋅ \nabla\left(\nabla ⋅ \vec{A}\right)\\ &=\nabla2\left(\nabla ⋅ \vec{A}\right)\\ \end{align}
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
\nabla-1
H3
\nabla-1\circ\nabla
H3\congL2 ⊕ \operatorname{im}(\operatorname{curl})
or equivalently, any square-integrable vector field on
R3
The splitting lemma states that, for a short exact sequence
0\toA \xrightarrow{ f } B \xrightarrow{ g } C\to0,
For non-commutative groups, the splitting lemma does not apply, and one has only the equivalence between the two last conditions, with "the direct sum" replaced with "a semidirect product".
In both cases, 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
A1\toA2\toA3\toA4\toA5\toA6
which implies that there exist objects Ck in the category such that
Ck\cong\ker(Ak\toAk+1)\cong\operatorname{im}(Ak-1\toAk)
Suppose in addition that the cokernel of each morphism exists, and is isomorphic to the image of the next morphism in the sequence:
Ck\cong\operatorname{coker}(Ak-2\toAk-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
H/{\left\langle\operatorname{im}f\right\rangle}H
The only portion of this diagram that depends on the cokernel condition is the object and the final pair of morphisms . If there exists any object
Ak+1
Ak\toAk+1
Ak-1\toAk\toAk+1
0\toCk\toAk\toCk+1\to0
Conversely, given any list of overlapping short exact sequences, their middle terms form an exact sequence in the same manner.
In the theory of abelian categories, short exact sequences are often used as a convenient language to talk about subobjects 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 fi+1 ∘ fi maps Ai to 0 in Ai+2, so every exact sequence is a chain complex. Furthermore, only fi-images of elements of Ai are mapped to 0 by fi+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 (that is, 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.