- Source: Serre spectral sequence
In mathematics, the Serre spectral sequence (sometimes Leray–Serre spectral sequence to acknowledge earlier work of Jean Leray in the Leray spectral sequence) is an important tool in algebraic topology. It expresses, in the language of homological algebra, the singular (co)homology of the total space X of a (Serre) fibration in terms of the (co)homology of the base space B and the fiber F. The result is due to Jean-Pierre Serre in his doctoral dissertation.
Cohomology spectral sequence
Let
f
:
X
→
B
{\displaystyle f\colon X\to B}
be a Serre fibration of topological spaces, and let F be the (path-connected) fiber. The Serre cohomology spectral sequence is the following:
E
2
p
,
q
=
H
p
(
B
,
H
q
(
F
)
)
⇒
H
p
+
q
(
X
)
.
{\displaystyle E_{2}^{p,q}=H^{p}(B,H^{q}(F))\Rightarrow H^{p+q}(X).}
Here, at least under standard simplifying conditions, the coefficient group in the
E
2
{\displaystyle E_{2}}
-term is the q-th integral cohomology group of F, and the outer group is the singular cohomology of B with coefficients in that group. The differential on the kth page is
d
k
:
E
k
p
,
q
→
E
k
p
+
k
,
q
+
1
−
k
{\displaystyle d_{k}:E_{k}^{p,q}\to E_{k}^{p+k,q+1-k}}
.
Strictly speaking, what is meant is cohomology with respect to the local coefficient system on B given by the cohomology of the various fibers. Assuming for example, that B is simply connected, this collapses to the usual cohomology. For a path connected base, all the different fibers are homotopy equivalent. In particular, their cohomology is isomorphic, so the choice of "the" fiber does not give any ambiguity.
The abutment means integral cohomology of the total space X.
This spectral sequence can be derived from an exact couple built out of the long exact sequences of the cohomology of the pair
(
X
p
,
X
p
−
1
)
{\displaystyle (X_{p},X_{p-1})}
, where
X
p
{\displaystyle X_{p}}
is the restriction of the fibration over the p-skeleton of B. More precisely, using this notation,
A
=
⨁
p
,
q
H
q
(
X
p
)
,
{\displaystyle A=\bigoplus _{p,q}H^{q}(X_{p}),}
E
1
p
,
q
=
C
=
⨁
p
,
q
H
q
(
X
p
,
X
p
−
1
)
,
{\displaystyle E_{1}^{p,q}=C=\bigoplus _{p,q}H^{q}(X_{p},X_{p-1}),}
f is defined by restricting each piece on
X
p
{\displaystyle X_{p}}
to
X
p
−
1
{\displaystyle X_{p-1}}
, g is defined using the coboundary map in the long exact sequence of the pair, and h is defined by restricting
(
X
p
,
X
p
−
1
)
{\displaystyle (X_{p},X_{p-1})}
to
X
p
.
{\displaystyle X_{p}.}
There is a multiplicative structure
E
r
p
,
q
×
E
r
s
,
t
→
E
r
p
+
s
,
q
+
t
,
{\displaystyle E_{r}^{p,q}\times E_{r}^{s,t}\to E_{r}^{p+s,q+t},}
coinciding on the E2-term with (−1)qs times the cup product, and with respect to which the differentials
d
r
{\displaystyle d_{r}}
are (graded) derivations inducing the product on the
E
r
+
1
{\displaystyle E_{r+1}}
-page from the one on the
E
r
{\displaystyle E_{r}}
-page.
Homology spectral sequence
Similarly to the cohomology spectral sequence, there is one for homology:
E
p
,
q
2
=
H
p
(
B
,
H
q
(
F
)
)
⇒
H
p
+
q
(
X
)
.
{\displaystyle E_{p,q}^{2}=H_{p}(B,H_{q}(F))\Rightarrow H_{p+q}(X).}
where the notations are dual to the ones above, in particular the differential on the kth page is a map
d
k
:
E
p
,
q
k
→
E
p
−
k
,
q
−
1
+
k
k
{\displaystyle d_{k}:E_{p,q}^{k}\to E_{p-k,q-1+k}^{k}}
.
Example computations
= Hopf fibration
=Recall that the Hopf fibration is given by
S
1
↪
S
3
→
S
2
{\displaystyle S^{1}\hookrightarrow S^{3}\to S^{2}}
. The
E
2
{\displaystyle E_{2}}
-page of the Leray–Serre Spectral sequence reads
1
H
0
(
S
2
;
Z
)
0
H
2
(
S
2
;
Z
)
0
H
0
(
S
2
;
Z
)
0
H
2
(
S
2
;
Z
)
0
1
2
{\displaystyle {\begin{array}{c|ccc}1&H^{0}(S^{2};\mathbb {Z} )&0&H^{2}(S^{2};\mathbb {Z} )\\0&H^{0}(S^{2};\mathbb {Z} )&0&H^{2}(S^{2};\mathbb {Z} )\\\hline &0&1&2\end{array}}}
The differential
d
2
+
i
{\displaystyle d_{2+i}}
goes
1
+
i
{\displaystyle 1+i}
down and
2
+
i
{\displaystyle 2+i}
right. Thus the only differential which is not necessarily 0 is d0,12, because the rest have domain or codomain 0 (since they are 0 on the E2-page). In particular, this sequence degenerates at E2 = E∞. The E3-page reads
1
ker
d
2
0
,
1
0
H
2
(
S
2
;
Z
)
0
H
0
(
S
2
;
Z
)
0
coker
d
2
0
,
1
0
1
2
{\displaystyle {\begin{array}{c|ccc}1&\ker d_{2}^{0,1}&0&H^{2}(S^{2};\mathbb {Z} )\\0&H^{0}(S^{2};\mathbb {Z} )&0&\operatorname {coker} d_{2}^{0,1}\\\hline &0&1&2\end{array}}}
The spectral sequence abuts to
H
p
+
q
(
S
3
)
,
{\displaystyle H^{p+q}(S^{3}),}
i.e.
E
3
p
,
q
=
G
r
p
H
p
+
q
(
S
3
)
.
{\displaystyle E_{3}^{p,q}=Gr^{p}H^{p+q}(S^{3}).}
Evaluating at the interesting parts, we have
ker
d
2
0
,
1
=
G
r
1
H
1
(
S
3
)
{\displaystyle \ker d_{2}^{0,1}=Gr^{1}H^{1}(S^{3})}
and
coker
d
2
0
,
1
=
G
r
0
H
2
(
S
3
)
.
{\displaystyle \operatorname {coker} d_{2}^{0,1}=Gr^{0}H^{2}(S^{3}).}
Knowing the cohomology of
S
3
,
{\displaystyle S^{3},}
both are zero, so the differential
d
2
0
,
1
{\displaystyle d_{2}^{0,1}}
is an isomorphism.
= Sphere bundle on a complex projective variety
=Given a complex n-dimensional projective variety X there is a canonical family of line bundles
O
X
(
k
)
{\displaystyle {\mathcal {O}}_{X}(k)}
for
k
∈
Z
{\displaystyle k\in \mathbb {Z} }
coming from the embedding
X
→
C
P
m
{\displaystyle X\to \mathbb {CP} ^{m}}
. This is given by the global sections
s
0
,
…
,
s
m
∈
Γ
(
X
,
O
X
(
1
)
)
{\displaystyle s_{0},\ldots ,s_{m}\in \Gamma (X,{\mathcal {O}}_{X}(1))}
which send
x
↦
[
s
0
(
x
)
:
…
:
s
m
(
x
)
]
{\displaystyle x\mapsto [s_{0}(x):\ldots :s_{m}(x)]}
If we construct a rank r vector bundle
E
{\displaystyle {\mathcal {E}}}
which is a finite whitney sum of vector bundles we can construct a sphere bundle
S
→
X
{\displaystyle S\to X}
whose fibers are the spheres
S
2
r
−
1
⊂
C
r
{\displaystyle S^{2r-1}\subset \mathbb {C} ^{r}}
. Then, we can use the Serre spectral sequence along with the Euler class to compute the integral cohomology of S. The
E
2
{\displaystyle E_{2}}
-page is given by
E
2
p
,
q
=
H
p
(
X
;
H
q
(
S
2
r
−
1
)
)
{\displaystyle E_{2}^{p,q}=H^{p}(X;H^{q}(S^{2r-1}))}
. We see that the only non-trivial differentials are given on the
E
2
r
{\displaystyle E_{2r}}
-page and are defined by cupping with the Euler class
e
(
E
)
{\displaystyle e({\mathcal {E}})}
. In this case it is given by the top chern class of
E
{\displaystyle {\mathcal {E}}}
. For example, consider the vector bundle
O
X
(
a
)
⊕
O
X
(
b
)
{\displaystyle {\mathcal {O}}_{X}(a)\oplus {\mathcal {O}}_{X}(b)}
for X a K3 surface. Then, the spectral sequence reads as
E
2
=
E
3
=
E
4
=
3
H
0
(
X
;
Z
)
H
1
(
X
;
Z
)
H
2
(
X
;
Z
)
H
3
(
X
;
Z
)
H
4
(
X
;
Z
)
2
0
0
0
0
0
1
0
0
0
0
0
0
H
0
(
X
;
Z
)
H
1
(
X
;
Z
)
H
2
(
X
;
Z
)
H
3
(
X
;
Z
)
H
4
(
X
;
Z
)
0
1
2
3
4
{\displaystyle E_{2}=E_{3}=E_{4}={\begin{array}{c|ccccc}3&H^{0}(X;\mathbb {Z} )&H^{1}(X;\mathbb {Z} )&H^{2}(X;\mathbb {Z} )&H^{3}(X;\mathbb {Z} )&H^{4}(X;\mathbb {Z} )\\2&0&0&0&0&0\\1&0&0&0&0&0\\0&H^{0}(X;\mathbb {Z} )&H^{1}(X;\mathbb {Z} )&H^{2}(X;\mathbb {Z} )&H^{3}(X;\mathbb {Z} )&H^{4}(X;\mathbb {Z} )\\\hline &0&1&2&3&4\end{array}}}
The differential
d
4
=
∪
a
⋅
b
H
2
{\displaystyle d_{4}=\cup a\cdot bH^{2}}
for
H
2
{\displaystyle H^{2}}
is the square of the Lefschetz class. In this case, the only non-trivial differential is then
d
4
0
,
3
:
H
0
(
X
;
Z
)
→
H
4
(
X
;
Z
)
{\displaystyle d_{4}^{0,3}:H^{0}(X;\mathbb {Z} )\to H^{4}(X;\mathbb {Z} )}
We can finish this computation by noting the only nontrivial cohomology groups are
H
k
(
X
;
Z
)
=
{
Z
k
∈
{
0
,
4
}
Z
⊕
22
k
=
2
{\displaystyle H^{k}(X;\mathbb {Z} )={\begin{cases}\mathbb {Z} &k\in \{0,4\}\\\mathbb {Z} ^{\oplus 22}&k=2\end{cases}}}
= Basic pathspace fibration
=We begin first with a basic example; consider the path space fibration
Ω
S
n
+
1
→
P
S
n
+
1
→
S
n
+
1
.
{\displaystyle \Omega S^{n+1}\to PS^{n+1}\to S^{n+1}.}
We know the homology of the base and total space, so our intuition tells us that the Serre spectral sequence should be able to tell us the homology of the loop space. This is an example of a case where we can study the homology of a fibration by using the E∞ page (the homology of the total space) to control what can happen on the E2 page. So recall that
E
p
,
q
2
=
H
p
(
S
n
+
1
;
H
q
(
Ω
S
n
+
1
)
)
.
{\displaystyle E_{p,q}^{2}=H_{p}(S^{n+1};H_{q}(\Omega S^{n+1})).}
Thus we know when q = 0, we are just looking at the regular integer valued homology groups Hp(Sn+1) which has value
Z
{\displaystyle \mathbb {Z} }
in degrees 0 and n+1 and value 0 everywhere else. However, since the path space is contractible, we know that by the time the sequence gets to E∞, everything becomes 0 except for the group at p = q = 0. The only way this can happen is if there is an isomorphism from
H
n
+
1
(
S
n
+
1
;
H
0
(
F
)
)
=
Z
{\displaystyle H_{n+1}(S^{n+1};H_{0}(F))=\mathbb {Z} }
to another group. However, the only places a group can be nonzero are in the columns p = 0 or p = n+1 so this isomorphism must occur on the page En+1 with codomain
H
0
(
S
n
+
1
;
H
n
(
F
)
)
=
Z
.
{\displaystyle H_{0}(S^{n+1};H_{n}(F))=\mathbb {Z} .}
However, putting a
Z
{\displaystyle \mathbb {Z} }
in this group means there must be a
Z
{\displaystyle \mathbb {Z} }
at Hn+1(Sn+1; Hn(F)). Inductively repeating this process shows that Hi(ΩSn+1) has value
Z
{\displaystyle \mathbb {Z} }
at integer multiples of n and 0 everywhere else.
= Cohomology ring of complex projective space
=We compute the cohomology of
C
P
n
{\displaystyle \mathbb {CP} ^{n}}
using the fibration:
S
1
↪
S
2
n
+
1
→
C
P
n
{\displaystyle S^{1}\hookrightarrow S^{2n+1}\to \mathbb {CP} ^{n}}
Now, on the E2 page, in the 0,0 coordinate we have the identity of the ring. In the 0,1 coordinate, we have an element i that generates
Z
.
{\displaystyle \mathbb {Z} .}
However, we know that by the limit page, there can only be nontrivial generators in degree 2n+1 telling us that the generator i must transgress to some element x in the 2,0 coordinate. Now, this tells us that there must be an element ix in the 2,1 coordinate. We then see that d(ix) = x2 by the Leibniz rule telling us that the 4,0 coordinate must be x2 since there can be no nontrivial homology until degree 2n+1. Repeating this argument inductively until 2n + 1 gives ixn in coordinate 2n,1 which must then be the only generator of
Z
{\displaystyle \mathbb {Z} }
in that degree thus telling us that the 2n + 1,0 coordinate must be 0. Reading off the horizontal bottom row of the spectral sequence gives us the cohomology ring of
C
P
n
{\displaystyle \mathbb {CP} ^{n}}
and it tells us that the answer is
Z
[
x
]
/
x
n
+
1
.
{\displaystyle \mathbb {Z} [x]/x^{n+1}.}
In the case of infinite complex projective space, taking limits gives the answer
Z
[
x
]
.
{\displaystyle \mathbb {Z} [x].}
= Fourth homotopy group of the three-sphere
=A more sophisticated application of the Serre spectral sequence is the computation
π
4
(
S
3
)
=
Z
/
2
Z
.
{\displaystyle \pi _{4}(S^{3})=\mathbb {Z} /2\mathbb {Z} .}
This particular example illustrates a systematic technique which one can use in order to deduce information about the higher homotopy groups of spheres. Consider the following fibration which is an isomorphism on
π
3
{\displaystyle \pi _{3}}
X
→
S
3
→
K
(
Z
,
3
)
,
{\displaystyle X\to S^{3}\to K(\mathbb {Z} ,3),}
where
K
(
π
,
n
)
{\displaystyle K(\pi ,n)}
is an Eilenberg–MacLane space. We then further convert the map
X
→
S
3
{\displaystyle X\to S^{3}}
to a fibration; it is general knowledge that the iterated fiber is the loop space of the base space so in our example we get that the fiber is
Ω
K
(
Z
,
3
)
=
K
(
Z
,
2
)
.
{\displaystyle \Omega K(\mathbb {Z} ,3)=K(\mathbb {Z} ,2).}
But we know that
K
(
Z
,
2
)
=
C
P
∞
.
{\displaystyle K(\mathbb {Z} ,2)=\mathbb {CP} ^{\infty }.}
Now we look at the cohomological Serre spectral sequence: we suppose we have a generator for the degree 3 cohomology of
S
3
{\displaystyle S^{3}}
, called
ι
{\displaystyle \iota }
. Since there is nothing in degree 3 in the total cohomology, we know this must be killed by an isomorphism. But the only element that can map to it is the generator a of the cohomology ring of
C
P
∞
{\displaystyle \mathbb {CP} ^{\infty }}
, so we have
d
(
a
)
=
ι
{\displaystyle d(a)=\iota }
. Therefore by the cup product structure, the generator in degree 4,
a
2
{\displaystyle a^{2}}
, maps to the generator
ι
a
{\displaystyle \iota a}
by multiplication by 2 and that the generator of cohomology in degree 6 maps to
ι
a
2
{\displaystyle \iota a^{2}}
by multiplication by 3, etc. In particular we find that
H
4
(
X
)
=
Z
/
2
Z
.
{\displaystyle H_{4}(X)=\mathbb {Z} /2\mathbb {Z} .}
But now since we killed off the lower homotopy groups of X (i.e., the groups in degrees less than 4) by using the iterated fibration, we know that
H
4
(
X
)
=
π
4
(
X
)
{\displaystyle H_{4}(X)=\pi _{4}(X)}
by the Hurewicz theorem, telling us that
π
4
(
S
3
)
=
Z
/
2
Z
.
{\displaystyle \pi _{4}(S^{3})=\mathbb {Z} /2\mathbb {Z} .}
Corollary:
π
4
(
S
2
)
=
Z
/
2
Z
.
{\displaystyle \pi _{4}(S^{2})=\mathbb {Z} /2\mathbb {Z} .}
Proof: Take the long exact sequence of homotopy groups for the Hopf fibration
S
1
→
S
3
→
S
2
{\displaystyle S^{1}\to S^{3}\to S^{2}}
.
See also
Gysin sequence
References
The Serre spectral sequence is covered in most textbooks on algebraic topology, e.g.
Allen Hatcher, Spectral Sequences
Edwin Spanier, Algebraic topology, Springer
Also
James Davis, Paul Kirk, Lecture notes in algebraic topology gives many nice applications of the Serre spectral sequence.
An elegant construction is due to
Andreas Dress, Zur Spektralsequenz einer Faserung, Inventiones Mathematicae 3 (1967), 172–178, EuDML.
The case of simplicial sets is treated in
Paul Goerss, Rick Jardine, Simplicial homotopy theory, Birkhäuser
Kata Kunci Pencarian:
- Serre spectral sequence
- Leray spectral sequence
- Spectral sequence
- Lyndon–Hochschild–Serre spectral sequence
- Fibration
- List of things named after Jean-Pierre Serre
- Inflation-restriction exact sequence
- Exact couple
- Atiyah–Hirzebruch spectral sequence
- Gysin homomorphism
