- Spectral sequence
In the area of

mathematics known ashomological algebra , especially inalgebraic topology andgroup cohomology , a**spectral sequence**is a means of computing homology groups by taking successive approximations. Spectral sequences are a generalization of exact sequences, and since their introduction byJean Leray in1946 , they have become an important research tool, particularly inhomotopy theory . However, they have a reputation for being abstruse and difficult to comprehend.**Discovery and motivation**Motivated by problems in

algebraic topology , Jean Leray introduced the notion of a sheaf and found himself faced with the problem of computingsheaf cohomology . To compute sheaf cohomology, Leray introduced a computational technique now known as theLeray spectral sequence . This gave a relationship between cohomology groups of a sheaf and cohomology groups of the pushforward of the sheaf. It was not a direct relation. Instead, Leray found that the cohomology groups of the pushforward formed a naturalchain complex , so that he could take the cohomology of the cohomology. The result was not the cohomology of the original sheaf, but it was closer, and it too formed a natural chain complex. Leray found that he could repeat this process, and that each step got him closer to the cohomology groups of the original sheaf. Taking the limit of the iterated cohomologies gave him exactly the cohomology groups of the original sheaf. This allowed Leray to compute sheaf cohomology.It was soon realized that Leray's computational technique was an example of a more general phenomenon. Spectral sequences were found in diverse situations, and they gave intricate relationships among homology and cohomology groups coming from geometric situations such as

fibration s and from algebraic situations involvingderived functors . While their theoretical importance has decreased since the introduction of derived categories, they are still the most effective computational tool available. This is true even when many of the terms of the spectral sequence are incalculable.Unfortunately, because of the large amount of information carried in spectral sequences, they are difficult to grasp. This information is usually contained in a rank three lattice of

abelian group s or modules. In most cases that can be computed, the spectral sequence eventually collapses, meaning that going out further in the sequence produces no new information. This does not always happen, however, and then it becomes necessary to use tricks to extract useful information. Even in these cases, however, it is still possible to get useful information from a spectral sequence.**Formal definition**Fix an

abelian category , such as a category of modules over a ring. A**spectral sequence**is a choice of a nonnegative integer "r_{0}" and a collection of three sequences:

# For all integers "r" ≥ "r_{0}", an object "E_{r}", called a "sheet" (as in a sheet ofpaper ),

# Endomorphisms "d_{r}" : "E_{r}" → "E_{r}" satisfying "d_{r}" o "d_{r}" = 0, called "boundary maps" or "differentials",

# Isomorphisms of "E_{r+1}" with "H"("E_{r}"), the homology of "E_{r}" with respect to "d_{r}".Usually the isomorphisms between "E

_{r+1}" and "H"("E_{r}") are suppressed, and we write equalities instead. "E_{r+1}" is sometimes called the**derived object**of "E_{r}".The most elementary example is a

chain complex "C_{•}". "C_{•}" is an object in an abelian category of chain complexes, and it comes with a differential "d". Let "r_{0}" = 0, and let "E_{0}" be "C_{•}". This forces "E_{1}" to be the complex "H"("C_{•}"): At the "i"' th location this is the "i"' th homology group of "C_{•}". The only natural differential on this new complex is the zero map, so we let "d_{1}" = 0. This forces "E_{2}" to equal "E_{1}", and again our only natural differential is the zero map. Putting the zero differential on all the rest of our sheets gives a spectral sequence whose terms are:* "E

_{0}" = "C_{•}"

* "E_{r}" = "H"("C_{•}") for all "r" ≥ 1.The terms of this spectral sequence stabilize at the first sheet because its only nontrivial differential was on the zeroth sheet. Consequently we can get no more information at later steps. Usually, to get useful information from later sheets, we need extra structure on the "E

_{r}".In the ungraded situation described above, "r

_{0}" is irrelevant, but in practice most spectral sequences occur in the category of doubly graded modules over a ring "R" (or doubly graded sheaves of modules over a sheaf of rings). The degree of the boundary maps depends on "r" and is fixed by convention. For a homological spectral sequence, the terms are written $E^r\_\{p,q\}$ and the differentials have bidegree (-r,r-1). For a cohomological spectral sequence, the terms are written $E^\{p,q\}\_r$ and the differentials have bidegree (r,1-r). (These choices of bidegree occur naturally in practice; see the example of a double complex below.) Depending upon the spectral sequence, the boundary map on the first sheet can have a degree which corresponds to "r" = 0, "r" = 1, or "r" = 2. For example, for the spectral sequence of a filtered complex, described below, "r_{0}" = 0, but for theGrothendieck spectral sequence , "r_{0}" = 2. Usually "r_{0}" is zero, one, or two.A morphism of spectral sequences "E" → "E' " is by definition a collection of maps "f

_{r}" : "E_{r}" → "E'_{r}" which commute with the given isomorphisms between cohomology of the "r"-th step and the ("r+1")-st step of "E" and "E' ", respectively. The category of spectral sequences is an abelian category.**Exact couples**The most powerful technique for the construction of spectral sequences is William Massey's method of exact couples. Exact couples are particularly common in algebraic topology, where there are many spectral sequences for which no other construction is known. In fact, all known spectral sequences can be constructed using exact couples. Despite this they are unpopular in abstract algebra, where most spectral sequences come from filtered complexes. To define exact couples, we begin again with an abelian category. As before, in practice this is usually the category of doubly graded modules over a ring. An

**exact couple**is a pair of objects "A" and "C", together with three homomorphisms between these objects: "f" : "A" → "A", "g" : "A" → "C" and "h" : "C" → "A" subject to certain exactness conditions:*Image "f" = Kernel "g"

*Image "g" = Kernel "h"

*Image "h" = Kernel "f"We will abbreviate this data by ("A", "C", "f", "g", "h"). Exact couples are usually depicted as triangles. We will see that "C" corresponds to the "E

_{0}" term of the spectral sequence and that "A" is some auxiliary data.To pass to the next sheet of the spectral sequence, we will form the

**derived couple**. We set:*"d" = "g" o "h"

*"A' " = "f"("A")

*"C' " = Ker "d" / Im "d"

*"f' " = "f"|_{"A'"}, the restriction of "f" to "A' "

*"h' " : "C' " → "A' " is induced by "h". It is straightforward to see that "h" induces such a map.

*"g' " : "A' " → "C' " is defined on elements as follows: For each "a" in "A' ", write "a" as "f"("b") for some "b" in "A' ". "g' "("a") is defined to be the image of "g"("b") in "C' ". In general, "g' " can be constructed using one of the embedding theorems for abelian categories.From here it is straightforward to check that ("A

' ", "C' ", "f' ", "g' ", "h' ") is an exact couple. "C' " corresponds to the "E_{1}" term of the spectral sequence. We can iterate this procedure to get exact couples ("A"^{("n")}, "C"^{("n")}, "f"^{("n")}, "g"^{("n")}, "h"^{("n")}). We let "E_{n}" be "C"^{("n")}and "d_{n}" be "g"^{("n")}o "h"^{("n")}. This gives a spectral sequence.**Visualization**A doubly graded spectral sequence has a tremendous amount of data to keep track of, but there is a common visualization technique which makes the structure of the spectral sequence clearer. We have three indices, "r", "p", and "q". For each "r", imagine that we have a sheet of graph paper. On this sheet, we will take "p" to be the horizontal direction and "q" to be the vertical direction. At each lattice point we have the object $E\_r^\{p,q\}$.

It is very common for "n" = "p" + "q" to be another natural index in the spectral sequence. "n" runs diagonally, northwest to southeast, across each sheet. In the homological case, the differentials have bidegree (-r,r-1), so they decrease "n" by one. In the cohomological case, "n" is increased by one. When "r" is zero, the differential moves objects one space to the right or left. This is similar to the differential on a chain complex. When "r" is one, the differential moves objects one space down or up. When "r" is two, the differential moves objects just like a knight's move in

chess . For higher "r", the differential acts like a generalized knight's move.**Examples of spectral sequences****The spectral sequence of a filtered complex**A very common type of spectral sequence comes from a filtered cochain complex. This is a cochain complex "C

^{•}" together with a set of subcomplexes "F^{p}C^{•}", where "p" ranges across all integers. (In practice, "p" is usually bounded on one side.) We require that the boundary map is compatible with the filtration; this means that "d"("F^{p}C^{n}") ⊆ "F^{p}C^{n+1}". We assume that the filtration is "descending", i.e., "F^{p}C^{•}" ⊇ "F^{p+1}C^{•}". We will number the terms of the cochain complex by "n". Later, we will also assume that the filtration is "Hausdorff" or "separated", that is, the intersection of the set of all "F^{p}C^{•}" is zero, and that the filtration is "exhaustive", that is, the union of the set of all "F^{p}C^{•}" is the entire chain complex "C^{•}".The filtration is useful because it gives a measure of nearness to zero: As "p" increases, "F

^{p}C^{•}" gets closer and closer to zero. We will construct a spectral sequence from this filtration where boundaries and cycles in later sheets get closer and closer to boundaries and cycles in the original complex. This spectral sequence will be doubly graded. One of the grades will be the filtration degree "p". The other is called the "complementary degree" and is denoted "q". The complementary degree satisfies the relation "p" + "q" = "n". (We use the complementary degree instead of the location in the chain complex because this is more natural in the common case of the spectral sequence of a double complex, explained below.)We will construct this spectral sequence by hand. "C

^{•}" has only a single grading and a filtration, so we first construct a doubly graded object from "C^{•}". To get the second grading, we will take the associated graded object with respect to the filtration. We will write it in an unusual way which will be justified at the "E_{1}" step::$Z\_\{-1\}^\{p,q\}\; =\; Z\_0^\{p,q\}\; =\; F^p\; C^\{p+q\}$:$B\_0^\{p,q\}\; =\; 0$:$E\_0^\{p,q\}\; =\; frac\{Z\_0^\{p,q\{B\_0^\{p,q\}\; +\; Z\_\{-1\}^\{p+1,q-1\; =\; frac\{F^p\; C^\{p+q\{F^\{p+1\}\; C^\{p+q$:$E\_0\; =\; igoplus\_\{p,qinold\{Z\; E\_0^\{p,q\}$

Since we assumed that the boundary map was compatible with the filtration, "E

_{0}" is a doubly graded object and there is a natural doubly graded boundary map "d_{0}" on "E_{0}". To get "E_{1}", we take the homology of "E_{0}".:$ar\{Z\}\_1^\{p,q\}\; =\; ker\; d\_0^\{p,q\}\; :\; E\_0^\{p,q\}\; ightarrow\; E\_0^\{p,q+1\}\; =\; ker\; d\_0^\{p,q\}\; :\; F^p\; C^\{p+q\}/F^\{p+1\}\; C^\{p+q\}\; ightarrow\; F^p\; C^\{p+q+1\}/F^\{p+1\}\; C^\{p+q+1\}$:$ar\{B\}\_1^\{p,q\}\; =\; mbox\{im\; \}\; d\_0^\{p,q-1\}\; :\; E\_0^\{p,q-1\}\; ightarrow\; E\_0^\{p,q\}\; =\; mbox\{im\; \}\; d\_0^\{p,q-1\}\; :\; F^p\; C^\{p+q-1\}/F^\{p+1\}\; C^\{p+q-1\}\; ightarrow\; F^p\; C^\{p+q\}/F^\{p+1\}\; C^\{p+q\}$:$E\_1^\{p,q\}\; =\; frac\{ar\{Z\}\_1^\{p,q\{ar\{B\}\_1^\{p,q\; =\; frac\{ker\; d\_0^\{p,q\}\; :\; E\_0^\{p,q\}\; ightarrow\; E\_0^\{p,q+1\{mbox\{im\; \}\; d\_0^\{p,q-1\}\; :\; E\_0^\{p,q-1\}\; ightarrow\; E\_0^\{p,q$:$E\_1\; =\; igoplus\_\{p,qinold\{Z\; E\_1^\{p,q\}\; =\; igoplus\_\{p,qinold\{Z\; frac\{ar\{Z\}\_1^\{p,q\{ar\{B\}\_1^\{p,q$

Notice that $ar\{Z\}\_1^\{p,q\}$ and $ar\{B\}\_1^\{p,q\}$ can be written as the images in $E\_0^\{p,q\}$ of :$Z\_1^\{p,q\}\; =\; ker\; d\_0^\{p,q\}\; :\; F^p\; C^\{p+q\}\; ightarrow\; C^\{p+q+1\}/F^\{p+1\}\; C^\{p+q+1\}$:$B\_1^\{p,q\}\; =\; (mbox\{im\; \}\; d\_0^\{p,q-1\}\; :\; F^\{p-1\}\; C^\{p+q-1\}\; ightarrow\; C^\{p+q\})\; cap\; F^p\; C^\{p+q\}$

and that we then have

:$E\_1^\{p,q\}\; =\; frac\{Z\_1^\{p,q\{B\_1^\{p,q\}\; +\; Z\_0^\{p+1,q-1$.

$Z\_1^\{p,q\}$ is exactly the stuff which the differential pushes up one level in the filtration, and $B\_1^\{p,q\}$ is exactly the image of the stuff which the differential pushes up one level in the filtration. This suggests that we should choose $Z\_r^\{p,q\}$ to be the stuff which the differential pushes up "r" levels in the filtration and $B\_r^\{p,q\}$ to be image of the stuff which the differential pushes up "r" levels in the filtration. In other words, the spectral sequence should satisfy

:$Z\_r^\{p,q\}\; =\; ker\; d\_0^\{p,q\}\; :\; F^p\; C^\{p+q\}\; ightarrow\; C^\{p+q+1\}/F^\{p+r\}\; C^\{p+q+1\}$:$B\_r^\{p,q\}\; =\; (mbox\{im\; \}\; d\_0^\{p,q-r\}\; :\; F^\{p-r\}\; C^\{p+q-1\}\; ightarrow\; C^\{p+q\})\; cap\; F^p\; C^\{p+q\}$:$E\_r^\{p,q\}\; =\; frac\{Z\_r^\{p,q\{B\_r^\{p,q\}\; +\; Z\_r^\{p+1,q-1$

and we should have the relationship

:$B\_r^\{p,q\}\; =\; d\_0^\{p,q\}(Z\_r^\{p-r,q+r-1\})$.

For this to make sense, we must find a differential on each "E

_{r}" which gives the "E_{r+1}" we stated above. Since we have written $Z\_r^\{p,q\}$ as a subobject of $C^\{p+q\}$, we get a differential on $E\_r^\{p,q\}$ by restricting the differential on $C^\{p+q\}$: :$d\_r^\{p,q\}\; :\; E\_r^\{p,q\}\; ightarrow\; E\_r^\{p+r,q-r+1\}$Now it is straightforward to check that the homology of "E

_{r}" with respect to this differential is "E_{r+1}", so this gives a spectral sequence. Unfortunately, the differential is not very explicit. Determining differentials or finding ways to work around them is one of the main challenges to successfully applying a spectral sequence.**The spectral sequence of a double complex**Another common spectral sequence is the spectral sequence of a double complex. A "double complex" is a collection of objects "C

_{i,j}" for all integers "i" and "j" together with two differentials, "d^{I}" and "d^{II}". "d^{I}" is assumed to decrease "i", and "d^{II}" is assumed to decrease "j". Furthermore, we assume that the differentials "anticommute", so that "d^{I}d^{II}" + "d^{II}d^{I}" = 0. Our goal is to compare the iterated homologies $H^I\_i(H^\{II\}\_j(C\_\{ull,ull\}))$ and $H^\{II\}\_j(H^I\_i(C\_\{ull,ull\}))$. We will do this by filtering our double complex in two different ways. Here are our filtrations::$(C\_\{i,j\}^I)\_p\; =\; left\{egin\{matrix\}0\; mbox\{if\; \}\; i\; p\; \backslash C\_\{i,j\}\; mbox\{if\; \}\; i\; ge\; p\; end\{matrix\}\; ight.$:$(C\_\{i,j\}^\{II\})\_p\; =\; left\{egin\{matrix\}0\; mbox\{if\; \}\; j\; p\; \backslash C\_\{i,j\}\; mbox\{if\; \}\; j\; ge\; p\; end\{matrix\}\; ight.$

To get a spectral sequence, we will reduce to the previous example. We define the "total complex" "T(C

_{•,•})" to be the complex whose "n"' th term is $igoplus\_\{i+j=n\}\; C\_\{i,j\}$ and whose differential is "d^{I}" + "d^{II}". This is a complex because "d^{I}" and "d^{II}" are anticommuting differentials. The two filtrations on "C_{i,j}" give two filtrations on the total complex::$T\_n(C\_\{ull,ull\})^I\_p\; =\; igoplus\_\{i+j=n\; atop\; i\; p\}\; C\_\{i,j\}$:$T\_n(C\_\{ull,ull\})^\{II\}\_p\; =\; igoplus\_\{i+j=n\; atop\; j\; p\}\; C\_\{i,j\}$

To show that these spectral sequences give information about the iterated homologies, we will work out the "E

^{0}", "E^{1}", and "E^{2}" terms of the "I" filtration on "T(C_{•,•})". The "E^{0}" term is clear::$\{\}^IE^0\_\{p,q\}\; =T\_n(C\_\{ull,ull\})^I\_p\; /\; T\_n(C\_\{ull,ull\})^I\_\{p+1\}\; =igoplus\_\{i+j=n\; atop\; i\; p\}\; C\_\{i,j\}\; Big/igoplus\_\{i+j=n\; atop\; i\; p+1\}\; C\_\{i,j\}\; =C\_\{p,q\}$

To find the "E

^{1}" term, we need to determine "d^{I}" + "d^{II}" on "E^{0}". Notice that the differential must have degree 1 with respect to "n", so we get a map:$d^I\_\{p,q\}\; +\; d^\{II\}\_\{p,q\}\; :T\_n(C\_\{ull,ull\})^I\_p\; /\; T\_n(C\_\{ull,ull\})^I\_\{p+1\}\; =C\_\{p,q\}\; ightarrowT\_\{n-1\}(C\_\{ull,ull\})^I\_p\; /\; T\_\{n-1\}(C\_\{ull,ull\})^I\_\{p+1\}\; =C\_\{p,q-1\}$

Consequently, the differential on "E

^{0}" is the map "C_{p,q}" → "C_{p,q-1}" induced by "d^{I}" + "d^{II}". But "d^{I}" has the wrong degree to induce such a map, so "d^{I}" must be zero on "E^{0}". That means the differential is exactly "d^{II}", so we get:$\{\}^IE^1\_\{p,q\}\; =\; H^\{II\}\_q(C\_\{p,ull\})$.

To find "E

^{2}", we need to determine:$d^I\_\{p,q\}\; +\; d^\{II\}\_\{p,q\}\; :H^\{II\}\_q(C\_\{p,ull\})\; ightarrowH^\{II\}\_q(C\_\{p+1,ull\})$

Because "E

^{1}" was exactly the homology with respect to "d^{II}", "d^{II}" is zero on "E^{1}". Consequently, we get:$\{\}^IE^2\_\{p,q\}\; =\; H^I\_p(H^\{II\}\_q(C\_\{ull,ull\}))$.

Using the other filtration gives us a different spectral sequence with a similar "E

^{2}" term::$\{\}^\{II\}E^2\_\{p,q\}\; =\; H^\{II\}\_q(H^\{I\}\_p(C\_\{ull,ull\}))$.

What remains is to find a relationship between these two spectral sequences. It will turn out that as "r" increases, the two sequences will become similar enough to allow useful comparisons.

**Convergence, degeneration, and abutment**In the elementary example that we began with, the sheets of the spectral sequence were constant once "r" was at least 1. In that setup it makes sense to take the limit of the sequence of sheets: Since nothing happens after the zeroth sheet, the limiting sheet "E"

_{∞}is the same as "E"_{1}.In more general situations, limiting sheets often exist and are always interesting. They are one of the most powerful aspects of spectral sequences. We say that a spectral sequence $E\_r^\{p,q\}$

**converges to**or**abuts to**$E\_infty^\{p,q\}$ if there is an "r"("p", "q") such that for all "r" ≥ "r"("p", "q"), the differentials $d\_r^\{p-r,q+r-1\}$ and $d\_r^\{p,q\}$ are zero. This forces $E\_r^\{p,q\}$ to be isomorphic to $E\_infty^\{p,q\}$ for large "r". In symbols, we write::$E\_r^\{p,q\}\; Rightarrow\_p\; E\_infty^\{p,q\}$

The "p" indicates the filtration index. It is very common to write the $E\_2^\{p,q\}$ term on the left-hand side of the abutment, because this is the most useful term of most spectral sequences.

In most spectral sequences, the $E\_infty$ term is not naturally a doubly graded object. Instead, there are usually $E\_infty^n$ terms which come with a natural filtration $F^ullet\; E\_infty^n$. In these cases, we set $E\_infty^\{p,q\}\; =\; mbox\{gr\}\_p\; E\_infty^\{p+q\}\; =\; F^pE\_infty^\{p+q\}/F^\{p+1\}E\_infty^\{p+q\}$. We define convergence in the same way as before, but we write

:$E\_r^\{p,q\}\; Rightarrow\_p\; E\_infty^n$

to mean that whenever "p" + "q" = "n", $E\_r^\{p,q\}$ converges to $E\_infty^\{p,q\}$.

The simplest situation in which we can determine convergence is when the spectral sequences degenerates. We say that the spectral sequences

**degenerates at sheet r**if, for any "s" ≥ "r", the differential "d_{s}" is zero. This implies that "E_{r}" ≅ "E"_{"r"+1}≅ "E"_{"r"+2}≅ ... In particular, it implies that "E_{r}" is isomorphic to "E_{∞}". This is what happened in our first, trivial example of an unfiltered chain complex: The spectral sequence degenerated at the first sheet. In general, if a doubly-graded spectral sequence is zero outside of a horizontal or vertical strip, the spectral sequence will degenerate, because later differentials will always go to or from an object not in the strip.The spectral sequence also converges if $E\_r^\{p,q\}$ vanishes for all "p" less than some "p"

_{0}and for all "q" less than some "q"_{0}. If "p"_{0}and "q"_{0}can be chosen to be zero, this is called a**first-quadrant spectral sequence**. This sequence converges because each object is a fixed distance away from the edge of the non-zero region. Consequently, for a fixed "p" and "q", the differential on later sheets always maps $E\_r^\{p,q\}$ from or to the zero object; more visually, the differential leaves the quadrant where the terms are nonzero. The spectral sequence need not degenerate, however, because the differential maps might not all be zero at once. Similarly, the spectral sequence also converges if $E\_r^\{p,q\}$ vanishes for all "p" greater than some "p"_{0}and for all "q" greater than some "q"_{0}.The

five-term exact sequence of a spectral sequence relates certain low-degree terms and "E"_{∞}terms.**Examples of degeneration****The spectral sequence of a filtered complex, continued**Notice that we have a chain of inclusions:

:$Z\_0^\{p,q\}\; supe\; Z\_1^\{p,q\}\; supe\; Z\_2^\{p,q\}supecdotssupe\; B\_2^\{p,q\}\; supe\; B\_1^\{p,q\}\; supe\; B\_0^\{p,q\}$

We can ask what happens if we define

:$Z\_infty^\{p,q\}\; =\; igcap\_\{r=0\}^infty\; Z\_r^\{p,q\}$,:$B\_infty^\{p,q\}\; =\; igcup\_\{r=0\}^infty\; B\_r^\{p,q\}$,:$E\_infty^\{p,q\}\; =\; Z\_infty^\{p,q\}/B\_infty^\{p,q\}$.

$E\_infty^\{p,q\}$ is a natural candidate for the abutment of this spectral sequence. Convergence is not automatic, but happens in many cases. In particular, if the filtration is finite and consists of exactly "r" nontrivial steps, then the spectral sequence degenerates after the "r"

' th sheet. Convergence also occurs if the complex and the filtration are both bounded below or both bounded above.To describe the abutment of our spectral sequence in more detail, notice that we have the formulas:

:$Z\_infty^\{p,q\}\; =\; igcap\_\{r=0\}^infty\; Z\_r^\{p,q\}\; =\; igcap\_\{r=0\}^infty\; ker(F^p\; C^\{p+q\}\; ightarrow\; C^\{p+q+1\}/F^\{p+r\}\; C^\{p+q+1\}$):$B\_infty^\{p,q\}\; =\; igcup\_\{r=0\}^infty\; B\_r^\{p,q\}\; =\; igcap\_\{r=0\}^infty\; (mbox\{im\; \}\; d^\{p,q-r\}\; :\; F^\{p-r\}\; C^\{p+q-1\}\; ightarrow\; C^\{p+q\})\; cap\; F^p\; C^\{p+q\}$

To see what this implies for $Z\_infty^\{p,q\}$ recall that we assumed that the filtration was separated. This implies that as "r" increases, the kernels shrink, until we are left with $Z\_infty^\{p,q\}\; =\; ker(F^p\; C^\{p+q\}\; ightarrow\; C^\{p+q+1\})$. For $B\_infty^\{p,q\}$, recall that we assumed that the filtration was exhaustive. This implies that as "r" increases, the images grow until we reach $B\_infty^\{p,q\}\; =\; mbox\{im\; \}(C^\{p+q-1\}\; ightarrow\; C^\{p+q\})\; cap\; F^p\; C^\{p+q\}$. We conclude

:$E\_infty^\{p,q\}\; =\; mbox\{gr\}\_p\; H^\{p+q\}(C^ull)$,

that is, the abutment of the spectral sequence is the "p"

' th graded part of the "p+q"' th homology of "C". If our spectral sequence converges, then we conclude that::$E\_r^\{p,q\}\; Rightarrow\_p\; H^\{p+q\}(C^ull)$

**Long exact sequences**Using the spectral sequence of a filtered complex, we can derive the existence of

long exact sequence s. Choose a short exact sequence of cochain complexes 0 → "A^{•}" → "B^{•}" → "C^{•}" → 0, and call the first map "f^{•}" : "A^{•}" → "B^{•}". We get natural maps of homology objects "H^{n}"("A^{•}") → "H^{n}"("B^{•}") → "H^{n}"("C^{•}"), and we know that this is exact in the middle. We will use the spectral sequence of a filtered complex to find the connecting homomorphism and to prove that the resulting sequence is exact. To start, we filter "B^{•}"::$F^0\; B^n\; =\; B^n$:$F^1\; B^n\; =\; A^n$:$F^2\; B^n\; =\; 0$

This gives:

:$E^\{p,q\}\_0=\; frac\{F^p\; B^\{p+q\{F^\{p+1\}\; B^\{p+q\; =\; left\{egin\{matrix\}0\; mbox\{if\; \}\; p\; 0\; mbox\{\; or\; \}\; p\; 1\; \backslash C^q\; mbox\{if\; \}\; p\; =\; 0\; \backslash A^\{q+1\}\; mbox\{if\; \}\; p\; =\; 1\; end\{matrix\}\; ight.$:$E^\{p,q\}\_1=\; left\{egin\{matrix\}0\; mbox\{if\; \}\; p\; 0\; mbox\{\; or\; \}\; p\; 1\; \backslash H^q(C^ull)\; mbox\{if\; \}\; p\; =\; 0\; \backslash H^\{q+1\}(A^ull)\; mbox\{if\; \}\; p\; =\; 1\; end\{matrix\}\; ight.$

The differential has bidegree (1, 0), so "d

_{0,q}" : "H^{q}"("C^{•}") → "H"^{"q"+1}("A^{•}"). These are the connecting homomorphisms from thesnake lemma , and together with the maps "A^{•}" → "B^{•}" → "C^{•}", they give a sequence::$cdots\; ightarrow\; H^q(B^ull)\; ightarrow\; H^q(C^ull)\; ightarrow\; H^\{q+1\}(A^ull)\; ightarrow\; H^\{q+1\}(B^ull)\; ightarrowcdots$

It remains to show that this sequence is exact at the "A" and "C" spots. Notice that this spectral sequence degenerates at the "E"

_{2}term because the differentials have bidegree (2, −1). Consequently, the "E"_{2}term is the same as the "E"_{∞}term::$E^\{p,q\}\_2cong\; mbox\{gr\}\_p\; H^\{p+q\}(B^ull)=\; left\{egin\{matrix\}0\; mbox\{if\; \}\; p\; 0\; mbox\{\; or\; \}\; p\; 1\; \backslash H^q(B^ull)/H^q(A^ull)\; mbox\{if\; \}\; p\; =\; 0\; \backslash mbox\{im\; \}\; H^\{q+1\}f^ull\; :\; H^\{q+1\}(A^ull)\; ightarrow\; H^\{q+1\}(B^ull)\; mbox\{if\; \}\; p\; =\; 1\; end\{matrix\}\; ight.$

But we also have a direct description of the "E"

_{2}term as the homology of the "E"_{1}term. These two descriptions must be isomorphic::$H^q(B^ull)/H^q(A^ull)\; cong\; ker\; d^1\_\{0,q\}\; :\; H^q(C^ull)\; ightarrow\; H^\{q+1\}(A^ull)$:$mbox\{im\; \}\; H^\{q+1\}f^ull\; :\; H^\{q+1\}(A^ull)\; ightarrow\; H^\{q+1\}(B^ull)\; cong\; H^\{q+1\}(A^ull)\; /\; (mbox\{im\; \}\; d^1\_\{0,q\}\; :\; H^q(C^ull)\; ightarrow\; H^\{q+1\}(A^ull))$

The former gives exactness at the "C" spot, and the latter gives exactness at the "A" spot.

**The spectral sequence of a double complex, continued**Using the abutment for a filtered complex, we find that:

:$H^I\_p(H^\{II\}\_q(C\_\{ull,ull\}))\; Rightarrow\_p\; H^\{p+q\}(T(C\_\{ull,ull\}))$:$H^\{II\}\_q(H^I\_p(C\_\{ull,ull\}))\; Rightarrow\_q\; H^\{p+q\}(T(C\_\{ull,ull\}))$

In general, "the two gradings on H

^{p+q}(T(C_{•,•})) are distinct". Despite this, it is still possible to gain useful information from these two spectral sequences.**Commutativity of Tor**Let "M" and "N" be "R"-modules. Recall that the derived functors of the tensor product are denoted Tor. Tor is defined using a projective resolution of its first argument. However, it turns out that Tor

_{"i"}("M", "N") = Tor_{"i"}("N", "M"). While this can be verified without a spectral sequence, it is very easy with spectral sequences.Choose projective resolutions "P

_{•}" and "Q"_{•}of "M" and "N", respectively. Consider these as complexes which vanish in negative degree having differentials "d" and "e", respectively. We can construct a double complex whose terms are "C_{i,j}" = "P_{i}" ⊗ "Q_{j}" and whose differentials are "d" ⊗ 1 and (−1)^{"j"}(1 ⊗ "e"). (The factor of −1 is so that the differentials anticommute.) Since projective modules are flat, taking the tensor product with a projective module commutes with taking homology, so we get::$H^I\_p(H^\{II\}\_q(P\_ull\; otimes\; Q\_ull))\; =\; H^I\_p(P\_ull\; otimes\; H^\{II\}\_q(Q\_ull))$:$H^\{II\}\_q(H^I\_p(P\_ull\; otimes\; Q\_ull))\; =\; H^\{II\}\_q(Q\_ull\; otimes\; H^I\_p(P\_ull))$

Since the two complexes are resolutions, their homology vanishes outside of degree zero. In degree zero, we are left with

:$H^I\_p(P\_ull\; otimes\; N)\; =\; mbox\{Tor\}\_p(M,N)$:$H^\{II\}\_q(Q\_ull\; otimes\; M)\; =\; mbox\{Tor\}\_q(N,M)$

In particular, the $E^2\_\{p,q\}$ terms vanish except along the lines "p" = 0 (for one spectral sequence) and "q" = 0 (for the other). This implies that the spectral sequence degenerates at the second sheet. We get isomorphisms:

:$mbox\{Tor\}\_p(M,N)\; cong\; E^infty\_\{p,q\}\; =\; mbox\{gr\}\_p\; H^\{p+q\}(T(C\_\{ull,ull\}))$:$mbox\{Tor\}\_q(N,M)\; cong\; E^infty\_\{p,q\}\; =\; mbox\{gr\}\_q\; H^\{p+q\}(T(C\_\{ull,ull\}))$

Finally, when "p" and "q" are equal, we get isomorphisms of the two right-hand sides, even after accounting for their different gradings, and the commutativity of Tor follows.

**Further examples**Some notable spectral sequences are:

*Adams spectral sequence instable homotopy theory

*Adams-Novikov spectral sequence , a generalization to extraordinary cohomology theories.

*Atiyah-Hirzebruch spectral sequence of anextraordinary cohomology theory

*Bar spectral sequence for the homology of the classifying space of a group.

*Barratt spectral sequence converging to the homotopy of the initial space of a cofibration.

*Bloch-Lichtenbaum spectral sequence converging to the algebraic K-theory of a field.

*Bockstein spectral sequence relating the homology with mod "p" coefficients and the homology reduced mod "p".

*Bousfield-Kan spectral sequence converging to the homotopy colimit of a functor.

*Cartan-Leray spectral sequence converging to the homology of a quotient space.

*Change of rings spectral sequence s for calculating Tor and Ext groups of modules.

*Chromatic spectral sequence for calculating the initial terms of theAdams-Novikov spectral sequence.

*Connes spectral sequence s converging to the cyclic homology of an algebra.

*EHP spectral sequence converging tostable homotopy groups of spheres

*Eilenberg-Moore spectral sequence for thesingular cohomology of thepullback of afibration

*Federer spectral sequence converging to homotopy groups of a function space.

*Frölicher spectral sequence starting from theDolbeault cohomology and converging to thealgebraic de Rham cohomology of a variety.

*Green's spectral sequence forKoszul cohomology

*Grothendieck spectral sequence for composingderived functor s

*Hodge-de Rham spectral sequence converging to thealgebraic de Rham cohomology of a variety.

*Hurewicz spectral sequence for calculating the homology of a space from its homotopy.

*Hyperhomology spectral sequence for calculating hyper homology.

*Kunneth spectral sequence for calcuating the homology of a tensor product of differential algebras.

*Leray spectral sequence converging to the cohomology of a sheaf.

*Leray-Serre spectral sequence of afibration

*Lyndon-Hochschild-Serre spectral sequence ingroup cohomology

*May spectral sequence for calcuating the Tor or Ext groups of an algebra.

*Miller spectral sequence converging to the mod "p" stable homology of a space.

*Milnor spectral sequence is another name for thebar spectral sequence .

*Moore spectral sequence is another name for thebar spectral sequence .

*Quillen spectral sequence for calcuating the homotopy of a simplicial group.

*Rothenberg-Steenrod spectral sequence is another name for thebar spectral sequence .

*Spectral sequence of a differential filtered group: described in this article.

*Spectral sequence of a double complex: described in this article.

*Spectral sequence of an exact couple: described in this article.

*Universal coefficient spectral sequence

*van Est spectral sequence converging to relative Lie algebra cohomology.

*van Kampen spectral sequence for calculating the homotopy of a wedge of spaces.**References****Historical references***

*

*

*

***Modern references***

*cite book

last = Hatcher

first = Allen

title = Spectral Sequences in Algebraic Topology

url = http://www.math.cornell.edu/~hatcher/SSAT/SSATpage.html

format = PDF

* | year=2001 | volume=58

*

* | year=1994

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