Spectral sequence

Spectral sequence

In the area of mathematics known as homological algebra, especially in algebraic topology and group 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 by Jean Leray in 1946, they have become an important research tool, particularly in homotopy 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 computing sheaf cohomology. To compute sheaf cohomology, Leray introduced a computational technique now known as the Leray 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 natural chain 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 fibrations and from algebraic situations involving derived 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 groups 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 "r0" and a collection of three sequences:
# For all integers "r" ≥ "r0", an object "Er", called a "sheet" (as in a sheet of paper),
# Endomorphisms "dr" : "Er" → "Er" satisfying "dr" o "dr" = 0, called "boundary maps" or "differentials",
# Isomorphisms of "Er+1" with "H"("Er"), the homology of "Er" with respect to "dr".

Usually the isomorphisms between "Er+1" and "H"("Er") are suppressed, and we write equalities instead. "Er+1" is sometimes called the derived object of "Er".

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 "r0" = 0, and let "E0" be "C". This forces "E1" 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 "d1" = 0. This forces "E2" to equal "E1", 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:

* "E0" = "C"
* "Er" = "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 "Er".

In the ungraded situation described above, "r0" 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, "r0" = 0, but for the Grothendieck spectral sequence, "r0" = 2. Usually "r0" is zero, one, or two.

A morphism of spectral sequences "E" → "E' " is by definition a collection of maps "fr" : "Er" → "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 "E0" 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 "E1" 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 "En" be "C"("n") and "dn" 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 "FpC", 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"("FpCn") ⊆ "FpCn+1". We assume that the filtration is "descending", i.e., "FpC" ⊇ "Fp+1C". 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 "FpC" is zero, and that the filtration is "exhaustive", that is, the union of the set of all "FpC" is the entire chain complex "C".

The filtration is useful because it gives a measure of nearness to zero: As "p" increases, "FpC" 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 "E1" 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, "E0" is a doubly graded object and there is a natural doubly graded boundary map "d0" on "E0". To get "E1", we take the homology of "E0".

: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 "Er" which gives the "Er+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 "Er" with respect to this differential is "Er+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 "Ci,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 \C_{i,j} & mbox{if } i ge p end{matrix} ight.:(C_{i,j}^{II})_p = left{egin{matrix}0 & mbox{if } j < p \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 "Ci,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 "E0", "E1", and "E2" terms of the "I" filtration on "T(C•,•)". The "E0" 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 "E1" term, we need to determine "d I" + "d II" on "E0". 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 "E0" is the map "Cp,q" → "Cp,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 "E0". That means the differential is exactly "d II", so we get

:{}^IE^1_{p,q} = H^{II}_q(C_{p,ull}).

To find "E2", 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 "E1" was exactly the homology with respect to "d II", "d II" is zero on "E1". 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 "E2" 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 "ds" is zero. This implies that "Er" ≅ "E""r"+1 ≅ "E""r"+2 ≅ ... In particular, it implies that "Er" 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 sequences. 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 "Hn"("A") → "Hn"("B") → "Hn"("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 \C^q & mbox{if } p = 0 \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 \H^q(C^ull) & mbox{if } p = 0 \H^{q+1}(A^ull) & mbox{if } p = 1 end{matrix} ight.

The differential has bidegree (1, 0), so "d0,q" : "Hq"("C") → "H""q"+1("A"). These are the connecting homomorphisms from the snake 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 \H^q(B^ull)/H^q(A^ull) & mbox{if } p = 0 \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 Hp+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 "Ci,j" = "Pi" ⊗ "Qj" 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 in stable homotopy theory
*Adams-Novikov spectral sequence, a generalization to extraordinary cohomology theories.
*Atiyah-Hirzebruch spectral sequence of an extraordinary 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 sequences for calculating Tor and Ext groups of modules.
*Chromatic spectral sequence for calculating the initial terms of the Adams-Novikov spectral sequence.
*Connes spectral sequences converging to the cyclic homology of an algebra.
*EHP spectral sequence converging to stable homotopy groups of spheres
*Eilenberg-Moore spectral sequence for the singular cohomology of the pullback of a fibration
*Federer spectral sequence converging to homotopy groups of a function space.
*Frölicher spectral sequence starting from the Dolbeault cohomology and converging to the algebraic de Rham cohomology of a variety.
*Green's spectral sequence for Koszul cohomology
*Grothendieck spectral sequence for composing derived functors
*Hodge-de Rham spectral sequence converging to the algebraic 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 a fibration
*Lyndon-Hochschild-Serre spectral sequence in group 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 the bar spectral sequence.
*Moore spectral sequence is another name for the bar spectral sequence.
*Quillen spectral sequence for calcuating the homotopy of a simplicial group.
*Rothenberg-Steenrod spectral sequence is another name for the bar 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


Wikimedia Foundation. 2010.

Нужна помощь с курсовой?

Look at other dictionaries:

  • Adams spectral sequence — In mathematics, the Adams spectral sequence is a spectral sequence introduced by Adams (1958). Like all spectral sequences, it is a computational tool; it relates homology theory to what is now called stable homotopy theory. It is a… …   Wikipedia

  • Serre spectral sequence — In mathematics, the Serre spectral sequence (sometimes Leray Serre spectral sequence to acknowledge earlier work of Jean Leray) is a basic tool of algebraic topology. It expresses the singular (co)homology of the total space E of a (Serre)… …   Wikipedia

  • Eilenberg-Moore spectral sequence — In mathematics, in the field of algebraic topology, the Eilenberg Moore spectral sequence addresses the calculation of the homology groups of a pullback over a fibration. The spectral sequence formulates the calculation from knowledge of the… …   Wikipedia

  • Grothendieck spectral sequence — In mathematics, in the field of homological algebra, the Grothendieck spectral sequence is a technique that allows one to compute the derived functors of the composition of two functors Gcirc F, from knowledge of the derived functors of F and G… …   Wikipedia

  • EHP spectral sequence — In mathematics, the EHP spectral sequence is a spectral sequence used for inductively calculating the homotopy groups of sphereslocalized at some prime p . It is described in more detail in harvtxt|Ravenel|2003|loc=chapter 1.5 and… …   Wikipedia

  • Lyndon–Hochschild–Serre spectral sequence — In mathematics, especially in the fields of group cohomology, homological algebra and number theory the Lyndon spectral sequence or Hochschild Serre spectral sequence is a spectral sequence relating the group cohomology of a normal subgroup N and …   Wikipedia

  • Leray spectral sequence — In mathematics, the Leray spectral sequence was a pioneering example in homological algebra, introduced in 1946 by Jean Leray. The formulation was of a spectral sequence, expressing the relationship holding in sheaf cohomology between two… …   Wikipedia

  • Atiyah–Hirzebruch spectral sequence — In mathematics, the Atiyah–Hirzebruch spectral sequence is a computational tool from homological algebra, designed to make possible the calculation of an extraordinary cohomology theory. For a CW complex X , or more general topological space, it… …   Wikipedia

  • Chromatic spectral sequence — In mathematics, the chromatic spectral sequence is a spectral sequence, introduced by Ravenel (1978), used for calculating the initial term of the Adams–Novikov spectral sequence for BP cohomology, which is in turn used for calculating the stable …   Wikipedia

  • May spectral sequence — In mathematics, the May spectral sequence is a spectral sequence, introduced by J. Peter May (1965, 1966), used for calculating the initial term of the Adams spectral sequence, which is in turn used for calculating the stable homotopy groups …   Wikipedia

Share the article and excerpts

Direct link
Do a right-click on the link above
and select “Copy Link”