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The spectral sequence of Y 3,3

whereLis the lower-triangular matrix that defines the stabilisation map, see Definition 19. Computing the determinants gives

Det(sn−1(v)) = (±v1, . . . ,±vm,±1, . . . ,±1),

with the signs dependent onnandm. Using the action of Tn to change the lastn−1 determinants as in the proof of Lemma 18, we can get an element ofYm,nwith any prescribed determinant. Altogether this defines a lift,f, of the identity map over the determinant,

Ym,n

Det

Tm+n−1

f 88

Id //Tm+n−1. By taking first cohomology, we get maps

H1(Ym,n)

f..

H1(Tm+n−1)

Det

mm ,

with

f◦Det= Id.

This shows that Det is injective andf is surjective. But by the previous theorem, f is a map between free abelian groups of the same rank, hence it must also be injective and so an isomorphism with inverse Det. This shows that the determinant map is an isomorphism on the first cohomology groups and immediately extends to the quotiented spaces, with

Det:H1(Tm+n−1/Tn)→H1(Xm,n)

an isomorphism. Note that the action of Tn on Tm+n−1 is not the obvious one, but is given by how the determinants change when Tn acts on Ym,n. The quotient is still isomorphic to Tm−1. Furthermore the stabilisation maps on degree one cohomology are surjective, since the stabilisation maps

s:Ym,nYm,n+1

change the signs of some determinants and add an extra determinant that is always plus or minus one. So if the class diH1(Ym,n+1) represents the image of moving once around zero in thei’th coordinate of Tn+1, then

s(di) =

(di 1≤in, 0 otherwise.

3.3. THE SPECTRAL SEQUENCE OFY3,3 37 The way we will calculate this is by using the spectral sequence defined in Section 3.1. Some of the calculations have been done in Sage and the relevant source code can be found in Appendix A.

The groups we need to compute for the first page in the spectral sequence are:

E1p,q ∼=









Hq(Y) p= 0,

Hq+1(Y{1}×(D, D−0))⊕Hq+1(Y{2}×(D, D−0)) p= 1, Hq+2(Y{1,2}×(D2, D2−0)) p= 2

0 otherwise.

The four spaces that appear will be handled separately.

The cohomology ofY{1,2}

Consider the spaceY{1,2}. This consists of the elements ofY3,3that have two zeroes in the last column:

Y{1,2}=

a b 0

c d 0

e f i

a6= 0, adbc6= 0 adibci6= 0

di6= 0, i6= 0

.

The space is homeomorphic to (C)3×C2×

(b, c)∈C2|bc6= 1 , with the home- omorphism given by

Y{1,2}→(C)3×C2×

(b, c)∈C2|bc6= 1

a b 0

c d 0

e f i

7→

a, d, i,e

i,f i,b

a,c d

.

We already computed the cohomology ofY ={(b, c)|bc6= 1}in Example 11, so we can calculate the cohomology ofY{1,2}:

Hq(Y{1,2}) =





















Z q= 0, Z4 q= 1, Z7 q= 2, Z7 q= 3, Z4 q= 4, Z q= 5, 0 otherwise.

Since we know the product structure from the Künneth formula, we can name the generators and get the ring

H(Y{1,2}) = Λ[a00, d00, i00]⊗H(Y).

The two generators ofY will be denotedy00,1for the degree one generator and y00,2

for the degree two generator. All other generators have degree one. The ring structure is the usual one on a tensor product, with the added relation y00,1·y00,2 = 0. The elementy00,1H1(Y) is given by the map

Y 3(b, c)7→1−bc∈C

in cohomology, since there is another map

C3λ7→(1,1−λ)∈Y

and the composition is the identity on C. ApplyingH1 shows that the two maps give isomorphisms in degree 1.

The cohomology ofY{1}

InY{1} we have the first entry of the last column equal to zero, which is the space

Y{1}=

a b 0

c d h

e f i

a6= 0, adbc6= 0 adi+behbciaf h6= 0

dif h6= 0, h6= 0, i6= 0 .

This space is homeomorphic to (C)5×C×Y:

a b 0

c d h

e f i

7→

a, i, h,d hf

i,d hbc

ah,e

i, bhi adiaf h, c

he i

.

Since the cohomology ofY is already known, applying the Künneth formula gives

Hq(Y{1}) =

































Z q= 0, Z6 q= 1, Z16 q= 2, Z25 q= 3, Z25 q= 4, Z16 q= 5, Z6 q= 6, Z q= 7, 0 otherwise.

As before, the ring structure is given by

H(Y{1}) = Λ[a01, d01, f01, h01, i01]⊗H(Y).

The cohomology ofY{2}

The space is

Y{2}=

a b g

c d 0

e f i

a6= 0, adbc6= 0 adi+cf gbcideg6= 0

di6= 0, g6= 0, i6= 0

,

which can also be identified with (C)5×C×Y using the homeomorphism

a b g

c d 0

e f i

7→

a

g, d, i, g,1 + cf g adieg

aibc ad,f

i,b a,c

d

.

3.3. THE SPECTRAL SEQUENCE OFY3,3 39 Since we already know the cohomology of this space, we know

Hq(Y{2}) = (Λ[a10, d10, f10, g10, i10]⊗H(Y))q=

































Z q= 0, Z6 q= 1, Z16 q= 2, Z25 q= 3, Z25 q= 4, Z16 q= 5, Z6 q= 6, Z q= 7, 0 otherwise.

The cohomology ofY

This space is slightly more complicated than the others. The space consists of the elements inY3,3 where all entries of the last vector are non-zero.

Y=

a b g

c d h

e f i

a6= 0, adbc6= 0, dif h6= 0, adi+beh+cf gdegbciaf h6= 0,

g6= 0, h6= 0, i6= 0

.

The space is homeomorphic to (C)7×

(x, y, z)∈C3|yzxyz= 1 , with the homeomorphism given by

a b g

c d h

e f i

7→

g, h, i,a g,f

id h, D= adbc

ah , C= c

ha

g + cdideh

f h2dhi+ behbci f ghdgi, bC

aD, c hCa

gC,D C

ehci f hdi

.

To get the cohomology, we refer back to Example 12, where we computed the cohomology of

Z =

(x, y, z)∈C3|yzxyz= 1 ,

and found it to be the same as the cohomology ofS2. The generator of H2(Z) will

be calledz11, withz211= 0. If we apply this, we get

Hq(Y) =









































Z q= 0, Z7 q= 1, Z22 q= 2, Z42 q= 3, Z56 q= 4, Z56 q= 5, Z42 q= 6, Z22 q= 7, Z7 q= 8, Z q= 9, 0 otherwise.

and the generators are

H(Y) = Λ[a11, d11, g11, h11, i11, C11, D11]⊗H(Z).

A note on the cohomology ofZ

The spaceZ defined above is a manifold, which we will prove by applying the implicit function theorem. Consider the formula defining Z,

(x, y, z)7→yzxyz−1.

Taking partial derivatives gives the three functions (x, y, z)7→yz, (x, y, z)7→1−xz, (x, y, z)7→ −1−xy.

If the first function is zero, then at least one of the two others must be non-zero.

By the implicit function theorem, the coordinate that has non-zero derivative can be written as a smooth function of the other coordinates. This shows thatZ is locally the graph of a smooth function, so it is a smooth manifold.

Later on it will be necessary to have a description of H2(Z). This is done by considering the subspace

R= (

(x, y, z)∈R3

x >0, y <0, xy <−1, z= y−1 1 +xy >0

)

Z.

This space is closed in Z since any sequence in R that converges in Z must also converge in R. Consider a subbundleN R∼=R×D of the normal bundle ofR in the tangent bundle T Z, such that the exponential map is a diffeomorphism onN R. This gives us a diagram

H2(N R, N R0)oo = H2(Z, ZR) j //H2(Z),

3.3. THE SPECTRAL SEQUENCE OFY3,3 41 whereN R0 isN Rwithout the zero section,N R0∼=R×(D−0). The isomorphism is given by excision, since Z=N R∪(ZR). The space Ris homeomorphic toR2, so we have

H2(Z, ZR)∼=H2(N R, N R0)∼=H2(R×(D, D−0))∼=Z.

From the diagram,j(1) gives us an element ofH2(Z). To see that this is a generator, consider the torus

T =b (

x, y, z= y−1 1 +xy

Z

|x|=|y|= 2 )

Z.

This intersectsRin exactly one point, namelyp= (2,−2,1). By taking the intersection withT we can extend the previous diagram,b

H2(N R, N R0)

i

H2(Z, ZR)

i

=

oo j //H2(Z)

i

H2(p×(D, D−0))oo = H2(bT,Tb−p) = //H2(bT).

The lefti is an isomorphism since the cohomology in degree two is given by the pair (D, D−0), which does not change under the inclusion. This shows that the inclusion Tb →Z is an isomorphism in cohomology, soj(1) is a generator ofH2(Z). Taking the same diagram with cohomology replaced with homology reverses all arrows but is otherwise exactly the same. This shows that to calculate the homology class of a cycle σinH2(Z), we can count the number of points of intersection betweenσand R with orientation, since each of these will contribute either 1 or−1, depending on orientation, to the homology class in (Z, ZR).

There is a smiliar argument with the space Y from before and the subspace RY =

(b, c)∈R2|b >0, c >0, bc >1 . In particular, the generator ofH2(Y) can be taken asi

[bT]

, where [T] is a generator ofb H2(T) for the torusb

T =b {(b, c)| |b|=|c|= 2} ⊂RY. The first page

With all of the above, we can draw theE1-page of the spectral sequence. Remember that this is

E1p,q ∼=









Hq(Y) p= 0,

Hq+1(Y{1}×(D, D−0))⊕Hq+1(Y{2}×(D, D−0)) p= 1, Hq+2(Y{1,2}×(D2, D2−0)) p= 2,

0 otherwise.

By inserting the groups that were calculated above into this, we get Figure 3.4 with the non-zero differentials moving directly to the right. To get theE2-page of the spectral sequence, we need to compute the homology of the differentials.

OO //

q p

9 Z 0 0

8 Z7 //Z2 0

7 Z22 //Z12 //Z 6 Z42 //Z32 //Z4 5 Z56 //Z50 //Z7 4 Z56 //Z50 //Z7 3 Z42 //Z32 //Z4 2 Z22 //Z12 //Z

1 Z7 //Z2 0

0 Z 0 0

0 1 2

Figure 3.4: TheE1-page with differentials.

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