Calculating the Z2 cohomology of the Klein Bottle using intersections

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In summary, the Klein bottle has a 1 dimensional Z2 cohomology class that is not the first Stiefel Whitney class.
  • #1
lavinia
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This thread asks for help calculating the Z2 cohomology ring of the Klein bottle using intersections.

This is what I think.

View the Klein bottle as a circle bundle over a circle. A fiber circle and the base circle generate the first Z2 cohomology by transverse intersection.

- The fiber cicle has zero transverse intersection with itself and intersects the base circle in a single point. This would appear to be the first Stiefel Whitney class of the tangent bundle. Since itself intersection is zero the cup product of the cohomology class that it determines with itself is zero. This seems right since the Euler characteristic of the Klein bottle is zero.

- the base circle intersects both itself and the fiber circle in a single point. so its square under the cup product is not zero.

This completely describes the cohomology ring in dimension 1.

What about the pull back of these classes under the two fold cover of the Klein bottle by a torus?

- the fiber circle class now intersects the base twice as so pulls back to zero. This makes sense because the torus is orientable so its first Stiefel Whitney class is zero.

- the base circle intersects itself twice and so has zero self intersection mod 2 - so itself cup product is now zero - but still intersects the fiber circle once. So it pulls back to one of the generators of the first cohomology of the torus.

I think this right.
 
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  • #2
whats the idea here lavinia? you know the Z/2 homology and assume that poincare duality holds mod 2, so you want to find dual cocycles to the generating cycles?
 
  • #3
Mathwonk

I was interested in computing the cohomolgy ring of the Klein bottle - not just its cohomology - using transverse circles on the boundary of its fundamental domain.

I wanted to find the first Stiefel-Whitney class and see why its square is zero and was surprised that there seems to be a 1 dimensional class whose square is not zero but which is not induced from the classifying map into projective space. I just thought I may have done it wrong and wanted to make sure.

But there is a broader idea. Can one compute the Z2 cohomology ring of a flat manifold of higher dimension using the same technique, intersection of hyperplanes on the boundary of a fundamental domain.? Are there cohomology classes that can not be obtained in this way? A priori without any other knowledge this could even be true of the Klein bottle so how does one see this?

I was hoping that for more complicated flat manifold this technique could also be used to compute the Z2 characteristic algebra and maybe to find a manifold whose fundamental Z2 cohomology class is actually in induced from the classifying map into the holonomy group.

The amazing thing to me about the Klein bottle is that its Z2 fundamental cocycle is the square of a 1 dimensional class but not the square of a class in its characteristic algebra (since the square of its 1st Stiefel Whitney class is zero).

I have started trying out some simple 3 manifolds such as two way Klein bottle - a half twist along both the y and z axes. The same sort of thing happens here but now that manifold is orientable so the 1 dimensional cohomology class induced by the classifying map into projective space is not the first Stiefel Whitney class.
 
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  • #4
Mathwonk

I have read you explanations of ramified covers in another thread and wonder whether a 2 fold ramified cover of the sphere by the torus can be set up to project to a 2 fold ramified cover of the projective plane by the Klein bottle.

This might be the classifying map of the tangent bundle.
 
  • #5


Your approach is correct. The key idea is to view the Klein bottle as a circle bundle over a circle, which allows us to use intersection theory to calculate its cohomology ring. As you mentioned, the first cohomology class is generated by the intersection of the fiber circle and the base circle, which has a coefficient of 1 since it intersects once.

The second cohomology class is generated by the intersection of the base circle with itself, which has a coefficient of 2 since it intersects twice. However, when we take mod 2 coefficients, this becomes 0 since 2 is equivalent to 0 mod 2. This is consistent with the fact that the Euler characteristic of the Klein bottle is 0.

When we pull back these classes under the two-fold cover of the Klein bottle by a torus, we see that the first cohomology class (generated by the intersection of the fiber circle and the base circle) becomes 0 since the fiber circle now intersects the base circle twice. This is again consistent with the fact that the torus is orientable and has a first Stiefel-Whitney class of 0.

The second cohomology class (generated by the intersection of the base circle with itself) now becomes 1 since it still intersects itself twice, but intersects the fiber circle once. This pulls back to one of the generators of the first cohomology of the torus, as you mentioned.

Overall, your approach using intersection theory is a valid and efficient way to calculate the Z2 cohomology of the Klein bottle. Well done!
 

1. What is the definition of Z2 cohomology?

Z2 cohomology is a mathematical concept used in algebraic topology to study geometric objects. It measures the topological properties of a space by assigning algebraic structures to its subspaces.

2. How is Z2 cohomology calculated?

Z2 cohomology is calculated using a mathematical tool called cohomology groups. These groups are constructed by taking the quotient of the space's chain groups by its boundary groups, and then forming a sequence of higher-order groups based on the intersections of these groups.

3. What is the Klein Bottle?

The Klein Bottle is a non-orientable surface in topology. It is a closed, non-orientable surface with no boundary. It is similar to a Mobius strip, but with an added twist in the other direction.

4. How are intersections used in calculating the Z2 cohomology of the Klein Bottle?

In calculating the Z2 cohomology of the Klein Bottle, intersections are used to determine the relationships between the subspaces of the Klein Bottle. These intersections help to define the chain groups and boundary groups, which are then used to calculate the cohomology groups.

5. What are the applications of calculating the Z2 cohomology of the Klein Bottle?

The Z2 cohomology of the Klein Bottle has applications in various fields, including topology, geometry, and physics. It can be used to study the topological properties of the Klein Bottle and to understand its relationship with other surfaces. It also has implications in understanding the behavior of certain physical systems, such as fluid dynamics and quantum mechanics.

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