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Tutorial 8: Holes, Tunnels and Spheres
In the last tutorial, you learned that Hypertorus Homotopy is a way to interpret Homotopy Theory using normal paths:
f[g]
Here, g is a loop around a point f.
Now, let us revisit the imaginary normal path in Tutorial 6:
concat[len x len -> id]
Using the Hypertorus Homotopy interpretation, len x len -> id is a loop around a point concat.
However, since this normal path has no solution, the loop around the point is not contractible.
This means, that the loop defines a hole.
Just like points, two holes can have a homotopy, for example:
concat[(id . len) x (id . len) -> id] <=> concat[len x len -> id]
In physics of space-time, this corresponds to a wormhole.
Reasoning about holes can also be used for toruses:
f[g[h]]
Here, f is a point, g is a loop and h is a torus.
When g[h] has no solution, the loop g hollows out the torus h.
A strange thing is that f[g[h]] can have a solution, even though g[h] has no solution.
This is because f can be an imaginary normal path.
When f[g[h]] has a solution while g[h] does not have a solution, the hollow torus might be thought of as a tunnel loop.
Two hollow toruses can have a homotopy:
f1[g1[h1]] <=> f2[g2[h3]]
A more complex example: Spheres are holes with loops that can be contracted to a point:
f[g1][g2]
Here, f[g1] has no solution, which creates a hole.
The loop g2 closes the hole such that it can be contracted to a point and hence form a sphere.
In the example used before:
∵ concat[len x len -> id][id x id -> len]
∴ concat[(id . len) x (id . len) -> (len . id)]
∴ concat[len x len -> len]
∴ concat[len]
∴ add
Here, concat[len x len -> id][id x id -> len] is a sphere.
At first, it might seem counter-intuitive that a sphere can behave like a point. However, from a topological perspective, when one can only contract paths in some space to check for holes, a sphere might be indistinguishable from a point.
A sphere can be continuously transformed into a point. The transformation of the sphere into a point is a homotopy.
In summary: One can reason about holes and other similar objects such as tunnels and spheres using normal paths in the same way one can reason about points.