06-1350/Class Notes for Tuesday September 12: Difference between revisions
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===Introduction=== |
===Introduction=== |
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We wish to define a <i>knot</i> as a continuous injective map from the circle to 3-dimensional Euclidean space |
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up to continuous homotopy. |
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Unfortunately this definition doesn’t quite work as most of the knots that we wish to |
Unfortunately this definition doesn’t quite work as most of the knots that we wish to |
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distinguish will actually be equivalent (we may shrink down the knotted part to a point). For this |
distinguish will actually be equivalent (we may shrink down the knotted part to a point). For this |
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R1: top left, R2: top right, R3: bottom middle |
R1: top left, R2: top right, R3: bottom middle |
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</center> |
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<br> |
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===3 Colouring=== |
===3 Colouring=== |
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Revision as of 16:48, 19 September 2006
Introduction
We wish to define a knot as a continuous injective map from the circle to 3-dimensional Euclidean space
up to continuous homotopy.
Unfortunately this definition doesn’t quite work as most of the knots that we wish to
distinguish will actually be equivalent (we may shrink down the knotted part to a point). For this
reason, we replace continuous with smooth or piecewise linear (this time we may not shrink down
the knotted part to the point as we will get a singularity). We will not discuss this in detail, but
rather state the results:
Every knot can be represented by a finite diagram, e.g.
http://katlas.math.toronto.edu/drorbn/images/e/e1/Trifoil.png
Two such diagrams represent the same knot if they differ by a sequence of
Reidemeister moves. When we draw diagrams, we often don’t draw the entire knot,
only the parts which are to be changed.
An invariant is a map from diagrams to say formal power series Z((q)) which respects R1 - R3. Thus, the invariant descends to equivalence classes of diagrams, i.e to knots.
http://katlas.math.toronto.edu/drorbn/images/8/8a/Reid.png
R1: top left, R2: top right, R3: bottom middle
3 Colouring
We give an example of an invariant. Define I3 : {diagrams}→{true, false},
I3 is true
whenever its arcs may be coloured with red, green, blue (RGB), such that all colours appear and
at every crossing is mono or tri-chromatic.
We can now distinguish the trifoil from the unknot as the trifoil is 3-colourable while the
unknot is not. However, we cannot distinguish (yet) the trifoil from its mirror image, so later we
will look for more powerful invariants.
http://katlas.math.toronto.edu/drorbn/images/9/93/Trifoil2.png
We now prove that I3 is an invariant, that is we need to show that I3 is preserved after R1, R2 and R3. The test for R1 is straight forward:
http://katlas.math.toronto.edu/drorbn/images/2/25/3col-a.png
For R2, we have two possibilities. The second case for R2 requires further consideration: where did the green go? Here, we
remember that we are only drawing part of the diagram. Since the red and blue branches must
meet, at such a crossing, green will appear.
Showing that invariance under R3 is more tedious (and is left as an exercise).
Jones Polynomial
The simplest way to define the Jones polynomial is via the Kauffman bracket. The idea is to
eliminate all crossings using the rule:
http://katlas.math.toronto.edu/drorbn/images/6/64/Kauffman.png
In the right hand side, the first bracket is called the 0-smoothing and the second
is called the 1-smoothing. To calculate the Kauffman bracket we must sum over all
possible smoothings. For instance, for the trifoil, we 23 = 8 summands, one of which will
be:
http://katlas.math.toronto.edu/drorbn/images/8/8b/Trifoil-smoothing.png
Each summand will have no crossing and thus will be a union of (possibly nested) unknots.
We define the bracket polynomial of k unknots to be dk-1 for some indeterminate d. Our hopes
that our polynomial in ℤ[d,A,B] will be an invariant under the Reidmeister moves. We first
verify R2.
http://katlas.math.toronto.edu/drorbn/images/c/cd/Jones-r2.png
Collecting like terms and comparing we find AB = 1 and A2 + B2 + dAB = 0. Thus, we must
have B = A-1 and d = -(A2 + A2). Things are looking bad, we still have two moves to verify
and we already lost two of our variables.
We now verify R3. For this we remark that
http://katlas.math.toronto.edu/drorbn/images/f/fb/Jones-r3.png
The two diagrams with coefficients B coincide; and the diagrams with coefficients A differ by
two R2 moves. Now we verify R1:
http://katlas.math.toronto.edu/drorbn/images/9/99/Jones-r1.png
The right hand side evaluates to A + A-1(-A2 -A-2) = -A3 of the desired. This is
unfortunate. One could salvage something by taking A to be one of the cube roots of -1;
however, the right way out of this is to define another invariant which fails in the exactly the
same way, and multiply it with the bracket polynomial.
Writhe
The invariant we are looking for is called the writhe. If D is a diagram of an oriented knot, we
define
http://katlas.math.toronto.edu/drorbn/images/8/88/Mathtext1.png
We choose +1 if the crossing is positive (the overpass goes over the underpass from left to right) and -1 if the crossing is negative (otherwise):
"http://katlas.math.toronto.edu/drorbn/images/3/38/Crossings.png
Lets have an example. Notice that the orientation of the knot is actually irrelevant.
http://katlas.math.toronto.edu/drorbn/images/c/c5/Writhe-example.png
We now show that the writhe is also invariant under R2 and R3, under R1 we gain ±1
depending which way we apply it. In R2, the two crossings have opposite signs; and in R3, the
diagonal crossing doesn’t change sign and the other two are reversed.
http://katlas.math.toronto.edu/drorbn/images/f/f9/Writhe-reid.png
It follows that 〈D〉⋅(-A-3)w(d) is a knot invariant. This is a polynomial in A, we now substitute q http://katlas.math.toronto.edu/drorbn/images/2/23/Mathtext2.png for A and call this the Jones polynomial (which strictly speaking, is not really a polynomial).