Here the details of the iguanodon series. Start with the Farey sequence
F(1) = {0โ1, 1โ1}
F(2) = {0โ1, 1โ2, 1โ1}
F(3) = {0โ1, 1โ3, 1โ2, 2โ3, 1โ1}
F(4) = {0โ1, 1โ4, 1โ3, 1โ2, 2โ3, 3โ4, 1โ1}
F(5) = {0โ1, 1โ5, 1โ4, 1โ3, 2โ5, 1โ2, 3โ5, 2โ3, 3โ4, 4โ5, 1โ1}
F(6) = {0โ1, 1โ6, 1โ5, 1โ4, 1โ3, 2โ5, 1โ2, 3โ5, 2โ3, 3โ4, 4โ5, 5โ6, 1โ1}
F(7) = {0โ1, 1โ7, 1โ6, 1โ5, 1โ4, 2โ7, 1โ3, 2โ5, 3โ7, 1โ2, 4โ7, 3โ5, 2โ3, 5โ7, 3โ4, 4โ5, 5โ6, 6โ7, 1โ1}
F(8) = {0โ1, 1โ8, 1โ7, 1โ6, 1โ5, 1โ4, 2โ7, 1โ3, 3โ8, 2โ5, 3โ7, 1โ2, 4โ7, 3โ5, 5โ8, 2โ3, 5โ7, 3โ4, 4โ5, 5โ6, 6โ7, 7โ8, 1โ1}
Farey sequences have plenty of mysterious properties. For example, in 1924 J. Franel and Edmund Landau proved that an asymptotic density result about Farey sequences is equivalent to the Riemann hypothesis.
More precisely, let a(n) be the number of terms in the Farey sequence F(n) (that is, a(1)=2,a(2)=3,โฆ,a(8)=23 etc. This is sequence A005728 in the online integer sequences catalog).
Let
For every
when n goes to infinity. Anyway, let us continue our construction. Farey sequences are clearly symmetric around 1/2 so let us just take half of them, so we jump to 1 when we have reached 1/2. Let us extend this halved Farey on both sides with
Now consider the Farey code in which we identify the two sides connected to
[tex]\xymatrix{f(n)_i \ar@{-}[r]_{\bullet} & f(n)_{i+1}}[/tex]
That is, the Farey code associated to the modified sequence f(3) is
[tex]\xymatrix{\infty \ar@{-}[r]_{1} & 0 \ar@{-}[r]_{\bullet} & \frac{1}{3} \ar@{-}[r]_{\bullet} & \frac{1}{2} \ar@{-}[r]_{\bullet} & 1 \ar@{-}[r]_{1} & \infty}[/tex]
Recall from earlier that to a Farey-code we can associate a special polygon by first taking the hyperbolic convex hull of all the terms in the sequence (the region bounded by the vertical lines and the bottom red circles in the picture on the left) and adding to it for each odd interval [tex]\xymatrix{f(n)_i \ar@{-}[r]_{\bullet} & f(n)_{i+1}}[/tex] the triangle just outside the convex hull consisting of two odd edges in the Dedekind tessellation (then we obtain the region bounded by the black geodesics for the sequence f(3)).
Next, we can associate to this special polygon a cuboid tree diagram by considering all even and odd vertices on the boundary (which are tinted red, respectively blue) together with all odd vertices in the interior of the special polygon. These are indicated in the left picture below. If we connect these vertices with the geodesics in the polygon we get a cuboid tree diagram. The obtained cuboid tree diagram is depicted on the right below.
Finally, identifying the red points (as they lie on geodesics connected to
and a verification with GAP tells us that this group is the sporadic Mathieu group
the following dissection of the Iguanodon may prove useful
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