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a(n) = ceiling(g) where g satisfies (2^n + 1 - 2*floor(2^(n/2)) - 2 + 2*g - ()/2^n - 1) = 0.
Ceiling[Flatten[Table[N[Flatten[g /. Solve[2*Floor[2^(n/2)] - 2 + 2*g - (2^n - 1) == 0, g]]], {n, 1, 32}]]]
nonn,easy,less,changed
Edited by Michel Marcus and Joerg Arndt, Aug 07 2020
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(PARI) a(n) = ceil((2^n + 1 - 2*floor(2^(n/2)))/2); \\ Michel Marcus, Aug 07 2020
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Maximum genus of fixed edge 2^m-1 binary state graph with 2*m+1 states: Vertices(n)=Floor[2^(n/2)]; Faces(n)=Floor[2^[m-n/2]; Edges(n)=Vertices(n)+Faces(n)-2+2*g=2^m-1; solved for g at the central point m.
a(n) = ceiling(g) where g satisfies 2*floor(2^(n/2)) - 2 + 2*g - (2^n - 1) = 0.
nonn,uned,less,changed
The idea was to get a binary graph system of vertices, edges and faces that had a genus near the exceptional group sequence dimension. It is a form of combinatorial optimization. The object was to get an idea of what higher dimensional exceptional group dimensions would look like if they existed.
a(n) =Ceiling[Flatten[Table[N[Flatten[g /. Solve[2*Floor[2^(n/2)] - 2 + 2*g - (2^n - 1) == 0, g]]], {n, 1, 32}]]]
Exceptional group dimension to output:
14->12->G2
24 ->25->A4
52 ->54->F4
133->113->E7
248->235->E8
484->481->E9
(?)->980->E10
Example 21 state system 2^10:
a = Table[Flatten[{n/20, N[Flatten[g /. Solve[v[n] + f[n] - 2 + 2*g - 1023 == 0, g]]/480.5]}], {n, 0, 20}];
ListPlot[a, PlotJoined -> True]
The normalized to one Plot has the form of dimension for a multifractal system.
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