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Second Draft (with algebra dimensional analysis corrections)

On Jan 25, 2015, at 9:12 AM, JACK SARFATTI <This email address is being protected from spambots. You need JavaScript enabled to view it.> wrote:

alpha = 2/3 comes most simply from
 
A/Lp^2 = A^3/2/(&L)^3
 
for a 2D horizon hologram screen of area A with quantum bit pixel area Lp^2
 
the bulk 3D hologram voxels have quantum volumes (&L)^3
 
However, if the horizon 2D screen is fractal with linear scale parameter y and the interior bulk is fractal with linear scale parameter x
 
A^(1 + y)/Lp^2(1 + y) = A^(3/2)(1 + x)/(&L)^3(1 + x)
 
(&L)^3(1 + x) = Lp^2(1 + y)A^3/2(1 + x)/A^(1 + y)
 
A^3/2(1 + x)/A^(1 + y) = A^3/2 A^3x/2/AA^y = A^1/2 A^(3x/2 - y)
 
(&L)  = [Lp^2A^1/2]^(1/3(1 + x) [Lp^2y A^(3/2x - y)]^1/3(1 + x)]
 
alpha = (2/3)(1 + y)/(1 + x)
 
Lp^2y A^(3/2x - y)]^1/3(1 + x)  is not a dimensionless pure number
 
If we use the non-fractal measures, it's no longer true that
 
A/Lp^2 = A^3/2/(&L)^3
 
that is the effective hologram mapping from screen to image is no longer 1 - 1 
 
this corresponds to a non-unitary S-Matrix I suspect.
 
to be continued
 
 
 
 
 
 
 
 
 
 
 
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