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Kerrmodulationentanglementsignal.pdf

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Can we modulate the entanglement signal from the outputs of a nonlinear Mach-Zehnder interferometer by sticking in a Kerr cell in one of the outputs that will control a phase difference in the other output?
Submitted On:
29 Jun 2012
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WheelerFeynmanITfromQBITv1.pdf

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The Galois Solvable Fourth Roots of Reality Wheeler-Feynman Spinor Qubits Cause Einstein’s Gravitational Field Spin Network Pre-Geometry for Dummies Jack Sarfatti[1] Abstract Local observers are defined by orthonormal “non-holonomic” (aka “non-coordinate”) tetrad gravity fields (Cartan’s “moving frames”). The tetrads are spin 1 vector fields under the 6-parameter homogeneous Lorentz group SO1,3 of Einstein’s 1905 special relativity. You can think of the tetrad gravity fields as the square roots of Einstein’s 1916 spin 2 metric tensor gravity fields. We will see that we must also allow for spin 0 and spin 1 gravity because the spin 1 tetrads, in turn, are Einstein-Podolsky-Rosen entangled quantum states of pairs of 2-component Penrose-Rindler qubits in the quantum pre-geometry. The Wheeler-Feynman qubits are the square roots of the advanced and retarded null tetrads and can therefore be called the Galois solva...
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29 Jun 2012
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