Petr Horava and the quantum gravity model

http://www.scientificamerican.com/article/splitting-time-from-space/

Physicists have struggled to marry quantum mechanics with gravity for decades. In contrast, the other forces of nature have obediently fallen into line. For instance, the electromagnetic force can be described quantum-mechanically by the motion of photons. Try and work out the gravitational force between two objects in terms of a quantum graviton, however, and you quickly run into trouble—the answer to every calculation is infinity. But now Petr Hořava, a physicist at the University of California, Berkeley, thinks he understands the problem. It’s all, he says, a matter of time.

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Gia Dvali, a quantum gravity expert at CERN, remains cautious. A few years ago he tried a similar trick, breaking apart space and time in an attempt to explain dark energy. But he abandoned his model because it allowed information to be communicated faster than the speed of light.

OK, this idea that a change in the quant rate for gravity travels fast than light. Cannot happen in the complete sequence, everything is at maximum entropy, and ordered. This effect always appears when one does not have the complete sequence, it is not a fault of quantum gravity, it is the fault of not having the complete sequence over which phase is minimized.

How do we model a change in quantization ratio in the complete sequence? The orbital parameters of the gravity packed nulls change, all packed nulls can move when free phase applies an offset by exchanging with nulls. Gravity nulls move, they ave associated wave numbers which may move. In the hyperbolic notation, these movements should always be standing waves, but when you have an incomplete sequence, you can approximate the travelling wave, which we do all the time with Maxwell equations.

Nothing wrong with a change in quantization ratio, as long as phase is conserved in your complete sequence.

Same problem solved as with quantum entanglement. Packed Nulls have an associated standing phase wave. If we had the complete sequence for separated particles, we would discover that phase is conserved, and each particle carries the inverse half phase of the other particle, which they gained at the source by conserving phase.