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And indeed the only thing that will be unique about the particular history that our universe has had will be that it is the one we have experienced.
One might have thought that states obtained from slices at different angles would inevitably be consistent only with different sets of underlying rules.
But if the underlying rules for the network preserve planarity then each of these pieces of non-planarity must on their own be persistent—and can in a sense only disappear through processes like annihilating with each other.
And one immediate feature of causal networks that differs from space networks is that their connections go only one way.
And ultimately the only reliable way to make contact will probably be to set up rather complete and realistic models of experiments—then gradually to see how limits and idealizations of these manage to match what is expected from the standard formalism.
But if the only things we have are particles, then to find out something about a given particle we inevitably have to have some other particle—say a photon of light—explicitly interact with it.
Indeed, beyond block frequencies, the only other ones that are common are those based on correlations, spectra, and occasionally run lengths—all of which we already discussed earlier in this chapter .
So what this means is that regardless of what kind of data one is storing, it takes only a very simple program to set up a hashing scheme that lets one retrieve pieces of data very efficiently.
Then when the stripe hits the first element in the sequence that exists at that step, it is allowed to pass only if the element is black.
Yet as of now we only know for certain about fairly few systems that are universal, albeit including ones like rule 110 that have remarkably simple rules.