Thanks for the positive assessment. I am not sure what words I misspelled.
The point of looking at AdS spacetimes is to argue that what I did with black holes carries over to general spacetimes such as cosmologies. This is rather much a work in progress. What the open world might mean is that two cosmologies with entangled states can swap them. In other words maybe in one with a bipartite entanglement plus extra state and the other with a tripartite entanglelent can swap these. This would give the local appearance of the violation of quantum monogamy.
To show entanglement conservation suppose we have two quantum states |ψ> and |ψ'> and that we have
|ψ> = a|+> + b|->
|ψ'> = c|+'> + d|-'>.
Now suppose there is a unitary operator such that
U(|ψ> + |ψ'>) = ad|+>|-'> + bc|->|+'>,
This is then a singlet state |χ> = |ψ> + |ψ'>, with assumed normalization etc. Now we have a|+> + b|-> = |+_z> and c|+> + d|-> = |+'_z>. This means
U(|ψ> + |ψ'>) = |+_z>|+'_z>.
This runs into a problem, for we have a sort of cloning of states here for with normalization if |ψ> = |ψ'> then |χ> = |ψ> and we can with this operation clone states.
Unitary operations can't create or destroy entanglements. Entanglements have symmetries and these serve as conservation laws that conserve them. They can diffuse of course. Two states that are completely entangled with another state not entangled can evolve into partial entanglements between the three. That can happen by unitary evolution.
Read the post I wrote to S. Gupta. I give more of an idea what this means. There is a duality of some kind with the unitary principle and equivalence principle. This stems from the breakdown of predictability in this open world.