On 3/22/2022 7:55 PM, Bruce Kellett wrote:
On Wed, Mar 23, 2022 at 1:35 PM Brent Meeker <meekerbr...@gmail.com>
wrote:
On 3/22/2022 6:11 PM, Bruce Kellett wrote:
On Wed, Mar 23, 2022 at 10:26 AM smitra <smi...@zonnet.nl> wrote:
Let's consider this whole non-locality issue right from the
start.
Probably a good idea. The discussion has become rather confused.
We should sort out exactly where we agree and where we disagree.
In my explication, I just assumed Alice and Bob are light-hours
apart so they can set the polarizers and run the whole experiment,
including recording the N results while still spacelike.
Actually, that is where I started. I assumed that Alice and Bob were
both able to collect results from N trials before they met. Then there
are 2^N copies of each experimenter, and a potential (2^N)^(2^N) pairs
when they meet. The trouble to be explained is that there are actually
only 2^N pairs in a real experiment, each with inequality-violating
correlations. What has happened to all the extra pairings that MWI
must produce? (Most of which have correlations violating the quantum
predictions.)
Don't you mean (2^N)x(2^N). Here's the cases for N=4
There are 16 different Alices and Bobs per MWI and the array shows the
number of agreements in their notebooks when they meet. It's symmetric
so I've only shown half.
Brent
Bruce
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