On 14 Jan 2014, at 22:04, LizR wrote:

Sorry, I realise that last sentence could be misconstrued by someone who's being very nitpicky and looking for irrelevant loopholes to argue about, so let's try again.

Now how about discussing what I've actually claimed, that the time symmetry of fundamental physics could account for the results obtained in EPR experiments?

Logically, yes.

But you need "hyper-determinism", that is you need to select very special boundary conditions, which makes Cramer's transaction theory close to Bohm's theory.

Those are still many-world theories, + some "ugly" selection principle to get one branch. It is very not "natural", as you have quasi microsuperposition (appearance of many branches), but the macro-one are eliminated by ad hoc boundary conditions, which will differ depending on where you will decide to introduce the Heisenberg cut. Also, QM will prevent us to know or measure those boundary conditions, which makes them into (local, perhaps, in *some* sense) hidden variable theory.

Many worlds is far less ad-hoc, imo. There is no Heisenberg cut, and the boundary conditions does not play any special role, and indeed they are all realized in the universal wave (and in arithmetic).

Bruno






On 15 January 2014 10:01, LizR <lizj...@gmail.com> wrote:
On 15 January 2014 06:11, John Clark <johnkcl...@gmail.com> wrote:
On Sun, Jan 12, 2014 at 6:41 PM, LizR <lizj...@gmail.com> wrote:

>>> "Retro-causality" (time symmetry is a better term) only exists at the quantum level.

>> Why? Where is the dividing line? And with a Schrodinger's Cat type device a quantum event can easily be magnified to a macro-event as large as desired, you could connect it up to an H-bomb.

> The dividing line appears to be roughly where decoherence occurs. Basically anything above a single quantum entity engaged in a carefully controlled interaction is liable to get its time symmetric properties washed out by interactions with other particles

The nucleus of an atom is tiny even by atomic standards so it is certainly at the quantum level, and in its natural state of existing inside a huge chunk of irregular gyrating matter this tiny thing is constantly subject to the slings and arrows of outrageous fortune from an astronomical number of other clumsy atoms; and yet the half life of Bismuth 209 is 1.9 * 10^19 years. Why?

Because that's how long it takes for the relevant particles to get over the potential barrier. But this is irrelevant. Atomic nuclei are (probably) already on the wrong side of the "entropy fence" in any case. They're bound states which can only occur under certain special cirumstances, namely when the universe expands and cools enough to allow them to form. And atomic nuclei haven't been used to violate Bell's inequality as far as I know.


>> It's just a fact, if time were symmetrical then you'd be just as good at predicting the future as you are at remembering the past, so you'd know the outcome of an experiment before you performed it just as well as you remember setting up the apparatus. But this is not the way things are because the second law exists. And the second law exists because of low entropy initial conditions. And I don't know why there were low entropy initial conditions.

> OK. So the above statement of yours about predicting the future is still false,

Yes it's false, I don't think this will come as a great news flash but the truth is we're not as good at predicting the future as we are at remembering the past. And the reason we're not is that time is not symmetrical.

Except below the level of coarse graining at which entropy operates, that is correct. And I never claimed otherwise. As I keep saying, I'm only claiming this is relevant in special circumstances like EPR experiments.

> To recap briefly -- the laws of physics are time symmetrical,

Yes, the fundamental laws of physics, the ones we know anyway, seem to be time symmetrical. But that doesn't mean that time is symmetrical.

...is just words. Stop nitpicking. If the laws of physics are time symmetrical, that has a potential influence on EPR experiments.

> and most particle interactions are constrained by boundary conditions.

Yes, and that is why time is NOT symmetrical.

Stop playing with words. The time symmetry of fundamental physics is there, so it's perfectly valid to say time is symmetrical below the level of coarse graining needed to derive the 2nd law, and asymmetrical above it. (That's virtually a simple restatement of Boltzmann's H-theorem "for dummies".) The point is that symmetrical time may become apparent in EPR setups. You haven't yet given even a suggestion of a reason why it wouldn't, just a load of hand waving about stuff that is IRRELEVANT to EPR experiments, which are carefully prepared to avoid all the influences you've mentioned.

Now how about discussing what I've actually claimed, that time symmetry of physics could account for the special situation which has to be created to obtain EPR results?



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