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Jee, you are chatty today :rofl: I will be brief since it is bed time over here and I shall only react upon the points where I disagree
just because I am a grumpy person.
(a) A semantic issue about the incompatibility of QM and GR: I guess we both agree upon what it means but we disagree upon the formulation. So, lets quit that one, it is getting boring.
(b) How to reach QG? My point of view is very clear: we have NO experimental guideline whatsoever (at least Einstein did have some indications for GR) so we are entirely lost. The good way to proceed in this case then is to radically sacrifice one of both theories and build upon the other one, i.e. see how far one theory ``deviates´´ from the other.
(1) LQG, STRT and CDT builds upon QM and it is far from sure that they get out GR in the classical limit.
(2) Local realism starts from GR and has to get out microscopic physics (note: this is NOT necessarily equal to QM).
Approach (1) has a long very active history and according to me, a key problem on the road there is the measurement (or micro - macro) problem in QM with the bourlesque name: Schroedinger's cat. This problem is especially important since I want to know how the macroworld, with its local realism can be understood to emerge from a microscopic world with an operational ontology. IMO, this problem is unsolvable within contemporary QM and little or no progress has been made in this field.
Penrose OR proposal is one of the more intelligent proposals I have heard concerning this problem. So (1) has a really bad record if you remember my list of four laws.
Now (2) is not experimentally falsified and it is really a mystery for me why people have not put more effort into this:
(a) there are no ontological problems whatsoever (so the approach is self consistent)
(b) spacetime locality and covariance are the MOST simplifying principles to construct a theory
(c) There EXIST already results which reasonably indicate that local realism (LR) can reproduce quantum mechanical results (think about stochastic electrodynamics and the Barut self field approach)
...
The reason why (2) is unpopular I guess is because it sacrifies QM (which is outcasting GR). Moreover, the deliberate misinformation about Bell test results is not really contributing to an honest evaluation (I have still some unfinished business on the QM forum). So, the best you can reasonably do is propose concrete test models and TEST them
That is actually Einsteins methodology which has proven to be highly succesful.
So, I am not contradicting myself here: the first *logical* step is to choose radically for one theory and option (2) is leading much faster to experimental falsification. Actually, this is the big *advantage* of (2) : we have pleanty of experimental results to test against: check out any book on quantum chemistry. Then, when it would turn out that (2) is reasonably not possible (which would require testing lots of continuum models for elementary particles and so on), *then* we might think about CAREFULLY abandonning spacetime locality (and not that wild as happens in QM). Next, if we would find such deviation which is in concordance with all experimental results, THEN we could try to derive this theory from basic new physical principles. This seems to me the road to succes.
** Haven't you already made an assumption that you can not be sure of?
I surely would not want to INcrease them. **
Sure, but now you should think of other models available on the market and do the (rough) counting there (you shall see there is no substantial deviation). You must admit that it is a fair way to get a rough estimate (and that is all I wanted to provide).
Your Nestle and wheel analogies can be easily answered but that will have to wait. It is nice talking to you too
Cheers,
Careful
(a) A semantic issue about the incompatibility of QM and GR: I guess we both agree upon what it means but we disagree upon the formulation. So, lets quit that one, it is getting boring.
(b) How to reach QG? My point of view is very clear: we have NO experimental guideline whatsoever (at least Einstein did have some indications for GR) so we are entirely lost. The good way to proceed in this case then is to radically sacrifice one of both theories and build upon the other one, i.e. see how far one theory ``deviates´´ from the other.
(1) LQG, STRT and CDT builds upon QM and it is far from sure that they get out GR in the classical limit.
(2) Local realism starts from GR and has to get out microscopic physics (note: this is NOT necessarily equal to QM).
Approach (1) has a long very active history and according to me, a key problem on the road there is the measurement (or micro - macro) problem in QM with the bourlesque name: Schroedinger's cat. This problem is especially important since I want to know how the macroworld, with its local realism can be understood to emerge from a microscopic world with an operational ontology. IMO, this problem is unsolvable within contemporary QM and little or no progress has been made in this field.
Penrose OR proposal is one of the more intelligent proposals I have heard concerning this problem. So (1) has a really bad record if you remember my list of four laws.
Now (2) is not experimentally falsified and it is really a mystery for me why people have not put more effort into this:
(a) there are no ontological problems whatsoever (so the approach is self consistent)
(b) spacetime locality and covariance are the MOST simplifying principles to construct a theory
(c) There EXIST already results which reasonably indicate that local realism (LR) can reproduce quantum mechanical results (think about stochastic electrodynamics and the Barut self field approach)
...
The reason why (2) is unpopular I guess is because it sacrifies QM (which is outcasting GR). Moreover, the deliberate misinformation about Bell test results is not really contributing to an honest evaluation (I have still some unfinished business on the QM forum). So, the best you can reasonably do is propose concrete test models and TEST them
So, I am not contradicting myself here: the first *logical* step is to choose radically for one theory and option (2) is leading much faster to experimental falsification. Actually, this is the big *advantage* of (2) : we have pleanty of experimental results to test against: check out any book on quantum chemistry. Then, when it would turn out that (2) is reasonably not possible (which would require testing lots of continuum models for elementary particles and so on), *then* we might think about CAREFULLY abandonning spacetime locality (and not that wild as happens in QM). Next, if we would find such deviation which is in concordance with all experimental results, THEN we could try to derive this theory from basic new physical principles. This seems to me the road to succes.
** Haven't you already made an assumption that you can not be sure of?
I surely would not want to INcrease them. **
Sure, but now you should think of other models available on the market and do the (rough) counting there (you shall see there is no substantial deviation). You must admit that it is a fair way to get a rough estimate (and that is all I wanted to provide).
Your Nestle and wheel analogies can be easily answered but that will have to wait. It is nice talking to you too
Cheers,
Careful
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