David Bohm, of Bohmian mechanics fame, believed otherwise.
I know Bohm well enough to tell you that he never believed in "accidental relativity". He BELIEVED in (what he called) a "field" theory of "unbroken whole" which (when formulated) contains relativity and quantum theory. His notion of "implicate order" does not mesh well with any "accidental" symmetry.
"On the meaning of non-Lorentz invariance of processes involving individual beables". The index lists page 292 for "preferred frame" and page 290 for "Lorentz ether" which reads on my comments on the Lorentz Ether Theory directly.
Bohm spent the last 30 years of his life (at Birkbeck college) trying to formulate his "field" theory. He experimented with many, but never found the appropriate mathematical system for his (philosophical) concepts.
This is the reason for the "speculative" material of the last 4 chapters of his book with Hiley.
What Bohm & Hiley said in chapter 12, regarding QM versus relativity,is the following:
IF QM does not break down at some fundamental level, and IF a metric tensor field CAN BE defined on such level, then a LARGE quantum fluctuations could prevent this metric from having diagonal form, i.e. spacetime may cease to be Minkowskian and Lorentz group ceases to be fundamental.
Now, it is equally possible that it is the QM that breaks down at such level. In this case, Lorentz symmetry may continue to be fundamental.
I believe, the book discusses this possibility in chapter 14.
Also see page 346 which shows up in the index. As I recall, this is where he discusses the possibility of future experiments showing violations of Lorentz symmetry.
Not just in the book, but even in private coversations, Bohm & Hiley never explained or proposed such a "future" experiment.
In chapter 14 ,I think, they claim that their "field theory" (when formulated properly) COULD go beyond both relativity and QM. I know their method of introducing "arbitrary forces & momenta" into Bohm's equation of motion of QM. I also know that the method does not work.
Bohm has an important physical effect named after him, the Aharonov-Bohm effect. I don't see how you have the standing to call his ideas rubbish. There are still a lot of physicists working on his ideas.
Nice one.
I heppened to be the last person, to whom, Bohm spoke physics just one hour befor his death on Oct.27th.1992.
You never presented a view similar to that of Bohm or/and (my ex supervisor) Hiley. I suggest you read AND understand the book you mentioned.
As for the A-B effect, let me tell you that it is a Birkbeck College effect, this is because; 1) Bohm worked (even after retirement) at Birkbeck for 31 years, and most importantly; 2) the effect was first discovered at Birkbeck in 1949 by R. Siday (who died from alcohol abuse). For 10 years, the poor man work went unnoticed until Bohm and his student Aharonov "REDISCOVERED" the effect in 1959 at Bristol university.
After Bohm's death, Hiley promised to speak out and make this fact known to people. Apart from one paragraph in one of his articles in the royal socity, Hiley seems to have forgotten the promise he made in his professorship lecture in 1996.
SO PEOPEL, THE A-B EFFECT SHOULD BE CALLED THE SIDAY'S EFFECT.
Agreed. You've made a series of clearly true statements but I'm not sure what your point is. I'm going to guess that your logic is to point out that quarks are subparticles of protons and neutrons and yet quarks obey Lorentz symmetry just like neutrons and protons do. Therefore, perhaps by a sort of induction, all deeper subparticles must also obey Lorentz symmetry.
The point is this; We have NO good reasons (experiment or good theory) to believe in:
1) Lorentz non-invariant physics.
2) quark is or can be a bound state of some "stuff".
In order to believe in some idea, say preons, physicists need to see two things (for me No1 is enough):
1) mathematically sound theory (logical consistency & explanatory power)
2) experimental evidence.
Well, regarding preons and/or Lorentz violation, we have niether (1) nor (2). So, according to Occam's razor, we are better without them.
Let's apply your logic to the neutrons and protons themselves. Back before quarks were accepted would you have argued that all known particles carry integral electric charges and therefore quarks must too? Would you have argued that all known particles can be found in a free state and therefore quarks must too?
Larger than SU(2) symmetry ,SU(3), led naturally to fractional charges. Most physicists accepted the quark model when it was first proposed
(I would have done the same thing), because
1) it is based on mathematically sound theory
2) soon after the introduction of the quark model, many experimental verifications began to appear.
So, if I was arround in 1963, I would have said what S Coleman said about the quark model:
"It is too d... successful"
It is unwise to compare "the quark model and its success" with "preons and their failures" because
1) preon models are based on mathematically "full of garbage" theories with no experimental evidence.
2) they can not even explain the need for proposing them in the first place.
3) they can not achieve their goal (they end up with more particles than it is in real life)
4) THEY ARE UGLY AND SMELL WRONG.
5) the best of them (the one that pridicts some thing) leads to wrong pridictions, therefore it is wrong.
Do you have an outline of a proof that it is impossible for a non Lorentz invariant preon model to produce Lorentz invariant bound states? Or are you saying it's impossible only because you've never heard of it?
The very fact "I never herd of it" makes this particular model one of many irrelevant garbage arround.
However, I am very interested to see how "Lorentz non-invariant" dynamics (Lagrangian) "produces" a "Lorentz invariant bound state". So, I want you to write down the Lagrangian of this model and show me how it leads to Lorentz invariant bound state. I believe you know how to use LaTex, so I will be waiting to see that Lagrangian next time you post, OK?
regards
sam