stevefaulkner
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Do physicists care whether Quantum Mechanics can be understood? Or are they happy with it as it is so long as they can do calculations with it?
The discussion revolves around the perspectives of physicists regarding the conceptual understanding of Quantum Mechanics (QM) versus its practical utility. Participants explore whether physicists are satisfied with QM as it stands, given its predictive success, or if they seek a deeper understanding of its foundations and implications.
Participants express a range of views, with no clear consensus on whether physicists are satisfied with QM as it is or if they seek a deeper understanding. Multiple competing perspectives on the implications and foundations of QM remain unresolved.
Participants highlight limitations in the current understanding of QM, including unresolved questions about electron behavior and the relationship between QM and gravity. There is also mention of the philosophical challenges that arise from the theory.
stevefaulkner said:Do physicists care whether Quantum Mechanics can be understood? Or are they happy with it as it is so long as they can do calculations with it?
A nucleus with a large charge will cause an electron to have a high velocity. A higher electron velocity means an increased electron relativistic mass. These relativistic effects are experimentally showed.
So, the electrons are actually moving fast obeying the probability density of the Schrödinger equation (or other equations which show the probability density) ?
If so, why don't they radiate energy?
If the electrons are not actually moving as the electron clouds, why does the relativistic mass change occur?
In the relativistic theory, the particle's movement in one direction means our (observer's) movement in the opposite direction. So if we (observers) are actually moving in one direction and the relativistic effects of the observed particles are seen,
this means that these effects are caused by the particles' actual movement in the opposite direction?
humanino said:There are a few mathematical details to polish, but I'm pretty happy with decoherence, and I think people who claim it is inconsistent with Bohr's interpretation never talked to him directly.
I just think it's quite unfair to imagine Bohr had a naive view on the so-called problem of measurement.Phrak said:Umm. Perchance, have you spoken to Bohr? Or know someone who has? If you have a story to tell, it would be wonderful if you told it.
ytuab said:Why doesn't the electron fall into the nucleus radiating energy in standard QM?
stevefaulkner said:Do physicists care whether Quantum Mechanics can be understood? Or are they happy with it as it is so long as they can do calculations with it?
Winter Flower said:As a person who is currently learning quantum mechanics, it seems like there is still room for something that would make it more intuitive. I am trying to learn the theory without wondering about the philosophical paradoxes too much (since it apparently works). Your project sounds interesting...
Some of them are happy, and some of them are not. Those who are happy are mainly interested in practical aspects of physics, while those who are not are interested in deep understanding of nature as well.stevefaulkner said:Do physicists care whether Quantum Mechanics can be understood? Or are they happy with it as it is so long as they can do calculations with it?
Demystifier said:Some of them are happy, and some of them are not. Those who are happy are mainly interested in practical aspects of physics, while those who are not are interested in deep understanding of nature as well.
You might like this:Bob_for_short said:I can safely say that nobody understands Classical Mechanics. I mean where CM determinism comes from.
It is not really what I wanted to underline. In CM we can entirely stay within CM to see where CM determinism comes from. It's easy.Demystifier said:You might like this:
http://xxx.lanl.gov/abs/quant-ph/0505143 [Found.Phys.Lett. 19 (2006) 553]
I think it comes from the fact that the contribution from non-renormalizable terms in QFTs are negligible at low energies. (The proof is an order-of-magnitude estimate based on dimensional analysis of the coupling constants. I read about it 11 years ago and I didn't fully understand it). For example, if we view QED as an effective field theory it should contain all the interaction terms that are consistent with Lorentz invariance and U(1) gauge invariance, but all but one are non-renormalizable and therefore negligible at low energies. The classical limit of the renormalizable theory is classical electrodynamics, which is nice enough to ensure that Newton's second law (for forces caused by electrodynamic interactions) is a differential equation of the formBob_for_short said:I can safely say that nobody understands Classical Mechanics. I mean where CM determinism comes from.
If we assume that the mathematical model defined by the axioms is a description of what actually happens when experiments are performed (the many-worlds interpretation), it can only be described as completely determininstic.Phrak said:Clearly, quantum mechanics, as a set of axioms that includes the Born postulate,
P(x) = ∫ |Ψ(x,t)|² dx, where P(x) is a probability density,
is a nondeterministic system.
Fra said:my approach during the courses was to adapt the best possible survival view - the copenhagen view, where the arbitrary choices was to be treated as "facts of science". This was just a survival strategy, otherwise I would have spend all time questioning the formalism, instead of learning how to use it (which is after all the purpose of the course).
Fredrik said:If we assume that the mathematical model defined by the axioms is a description of what actually happens when experiments are performed (the many-worlds interpretation), it can only be described as completely determininstic.
If we instead assume that the mathematical model defined by the axioms doesn't describe what actually happens (the ensemble interpretation), the time evolution of the state vector is still deterministic, but measurement results are not.
Bob_for_short said:It is not really what I wanted to underline. In CM we can entirely stay within CM to see where CM determinism comes from. It's easy.
Let us consider a body that is cinsidered as a point in CM. In fact, it is not a just point but a compound system. In its "entire" CM descriprion we naturally use the center of inertia (CI) or center of mass coordinates R(t) and the relative coordinates {ri}, i = 1-N, N>>1. The relative coordinates are normally oscillating/rotating and exchanging their energy with the envoronement. For example, we see the full Moon due to light emitted with the Moon's internal degrees of freedom. We take many-photon picture, make an average of it and obtain one definite value R(t). The entire concept of space-time in CM implies this multi-photon exchange. Then we forget about the way how we "observe" CM objects, concentrate on simple mathematics of CI dynamics and speak of determinism. But factually our way of obtaining definite pictures in CM is the same as our way of obtaining an interference pattern in QM. In both cases we take huge ensembles of points. In this sense QM results - wave functions, are as determinate as CM ones, if dealt with properly - describing ensembles of points and thir derivatives (average ="position", dispersion ="size", etc.). Unfortunately, in QM (a low intensity regime) we concentrate too much on one-point experimental issue and "discover" "indeterminism" in its prediction. But observing the Moon with one- or few-photon picture brings the same indeterminism in CM as that in QM. So there is only one indeterminism in both CM and QM and it is of the same nature - lack of statistics (lack of data). The randomness of particular points is easily understood as due to "multi-particle", compound, complex nature of observed objects.
Phrak said:Do you know how either the pilot wave interpretation or ensemble interpetation interprets the Born postulate?