BOAS
- 546
- 19
Bose-Einstein condensates allow us to look at quantum effects at the macroscopic scale.
jarekd said:Another place we use them in quantum mechanics is the Wick rotation to "imaginary time", which corresponds just to the Legendre transform: changing sign in kinetic term while getting from Hamiltonian to Lagrangian density
https://en.wikipedia.org/wiki/Photon_antibunchingjarekd said:bhobba, sure everything can be seen from quantum perspective ... but is there anything what cannot be also seen from classical field theory perspective?
Yes and that's a very fundamental property of systems with identical particles: their states have to be symmetric or antisymmetric under particle exchange. "Breaking" such a joint state is not possible because the resulting state wouldn't have the right symmetry.Maui said:Correct me if I am wrong but they do not occupy the same state but a joint state similar to the joint state of entangled particles where even the slightest disturbance breaks the joint quantum state. Obviously in the superfluid helium somehow it does not.
Do you disagree with the argument given in the wikipedia-link? (I don't have access to better sources at the moment but the claim that antibunching is not explainable classicaly is widely accepted in the quantum optics community)jarekd said:Kith, I don't understand why you have pointed photon antibunching? [...] Why are suggesting that it cannot be understood from one of these perspectives?
kith said:As far as classical behaviour is concerned, you seem to define it via decoherence. This doesn't make sense. A phenomenon is "classical" if it can be explained by classical mechanics. Decoherence shows how classical mechanics emerges from QM. This doesn't say anything about the existence of genuine quantum effects which can not be explained by classical mechanics. If there were none, we wouldn't need QM in the first place.
Of course, it is justified to check how the formalism of QM can be explained from more fundamental principles. For example, there has been a lot of reasearch on the question "why do observers see random results?". We now have all kinds of different explanations: hidden variables, influences from the future, other worlds and so on.jarekd said:Quantum mechanics has became kind of "intelligent project" type of argument - if we don't understand something, we can always say that "it is quantum" ... and problem solved.
And why should this be a sensible definition? After all, it includes classical electrodynamics. Why do you reject the obvious definition that quantum effects are effects which are only predicted by quantum mechanics but not by classical mechanics / electrodynamics?Maui said:No, my definition of quantum behavior is observing directly or indirectly(post factum observation of) behavior that can only be explained in terms of wave like properties(e.g putting an object in its ground state).
kith said:And why should this be a sensible definition? After all, it includes classical electrodynamics. Why do you reject the obvious definition that quantum effects are effects which are only predicted by quantum mechanics but not by classical mechanics / electrodynamics?
I agree. Different points of view regarding the interpretation of QM may lead to different paths for physics beyond the Standard Model.jarekd said:The purpose of deeper theories is different - like understanding, intuitions ... and thanks of it also better models of what we cannot directly measure - which could not only explain, but also derive quantitative properties of more effective models, like parameters of the standard model ...
jarekd said:It has the essence of wave-corpuscle duality: it is going from thermodynamics of a point particle (after some small correction it can be seen as stochastic modeling) to seeing them only through their wave nature.
kith said:But the problem with all of them is that the thing which is supposed to explain the random results, can not be observed in measurements even in principle. And QM suggests why this is so: any interaction leads to entanglement and in order to perform a measurement on a system, you have to interact with the system.
jarekd said:Bill, Schrodinger's original derivation was practically based on Hamilton-Jacobi these nine decades ago: http://gallica.bnf.fr/ark:/12148/bpt6k153811/f373.image.langFR
Quantum mechanics is universal; it applies to all objects, including big objects. But most of quantum mechanics is simply not spectacular enough to make headlines. Only the quantum effects that sound weird in everyday language, and hence are the focus of most of the popular talk about QM, get weaker and weaker as the object mass grows, and hence are spectacular enough for public attention only for very small quantum systems of a kind with which one can readily make experiments with.AdrianHudson said:Why can't QM be applied to bigger objects?