Conversation started May 11, 2016 at 9:59.
May 11, 2016 09:59
I'm bored...I have to finish a paper but I'm lazy today
user116211
May 11, 2016 10:17
okay, I discovered that the old guy who formulated decoherence is....
user116211
can anyone guess?
user116211
No one ;_;
user116211
okay that old guy is from ACM's university! ACM must be acquainted with him ;/
a google search reveals him immediately
user116211
@yuggib yeh!
May 11, 2016 10:30
but I never heard of him before
user116211
@yuggib not even I. At least no undergrad QM books cover decoherence, let alone the man behind it.
yes, but decoherence is something quite natural
even if poorly understood from a mathematical standpoint (apart very few examples)
nevertheless some of the ideas are interesting
user116211
@yuggib CuriousOne understands it VERY well.
@MAFIA36790 he may understand the physics, surely not the mathematics behind it
;-P
user116211
I still do think decoherence doesn't explain collapse.
May 11, 2016 10:34
well, it actually does
but that has been proved by Ozawa, following von Neumann's ideas
user116211
@yuggib ooh... then i've to wait for more studies.
the point is that it is possible to define a measurement process (intended as a big system that couples the measurement apparatus to the observed system) that satisfies the required features of a measurement
at least it is possible, in QM systems, for every observable
and the apparatus has a scale on which you read the outcome of the measurement, and the system is suitably perturbed by the measurement, giving the apparent "collapse" of it if considered isolated
user116211
So, why do people still argue on that if it is well settled that collapse is explainable already by Decoherence?
that is mathematically pretty well understood (even if very few people know about that I think)
because people do not know that result...also it is a mathematical result
that describes theoretically the existence of such apparati and measurement processes for any given observable
for me it's crystal clear, but I don't know what other people may think
user116211
At least one statement, I remember, from Moretti:
user116211
May 11, 2016 10:41
> The nature of the second type of evolution is still source of an animated debate
in the scienti c community of physicists and philosophers of Science. There are
many attempts to reduce the collapse of the state to the standard time evolution
referring to the quantum evolution of the whole physical system, also including the
measurement apparatus and the environment (de-coherence processes). None
of these approaches seem to be completely satisfactory up to now.
user116211
Why that debate ;((
I find it satisfactory; but that is my opinion ;-)
user116211
People should stop spreading ambiguity then if the debate issue is solved ;(
user116211
Sigh
I'm saying that I find that answer satisfactory
but I am not the repository of ultimate truth
so I may very well be wrong
user116211
May 11, 2016 10:45
@yuggib Did I sound otherwise :(
I'm just saying I do not assert that I'm always right, and what I find satisfactory may not be such for other people
user116211
@yuggib ohh.
My current interpretation of quantum basically treat the maths as real entities. So far for most of the simple systems encountered in textbooks it worked pretty well because quantum states obey some kind of continuity equation, thus in some sense they behave like stuff in that they have some kind of conserved quantity. Under this interpretation, I found the interaction picture most natural of all the approaches
oh no
He's going Max Tegmark
I can comprehend any concepts that are chunky, which means, can be in some way represented as elements in a block diagram
May 11, 2016 10:52
He cannot understand love
Art is NOT one of them, though it seems somehow I do have emotions about them, but these cannot be described other than it is based on experience
Actually, I am not even sure if I understood romance, given that the minimal requirement I seek in all my friendships turns out to have qualities matches what other people called romance
I believe in a thing called love
user116211
May 11, 2016 11:29
@CuriousOne aren't you slightly exaggerating the insights from de-coherence? It can explain why a density matrix is diagonalized, but it still cannot tell us which one of the diagonals will be selected by a measurement and that's still a non-unitary process. It doesn't solve the measurement problem. — innisfree Jul 3 '15 at 10:55
@MAFIA36790 apart from the physics jargon, the dynamics of the full system apparatus+measured sys is unitary, as it is the isolated dynamics of the measured system
user116211
thanks for commenting @yuggib :)
@MAFIA36790 I would agree fully with the comment of innisfree
Well, almost
simply, to describe the measurement process happening in an interval $[0,T]$ of time you need to consider both: the resulting global evolution would be time-dependent, and the full Hamiltonian would contain an interaction term that is non-zero only in the time interval $[0,T]$
The selection of the diagonal doesn't have to be non-unitary, since it can be a process that happens in your mind, i.e. just Bayesian updating of a probability distribution. But that implies a radical denial of realism to the point of solipsism
May 11, 2016 11:33
(interaction between system and measurement apparatus)
@MarkMitchison still that is not necessary, since the process can be explained in satisfactory and unitary terms considering a more complete system+apparatus picture
@yuggib That's not true, but I assume you didn't understand what I meant. The interaction between quantum systems only explains the reduction of marginal states from coherent superpositions to incoherent mixtures. My point is that it remains unexplained why only a single element of the incoherent mixture is ever observed.
May 11, 2016 11:48
@MarkMitchison Either I do not understand the language, or that is an oversimplification. It is not true, apart from special observables with discrete spectrum, that "a single element of the mixture is ever observed".
In a measurement you observe a value on your scale that is included in an interval of the real numbers (due to the limited precision of your scale or whatever; possibly the interval may consist of just a single point)
that induces accordingly a change on the reduced state of the system (partial trace of the whole state), that it is possible to understand theoretically
and that represents the fact that the measurement yielded the aforementioned outcome lying in an interval of real values
that is how I would explain the "collapse" (actually, von Neumann and Ozawa provided the explanation)
@yuggib Of course you are right (except that I disagree with you about continuous spectra: all actual observables have discrete spectra). What I am talking about is the process whereby one of these values or intervals of values is actually "selected", which cannot be described simply by invoking interaction with a larger system.
@MarkMitchison well, it is hard (actually impossible) to explain how values are "selected" in a probability theory; and quantum theories are (non-commutative) probability theories
@yuggib Yes, but in classical probability theory you can always assume that there was only one "real" underlying value, which was obscured by uncertainty over initial conditions. And therefore there is no philosophical problem with the selection process. In QM you cannot do this (unless you want to use non-local hidden variables). This is the crux of the problem. If QM admitted an acceptable realistic interpretation then of course everything would be fine.
@MarkMitchison I don't care less about the philosophical interpretation, sorry ;-P For me probability theory is still perfectly acceptable without that assumption you make.
@yuggib Sure, you don't have to care. But what I was talking about is the philosophical problem you don't care about, i.e. the measurement problem. So it's not true that extending the Hilbert space to include the measurement device somehow solves anything regarding this problem.
May 11, 2016 12:03
@MarkMitchison if the measurement problem is a metaphysical problem, then it has nothing scientifical.
and nothing could help solve a metaphysical problem apart from belief and hope
@yuggib Yep. This is of course well known.
Although perhaps it deserves to be better known.
Maybe, but that applies also to the supposed existence of a god... ;-P
(maybe the two questions are related somehow)
But the metaphysics is nevertheless important for science, because it frames the language in which we speak. For example, if there is nothing real or physically meaningful about "observables" such as position and momentum, perhaps we are missing out on a much more efficient description.
For you of course they're not physical, since you said before that "actual" observables have only discrete spectrum
isn't quantum is already being experimentally proved to be a non realist theory?
user116211
May 11, 2016 12:07
Okay, if the measurement problem is metaphysical, then why not discard it? There would be no debate then.
@yuggib I'm just saying that position and momentum cannot be measured to arbitrary precision.
@Secret No, it's been proven to be incompatible with local realism. Non-local realism is still "fine".
@MarkMitchison Yes, so that qualifies them as not observables?
@MAFIA36790 See my comment above, scientific interpretation is based on metaphysics. I'm not saying you should waste your time debating the measurement problem, though it is fun when drunk
@yuggib I'm just saying operators with continuous spectra are a mathematically convenient model for position and momentum observables, but there is no fundamental need for them to be continuous.
@MarkMitchison apart that, roughly speaking, no non-continuous observables can satisfy the canonical commutation relations?
user116211
@MarkMitchison There is no waste of time as it is a physical problem and not just based on trivial metaphysical arguments.
May 11, 2016 12:14
@yuggib Of course, but that's hardly a problem. It's clear that no deviations from the CCR would be observed assuming a sufficiently dense discrete spectrum for $q$ and $p$
Really the point I'm making is that it's a convenient, yet entirely metaphysical, choice to assume that $x$ and $p$ are really continuous. There is no experiment that could ever disprove that hypothesis.
So again it's not science. But you nevertheless find it important enough to discuss with me ;) So I think we all like a bit of metaphysics somewhere.
Well, science is about making falsifiable statements, and the statement $x$ and $p$ are continuous observable is a falsifiable statement, at least in theory
the fact that no experimentalist is (supposedly) able to falsify it, does not make it less scientifical
@yuggib Actually yes, that's a fair point. An experiment demonstrating violation of the CCR on some scale is conceivable. So in that case, I guess what I'm saying is that I am sceptical about the unproved hypothesis that $x$ and $p$ are continuous.
I say supposedly because I am absolutely not convinced that you could "approximate" CCR to any given precision by means of sufficiently dense discrete spectra
@MarkMitchison Ok, I see your point. Nevertheless you have to admit that such an assumptions, i.e. the assumptions of CCR gives you a lot of very accurate and tested predictions about quantum systems
would you be able to reproduce all the aforementioned confirmed predictions by means of an alternative theory? Is it worth it?
@yuggib In the end the CCR are irrelevant. What matters is that observable properties are the same either way. In my experience, lattice models always correctly reduce to the continuum limit when taken.
Lattice models are done via path integrals, though
They reduce to a path integral in the end which has Ways to derive the CCR
via the class of paths that have a non-0 measure
May 11, 2016 12:22
@yuggib No, it's of course not worth it because calculus is easy and discrete summations and difference equations are hard.
If x and p has a continous spectrum, must it also necessary mean that spacetime is also continous (as otherwise I cannot see how x and p states can be quantised at all, what kind of mechanism can induce them to be quantise like in a bound state scenario, if any?
@Slereah Um, path integrals are defined on a lattice.
Depends
You can define them on a lattice
Or not
Lattice is certainly easier
If you want to actually solve them, you define on a lattice
Otherwise it's just a notation
(i;.e. shorthand for the lattice definition)
Nah, it can work out alright if you use like
a wiener measure
(heheheh wiener)
For a somewhat restricted class of potentials, but still
May 11, 2016 12:25
Yeah, but now you're going to undue effort just to restore the continuum description!
From the point of view of actually calculating anything in modern QFT, space and time are discretised.
well gee sorry I didn't know doing physics was undue effort
Of course, one does assume that the fields are continuous.
@HariPrasad : I know exactly how magnets work.
@Slereah Ha, no I was more referring to the idea that it's always easier to assume continuous variables.
Formally speaking
Though to be fair, yeah most computations are done on a lattice
It is way easier
Though you lose some in rigor
May 11, 2016 12:28
Actually, I would say that the choice of $x$ and $p$ being discrete or continuous is arbitrary and philosophical, until such time as one could experimentally falsify one choice or the other.
And given the lack of any direct experimental evidence for continuous spectra, I choose to be sceptical.
How do you check for that, though
You can always say that the discrete scale is arbitrarily small
You can falsify the hypothesis that they are continuous
You can't strictly speaking falsify the converse
@MarkMitchison and I would say that the predominance of a theory over another is given by the predictive power; and the extent of predictive power given by usual quantum mechanics, i.e. the non-commutative probability given by the algebra of CCR over finite dimensional symplectic spaces, is unsurpassed by any other alternative theory
on what scale will we expect to see p and x became discrtised?
Planck scale, hopefully
May 11, 2016 12:31
so pretty much that question can be expt tested under quantum gravity conditions, I guess
@yuggib The predominant formalism in modern quantum mechanics is the path integral, which to all practical purposes is based on a discrete lattice of spacetime points not a continuous manifold. And is also known to reproduce the predicitons of other formulations of QM. So I don't agree with that statement at all.
@MarkMitchison path integral is not even wrong, since it is a non-rigorous pseudo-mathematical theory (at least at the present level of knowledge)
so statements given using path integrals are, in my opinion, moot
Well there are rigorous path integrals
apart from the very few cases where everything has a rigorous meaning
The hard part is making them rigorous for interacting fields
May 11, 2016 12:33
@yuggib Well that is what I really call metaphysics (for mathematicians). Path integrals have survived every experimental test, genuine science doesn't care about (mathematical) rigour. Or rather, science has a different kind of rigour (experimental rigour).
QFT without path integrals? I am not aware of that
@yuggib But I can see this is another one of those "agree to disagree" situations between physics and mathematics approaches.
there's plenty of QFT without path integrals
@MarkMitchison I don't think so; it is an example of people saying "who cares" until they find something for which it is important to care
in physics, we cared more about whether the model fits the observations and predict new phenomenon, more than the mathematical rigor. Personally, I prefer the maths to be rigorous, as it provide a soild frame work to extend a model to fit new observations, but ultimiately it is the experiments that has the final verdict on whether a model survives
May 11, 2016 12:36
@yuggib How do you mean?
Do you mean you expect that one day we will find a physical situation that cannot be modelled properly with non-rigorous path integrals?
@MarkMitchison Yes exactly
OK. But until such time, this remains metaphysics ;)
well, you may say that physicists at the beginning modelled the volume of space we live in with a lattice of integers (and you still believe it to be true); however the discovery of the circumference of a circle put that belief in jeopardy
@yuggib And for what it's worth I would claim the opposite: that one day some illustrious mathematician will finally make the formalism rigorous. Of course, physicists will not be that interested.
since there is no experiment that can fix the integer value of the circumference of a circle of radius one
May 11, 2016 12:40
But @yuggib, how will you know
With a small enough lattice it would drop below experimental error
I am saying that no known experiment could prove that the circumference has an integer value
no matter how much precise the experiments became, there is no way of proving that
Tell that to Leopold Kronecker
you may still believe that the circumference has an integer value
@yuggib Or you could just choose not to really pick a strong side, accepting that you'll never prove things one way or another.
But I am perfectly aware of that, as is every mathematician; I am not sure physicists are so willing to accept that, and stick to beliefs and interpretations
in fact, if I produce a mathematical result, I do it in a certain theory (i.e. "choosing one side"), but I am perfectly aware it is possible to prove different results in a different theory (the other side)
May 11, 2016 12:45
Well, I agree with the sentiment, but it's also just a practical choice. Path integrals are a wonderful tool. It's a shame not to use them just because we don't understand them fully. As soon as you prove that they aren't self-consistent, of course they'll be dropped immediately. But until then, it's crazy not to use them.
the results have equal value for a mathematician, i.e. they are true in the given theory
@yuggib And of course you are right that physicists like to believe and interpret a lot.
But as long as it's remembered that all interpretations must be ultimately limited by scientific rigour (i.e. agreement with empirical results), then it's ok I think
@MarkMitchison I agree about that, nevertheless there is the risk of saying something false when you use a theory that is not well understood. My personal belief is that everything that is done using path integrals may be justified one day mathematically
QFT is kind of weird really
but there is always the risk of some unexpected thing popping out
May 11, 2016 12:48
So many things in it have big theorems saying THIS SHOULD NOT WORK
@yuggib Yes, but of course the correct approach is to use the tool until it breaks (or breaks something else), not to leave it out of fear of the unknown.
@Slereah well everything that is used in practice would work in some sense, simply you have to be careful
@MarkMitchison Well that is your job, mine is to justify why that tool should work (and possibly understand something deeper in doing that)
@yuggib Indeed
 
Conversation ended May 11, 2016 at 12:49.