B Is there a probability in QM that an event happens at time t?

  • #51
Morbert said:
iirc from a previous thread, it's concluded that the Zeno effect isn't due to measurement per se, but interaction between the measurement device and the measured system. I.e. the effect is present in the dynamics (even for seemingly, but not actually, indirect measurement scenarios) regardless of when we build "collapsed states" of measurement outcomes from some projective decomposition. https://www.physicsforums.com/threads/geiger-counters-and-measurement.1015428/
Indeed. Measurement always involves the interaction between measurement device and measured system. While for macroscopic objecs one can often neglect the influence of the measurement on the system, that's impossible for microscopic objects like single elementary particles. For sure, the explanation of the quantum Zeno effect is not to be based on an abuse of the well-understood mathematics of quantum theory and self-adjoint (not hermitean!) operators in Hilbert space!
 
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  • #52
.Scott said:
That would suggest that your were discussing (in your paper) strictly logarithmic decay - So P(n)/P(n-1) is a constant.
Is that really the case?
If it isn't, then knowledge of what measurements were attempted before t0 could be used to tweak the P(n)'s.
Measurements performed before ##t_0## are irrelevant to events that will happen after ##t_0##. The decay does not need to be exponential, but the stochastic process is Markovian (if you are familiar with that concept).
 
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  • #53
vanhees71 said:
For sure, the explanation of the quantum Zeno effect is not to be based on an abuse of the well-understood mathematics of quantum theory and self-adjoint (not hermitean!) operators in Hilbert space!
Just tell me one thing. If a wave packet travels towards the detector, and a part of the wave packet has already entered the detector region but the detector has not clicked yet, do I have to update the wave function of the packet?
 
  • #54
Demystifier said:
If a wave packet travels towards the detector, and a part of the wave packet has already entered the detector region but the detector has not clicked yet, do I have to update the wave function of the packet?
Does your model include the detailed interaction between the wave packet and the detector? Or does your model just treat the detector as a black box that emits clicks?

The answer to your question will depend on which type of model you have.
 
  • #55
Demystifier said:
Measurements performed before ##t_0## are irrelevant to events that will happen after ##t_0##. The decay does not need to be exponential, but the stochastic process is Markovian (if you are familiar with that concept).
I did just read an article on "Markovian" and it involved "current state" which I believe to be at the crux of my question. In essence I am asking about the nature of this "current state" in the kind of experiments explored in your paper.

I think I have a better way of asking this question. Basically I want to know whether there can be a QM case where this "current state" can be interrogated to reveal some of its history.

So, let's say that I have I have 512 experimental set-ups numbered 0 to 511. Each one simply repeats the same experiment over and over - but each one runs a slightly different variation of what is described in your paper. In all 512 set-ups, ##t_0##, ##t_10##, and all measurements after ##t_10## are always measured. But depending on the set-up some of the ##t_0## to ##t_9## measurements are made and some are skipped.

As examples:
In set-up number 0 (binary 000000000), ##t_1## through ##t_9## are all skipped.
In set-up number 1 (binary 000000001), ##t_1## through ##t_8## are skipped, but ##t_9## is made.
In set-up number 9 (binary 000001001), only ##t_1## and ##t_5## are made, the other 7 are skipped.

In set-up number 511, all the ##t_n##'s are measured, so the P(n)'s can be calculated exactly from the equations in your paper.

In every case, we capture measurement results starting with ##t_10##.

Question: Based only on the results of that captured information, could it ever be possible to deduce which data set goes with which set-up?

Can that much information be available in what the description of "Markovian" refers to as the "current state"?
 
  • #56
Demystifier said:
I don't have tome to read the whole thread. Can you tell which post concludes it?
Here is the relevant paper: https://arxiv.org/abs/quant-ph/0307075 the thread eventually touches on.

The paper models a continuous indirect measurement of the decay of an unstable atom with a Hamiltonian consisting of three terms: the atom, the interaction between the atom and the photon+detector terms that couple to it, and the photon+detector terms decoupled from the atom (see equations 7+8). The detector is physical insofar as it has a finite bandwidth.

The distinction between measurement and non-measurement is made with the Hamiltonian, specifically a form-factor that gets renormalised when the detector is present.
 
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  • #57
PeterDonis said:
Does your model include the detailed interaction between the wave packet and the detector?
No.
PeterDonis said:
Or does your model just treat the detector as a black box that emits clicks?
Yes.
 
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  • #58
.Scott said:
Can that much information be available in what the description of "Markovian" refers to as the "current state"?
No.
 
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  • #59
Demystifier said:
Measurements performed before ##t_0## are irrelevant to events that will happen after ##t_0##. The decay does not need to be exponential, but the stochastic process is Markovian (if you are familiar with that concept).
The decay cannot even be exactly exponential, because the energy is bounded from below. See the textbook by Sakurai about this. The stochastic process of a closed quantum system is Markovian.
 
  • #60
vanhees71 said:
No matter what, I'm not convinced that starting from obvious wrong maths leads to anything useful.
Sometimes it does. A good example is the Dirac delta function, because when Dirac introduced it, it was "obviously wrong" as it was not even a function. Nevertheless, it produced results that made perfect sense from a physical point of view, and later Laurent Schwartz found a way to make it "right" in a rigorous mathematical sense. I'm convinced that we have found something similar, in the sense that our idea is essentially consistent and correct, even if it still needs to be somewhat refined for the sake of mathematical purity. We developed our idea on the level of Dirac (and a little bit more), what remains is that someone does it on the level of Schwartz.
 
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  • #62
Closing this thread since the OPs question has been answered.

Jedi
 
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