Heisenberg Uncertainty Principle

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Discussion Overview

The discussion centers around the Heisenberg Uncertainty Principle and its implications for measuring the position and momentum of particles, particularly in the context of particle accelerators. Participants explore the limitations of measurements and the theoretical underpinnings of the principle.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that the uncertainty principle implies that precise measurements of both position and momentum cannot be obtained simultaneously, leading to rough measurements in particle accelerators.
  • Others argue that while one can measure position or momentum with high accuracy, doing so for both at the same time is not possible due to the nature of non-commuting observables.
  • A participant references the EPR paper and suggests that the discussion relates to the concept of entangled particles and their properties.
  • Some participants challenge the interpretation of the uncertainty principle, suggesting that it may be misleading to state that both quantities cannot be measured accurately at the same time.
  • There is a mathematical discussion regarding the implications of assuming zero uncertainty in position and its consequences for momentum.
  • Another participant asserts that no particle can possess both a precise position and momentum simultaneously, aligning with the principles of quantum mechanics.

Areas of Agreement / Disagreement

Participants express differing views on the interpretation of the Heisenberg Uncertainty Principle, with no consensus reached on the implications for measurements in particle physics. Some agree on the fundamental nature of the principle, while others contest the explanations and interpretations provided.

Contextual Notes

Limitations include the dependence on definitions of measurement accuracy and the theoretical nature of particles in quantum mechanics, which complicates the discussion of precise measurements.

tom_the_cowboy
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The Heisenberg Uncertainty Principle states that both the exact (as near as we can get to thusfar) position AND momentum of a particle cannot be obtained because in learning its exact position we alter its momentum and vice versa. Does this mean we only have rough measurements of particles produced in particle accelerators? If so, why can't two particles be produced from a collision and the momentum of one measured and the position of the other measured thereby giving exact measurements of both position and momentum for each (albeit after the measurements were taken both variables would have changed, but at least exact measurements at the point of collision could be obtained). Can this be done? Has it? Is there some basic physics principle I've forgotten about?

Thanks for your replies in advance.
 
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tom_the_cowboy said:
The Heisenberg Uncertainty Principle states that both the exact (as near as we can get to thusfar) position AND momentum of a particle cannot be obtained because in learning its exact position we alter its momentum and vice versa. Does this mean we only have rough measurements of particles produced in particle accelerators? If so, why can't two particles be produced from a collision and the momentum of one measured and the position of the other measured thereby giving exact measurements of both position and momentum for each (albeit after the measurements were taken both variables would have changed, but at least exact measurements at the point of collision could be obtained). Can this be done? Has it? Is there some basic physics principle I've forgotten about?

Thanks for your replies in advance.

The uncertainty principle states that for "non-commuting observables" like position and momentum, The product of the uncertainty in one times the uncertainty of the other has a constant lower bound.

Note that you can get position as accurate as you like (and your experimental techniques can support), or you can do momentum as accurately as you want. You just can't do them BOTH with arbitrary precision at the same time. Classical readouts from accelerators, like bubble chambers, tried for position accuracy and simply didn't look at momentum. You got photographs of trajectories.

On the other hand "calorimeters", essentially stacked sheets of armor plate that measure momentum by seeing how many sheets the particle can penetrate, look only at momentum. So you see they DO obey the Uncertainty Principle - they have to! But they do manage to collect the information they need by looking at different events with different particles.
 
tom_the_cowboy said:
The Heisenberg Uncertainty Principle states that both the exact (as near as we can get to thusfar) position AND momentum of a particle cannot be obtained because in learning its exact position we alter its momentum and vice versa. Does this mean we only have rough measurements of particles produced in particle accelerators? If so, why can't two particles be produced from a collision and the momentum of one measured and the position of the other measured thereby giving exact measurements of both position and momentum for each (albeit after the measurements were taken both variables would have changed, but at least exact measurements at the point of collision could be obtained). Can this be done? Has it? Is there some basic physics principle I've forgotten about?

Thanks for your replies in advance.
Dear Cowboy,
You are right! Your idea is the same which you can read in A. Einstein, P. Podolsky, R Rosen "Can the Quantum-Mechanical Description be Complete?" in Phys. Rew., 1935, p.777, Number I do not remember.
This paper is very often citation. But the EPR idea is change and now employ to the spin-states. In this paper you cannot see particles with SPIN. In the same time Bell's experiments was found on the this paper but Bell employ EPR idea to spin-statistics.
Cartuz.
 
selfAdjoint said:
Note that you can get position as accurate as you like (and your experimental techniques can support), or you can do momentum as accurately as you want. You just can't do them BOTH with arbitrary precision at the same time.

TO THE OP : Though this is very correct, i never understood why people explained the HUP like this. I find it very misleading. As a matter of fact you can get both position and momentum completely accurate, or at least as accurate as your measuring device alows you to acquire these data. What i mean is that for a given fixed position, you can get a definite momentum value. It is just that if you were to measure the momentum value again at that same position, you will acquire another value. This way of looking at the HUP also gives a clear view as to how you need to look at the calorimeter thing.

regards
marlon
 
marlon said:
i mean is that for a given fixed position,

And how do u define that using physical & mathematical terms...?

Daniel.
 
dextercioby said:
And how do u define that using physical & mathematical terms...?

Daniel.
:smile:

just assume that the uncertainty of position is zero and the uncertainty of p is infinite. :smile: That's the whole point

marlon
 
U can't assume the uncertainty in position is zero.It's a nonphysical state.

Daniel.
 
I can to clear HUP by my way.

[tex]xp=\hbar/2[/tex]

[tex]xm\overset{\cdot}{x}=x\overset{\cdot}{x}\frac{F}{\overset{\cdot\cdot}{x}}=\hbar/2[/tex]

It is the equation which I can name the quantum oscillation equation

[tex]\overset{\cdot\cdot}{x}-(\frac{2F\overset{\cdot}{x}}{\hbar})x=0[/tex]
[tex]\omega^{2}=\frac{2F\overset{\cdot}{x}}{\hbar}[/tex]

Than HUP is equal to oscillation equation! Because x and p not independent.
 
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It doesn't make any sense what u wrote there,i sincerely hope u realize that,too.

Daniel.
 
  • #10
dextercioby said:
U can't assume the uncertainty in position is zero.It's a nonphysical state.

Daniel.

I think you are missing the point. If you don't want to take a zero uncertainty, then just take a small one...Even you can take it as big as you want, it really does not matter to what i am trying to say. There is nothing that says you cannot place a detector at one fixed position and check out if a particle passed through it.

marlon
 
  • #11
marlon said:
I think you are missing the point.

Maybe... :rolleyes:

marlon said:
If you don't want to take a zero uncertainty,

Oh,but I do,but it's IMPOSSIBLE.

Daniel.
 
  • #12
tom_the_cowboy said:
Does this mean we only have rough measurements of particles produced in particle accelerators? If so, why can't two particles be produced from a collision and the momentum of one measured and the position of the other measured thereby giving exact measurements of both position and momentum for each (albeit after the measurements were taken both variables would have changed, but at least exact measurements at the point of collision could be obtained). Can this be done? Has it? Is there some basic physics principle I've forgotten about?

Actually it's not even about measurement, as no particle exists in the theory with the properties of both a precise position and a precise momentum, so if quantum mechanics is the correct way to describe nature, then both can't be assigned to any particle in the way we might like. :smile:
 
Last edited:
  • #13
tom_the_cowboy said:
The Heisenberg Uncertainty Principle states that both the exact (as near as we can get to thusfar) position AND momentum of a particle cannot be obtained because in learning its exact position we alter its momentum and vice versa. Does this mean we only have rough measurements of particles produced in particle accelerators? If so, why can't two particles be produced from a collision and the momentum of one measured and the position of the other measured thereby giving exact measurements of both position and momentum for each (albeit after the measurements were taken both variables would have changed, but at least exact measurements at the point of collision could be obtained). Can this be done? Has it? Is there some basic physics principle I've forgotten about?

Thanks for your replies in advance.

I think EPR is the key to your question, as posts has discussed before, but i still have one point to say. at colliders, this is not a problem in experiment (although it is still a problem in theory), because the momentum is very large, and a uncertainty delta p can be egnored for practical insterest. That is why
at colliders it *seemed* to be able to measure x and p together.
 

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