Uncertainty principle and photon

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SUMMARY

The discussion clarifies misconceptions regarding the measurement of a particle's position and momentum in relation to the uncertainty principle. It highlights that while shining a photon is a common method for measurement, it is not the only technique available. The single slit diffraction experiment demonstrates that the width of the slit (\Delta(x)) can also define the position of a photon without the need for additional light. The intrinsic nature of the uncertainty principle means that improvements in measurement techniques do not eliminate the fundamental limits imposed by quantum mechanics.

PREREQUISITES
  • Understanding of the Heisenberg Uncertainty Principle (HUP)
  • Familiarity with quantum mechanics concepts such as conjugate pairs
  • Knowledge of single slit diffraction and its implications
  • Basic principles of measurement techniques in quantum physics
NEXT STEPS
  • Research the implications of the Heisenberg Uncertainty Principle on quantum measurements
  • Study single slit diffraction and its role in quantum mechanics
  • Explore advanced measurement techniques in quantum physics, such as using CCDs
  • Investigate the relationship between measurement accuracy and quantum uncertainty
USEFUL FOR

Students and professionals in physics, particularly those focused on quantum mechanics, experimental physicists, and anyone interested in the foundational principles of measurement in quantum systems.

spidey
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i have always read in almost all sites that we have to shine at least a photon to measure the particle's position and momentum and hence comes the uncertainty principle...why we are using this shining photon technique always...is this the only way of measuring particle's position and momentum...is there any other method other than shining photon method to measure particle's position and momentum so that we can measure position and momentum with great accuracy...am i missing anything?
 
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spidey said:
i have always read in almost all sites that we have to shine at least a photon to measure the particle's position and momentum and hence comes the uncertainty principle...why we are using this shining photon technique always...is this the only way of measuring particle's position and momentum...is there any other method other than shining photon method to measure particle's position and momentum so that we can measure position and momentum with great accuracy...am i missing anything?

This is not actually correct. For example, in the single slit diffraction, one narrow down the position of a photon passing through the slit using just the slit width. So if the slit has a width of \Delta(x), then the photon that passed through the slit was in that position, with an uncertainty of position being \Delta(x).

You will also notice that if the width is made smaller and smaller, your ability to predict the value of p_x after it passes the slit becomes less and less accurate. The photon can acquire a larger range of momentum values as you make the slit smaller. Thus, the spread in momentum becomes larger as more and more photons passes through the slit. The uncertainty in position (\Delta(x)) will corresponds in the spread in this momentum, i.e.\Delta(p_x).

In this case, you'll notice that we did not use any light to shine on the particle that we want to measure (this works for any quantum particle such as photons, electrons, neutrons, protons, etc.). In other words, it has nothing to do with instrumentation accuracy. It is intrinsic.

Zz.
 
ZapperZ said:
This is not actually correct. For example, in the single slit diffraction, one narrow down the position of a photon passing through the slit using just the slit width. So if the slit has a width of \Delta(x), then the photon that passed through the slit was in that position, with an uncertainty of position being \Delta(x).

You will also notice that if the width is made smaller and smaller, your ability to predict the value of p_x after it passes the slit becomes less and less accurate. The photon can acquire a larger range of momentum values as you make the slit smaller. Thus, the spread in momentum becomes larger as more and more photons passes through the slit. The uncertainty in position (\Delta(x)) will corresponds in the spread in this momentum, i.e.\Delta(p_x).

In this case, you'll notice that we did not use any light to shine on the particle that we want to measure (this works for any quantum particle such as photons, electrons, neutrons, protons, etc.). In other words, it has nothing to do with instrumentation accuracy. It is intrinsic.

Zz.

thank you for clearing my doubt...
 
ZapperZ said:
In other words, it has nothing to do with instrumentation accuracy. It is intrinsic.

I always thought of it as something fundamental about physical laws (about conjugate pairs in mechanics), such that measuring devices *always* causes a back-reaction at least as large as uncertainty principle says. I guess I mean that I think it's both.
 
genneth said:
I always thought of it as something fundamental about physical laws (about conjugate pairs in mechanics), such that measuring devices *always* causes a back-reaction at least as large as uncertainty principle says. I guess I mean that I think it's both.

Maybe it does. However, we should also pay attention to the fact that the uncertainty in a single measurement can be improved with better technique and better technology. I can measure the position that an electron hit a CCD much better than using simply a charge-sensitive plate. That improves the accuracy of a position measurement. Yet, it does nothing to my knowledge of its non-commuting observable within the HUP.

Thus, improving the measurement uncertainty isn't tied to the HUP. Simply having better instruments does not make the HUP go away, or make the non-commuting observable better known.

Zz.
 

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