Double-slit experiment and watching the electrons

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SUMMARY

The forum discussion centers on the double-slit experiment and the implications of "watching the electrons" using a strong light source. Participants debate whether using a long wavelength light source allows for interference patterns to persist when observing electrons. Key points include the relationship between photon interaction and interference visibility, as well as the mathematical formulations of probabilities associated with electron detection. The discussion references Feynman's lectures and explores the duality of wave-particle behavior in quantum mechanics.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly wave-particle duality.
  • Familiarity with the double-slit experiment and its significance in quantum physics.
  • Knowledge of photon-electron interactions and their effects on interference patterns.
  • Basic grasp of quantum probability amplitudes and Hilbert spaces.
NEXT STEPS
  • Research the mathematical formulations of quantum probability amplitudes in the context of the double-slit experiment.
  • Explore Feynman's lectures on quantum mechanics, specifically the implications of observation on wave functions.
  • Investigate experiments utilizing long wavelength light sources in double-slit setups to observe interference patterns.
  • Study the Englert-Greenberger duality relation and its relevance to interference and which-path information.
USEFUL FOR

Quantum physicists, students of quantum mechanics, and researchers interested in the foundational principles of wave-particle duality and experimental quantum physics.

  • #31
Do you know if S M TAN is Shina Tan? He looks very young.
 
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  • #32
naima said:
Do you know if S M TAN is Shina Tan?

No. S M Tan is Sze Meng Tan.
 
  • #33
thank you.
There is a 3/2 factor in the visibility formula. From which identity does it come?
 
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  • #34
We begin with an integral from zero to pi of a function of the angle \theta.
Using x = cos (\theta.) visibility of the fringes becomes
A\int_{-1}^1 (1+x^2) e^{i u x} dx.
Integrating it twice by parts we get
4A [\frac{sin u}{u}+\frac{cos u}{u^2}-\frac{sin u}{u^3}].
"u" being the distance of slits divided by the wavelength of the photon when it decreases to zero the limit of visibility must be 1. We need so a normalization factor and the good formula is
3/2 [\frac{sin u}{u}+\frac{cos u}{u^2}-\frac{sin u}{u^3}].

We can compute the visibility when u = 1. It is when we watch the electrons with light having for wavelength the distance
between the slits. We have V(1) = 3/2 cos(1) = 0.8
So the visibility is still very good!
 
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