I Math of Electron Double Slit Experiment

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The discussion centers on seeking a derivation of the wave patterns observed in the electron double slit experiment, questioning the relevance of wave-particle duality. Participants reference a previous thread on wave-matter duality and suggest familiarity with classical electrodynamics and optics as foundational knowledge. They mention that nonrelativistic quantum theory parallels classical diffraction theory through the Helmholtz equation and Green's function. An alternative approach using path integrals, as detailed in Feynman and Hibbs' work, is also recommended. The conversation concludes with a user expressing gratitude for the helpful resources shared.
Ghost Quartz
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I'm looking for a good derivation of the "wave" patterns in this experiment. I suppose that if wave-particle duality is an obsolete idea, there must be a derivation from quantum mechanics that gets close results.
Thanks in advance
 
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There was a thread recently called "Is wave-matter duality a proven theory" which involved a discussion about this, with some links.

That might be interesting.
 
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How familiar are you with the description of diffraction in classical electrodynamics/optics? In nonrelativistic QT it's almost the same theory, based on the Helmholtz equation and the corresponding Green's function given the boundary conditions due to the slits.

An alternative also pretty intuitive way is the use of the path integral. This is nicely worked out in the book by Feynman and Hibbs.
 
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the link posted by DrChinese is what I was looking for. Thank you, everyone!
 
For the quantum state ##|l,m\rangle= |2,0\rangle## the z-component of angular momentum is zero and ##|L^2|=6 \hbar^2##. According to uncertainty it is impossible to determine the values of ##L_x, L_y, L_z## simultaneously. However, we know that ##L_x## and ## L_y##, like ##L_z##, get the values ##(-2,-1,0,1,2) \hbar##. In other words, for the state ##|2,0\rangle## we have ##\vec{L}=(L_x, L_y,0)## with ##L_x## and ## L_y## one of the values ##(-2,-1,0,1,2) \hbar##. But none of these...