Electron orbits, QM, Exclusion Principle and location

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Discussion Overview

The discussion revolves around the behavior of electrons in quantum mechanics, particularly focusing on their probability distributions, the implications of the Pauli Exclusion Principle, and the effects of measurement on their locations. Participants explore concepts related to wavefunctions, potential barriers, and the nature of electron positioning in quantum systems.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants note that electrons exist in a probability cloud and cannot share spin in the same orbital due to the Pauli Exclusion Principle.
  • One participant questions whether an electron's location after measurement is influenced by its previous position or if it can appear anywhere within its probability cloud.
  • Another participant suggests that measurement in quantum mechanics is controversial and that previous measurements do not necessarily inform future locations of the electron.
  • A participant introduces the concept of an electron encountering a square potential barrier, discussing the probabilities associated with finding the electron in different regions after the barrier.
  • Clarifications are made regarding the behavior of the wavefunction, including the possibility of finding the electron in regions beyond the initial position after it interacts with a potential barrier.
  • There is a mention of different types of waves (incident, reflected, tunneling, and transmission) that contribute to the electron's behavior in quantum mechanics.

Areas of Agreement / Disagreement

Participants express varying interpretations of the electron's behavior upon measurement and its probability distribution, indicating that multiple competing views remain without a clear consensus.

Contextual Notes

The discussion includes assumptions about the nature of wavefunctions and the effects of measurement, which may not be fully resolved. The implications of the Pauli Exclusion Principle and the specifics of quantum tunneling are also noted but not definitively concluded.

Who May Find This Useful

This discussion may be of interest to those studying quantum mechanics, particularly in understanding the implications of measurement, wavefunctions, and electron behavior in potential barriers.

eehiram
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I remember that electrons exist in the probability cloud that corresponds to the orbital they reside in, and according to the Pauli Exclusion Principle, they can't share spin in the same orbital.

According to the Copenhagen interpretation of quantum mechanics, when the wavefunction is collapsed because the electron is observed, is it located near it's previous location the last time it was observed or is it anywhere in the probability cloud? I ask this because I thought the electron can be anywhere in the probability cloud, even despite having previously been observed to be in a specific point.

So perhaps the electron appears at any random place at any time, right?

o| Hiram
 
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I'm not an expert in the field of QM. But it is clear that Measurement in QM is a very big and at times controversial subject. I would guess that the electron would be distributed according to its probability distribution and your previous measurement cannot tell you anything about your next.
 
"So perhaps the electron appears at any random place at any time, right?"...maybe the uncertainty answer this question...now try the example of an electron going to a square potential barrier... there is a probability that the electron will be in other region after the barrier but it is a small probability and if u take the electron over it , the probability is big of finding the electron in the 3rd region and so the transmission coefficient is higher then the reflected coefficeint now if the energy is equal the potential energy ...shroedinger's solution is linear now and so some things changes ... but for me i know there is a transmission coeff. but i am not getting to it ... i keep trying ... hope i helped in some way
 
I think I understood part of it

Let me clarify this: if the electron is in region 1, and goes near a square potential barrier, it might be found in region 2, on the other side of the barrier. If we take the part of the wavefunction that has crossed over, then sometime later it might be found in region 3, also on the other side of the square potential barrier and even farther away from region 1 than region 2?

This would mean that the electron partially might moving consistently in that general direction. This does help me with my original question.

Would part of the wavefunction still be found in region 1 when the wavefunction reaches region 3?

o| Hiram
 
yes absolutely ...because we have incident wave and reflected wave and tunneling wave and transmission wave ...
 

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