Collapse of the wave function, help understand

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SUMMARY

The discussion centers on the concept of wave function collapse in quantum mechanics, particularly its mathematical underpinnings and interpretations. Participants highlight the confusion surrounding eigenvectors and the probabilistic nature of wave functions, noting that the wave function does not truly collapse but rather splits into distinguishable branches. Two interpretations are presented: the many-world interpretation, which posits that observers are one of the branches, and the Bohmian interpretation, which suggests that particles end up in one branch. For further mathematical insight, a reference to a specific paper is provided.

PREREQUISITES
  • Understanding of quantum mechanics fundamentals
  • Familiarity with eigenvectors and eigenvalues
  • Basic knowledge of probability theory in quantum contexts
  • Awareness of different interpretations of quantum mechanics
NEXT STEPS
  • Study the mathematical framework of quantum mechanics, focusing on wave functions and their properties
  • Learn about the many-world interpretation and its implications in quantum theory
  • Explore the Bohmian interpretation and its approach to particle behavior
  • Read the paper referenced in the discussion for deeper mathematical insights: http://xxx.lanl.gov/abs/1112.2034
USEFUL FOR

Students in physics, particularly those studying quantum mechanics, as well as educators and researchers seeking to clarify the concept of wave function collapse and its interpretations.

Lengalicious
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Ok so when observed, the wavefunction collapses, can someone delicately explain the maths behind it? Or send me to a page with a coherent explanation, that is followable for a first year undergrad? I've covered Eigenvectors briefly in my algebra course last semester and i find that the explanations focus on some eigenvector stuff but i don't completely understand what an eigenvector is, just how to get an eigen vector/value. All i know is that the wave function decreases with path difference and therefore decreases the probability of the particle being at that particular point. But the fact that randomly when a detector interacts with the particle the wavefunction collapses and it acts as a classical particle is confusing me. Whyy? =(
 
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Lengalicious said:
Ok so when observed, the wavefunction collapses, can someone delicately explain the maths behind it? Or send me to a page with a coherent explanation, that is followable for a first year undergrad? I've covered Eigenvectors briefly in my algebra course last semester and i find that the explanations focus on some eigenvector stuff but i don't completely understand what an eigenvector is, just how to get an eigen vector/value. All i know is that the wave function decreases with path difference and therefore decreases the probability of the particle being at that particular point. But the fact that randomly when a detector interacts with the particle the wavefunction collapses and it acts as a classical particle is confusing me. Whyy? =(
The wave function does not really collapse. It only splits into distinguishable branches, so that any branch does not know about the existence of the others. The right question is why can't we see all the branches at once?

One possible answer is - because we ARE one of the branches (many-world interpretation).

Another possible answer - because we are made of little particles which end up in one of the branches (Bohmian interpretation).

There are also other possible answers, but nobody knows which one is correct.

If you want more math behind it, see e.g. Sec. 2 of
http://xxx.lanl.gov/abs/1112.2034
 

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