A few questions on quantum physics

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SUMMARY

This discussion focuses on determining the wave function of a particle, specifically the muon, using the Schrödinger Equation. It emphasizes the concept of wave-particle duality, highlighting that a particle behaves as a wave until observed, leading to the collapse of the wave function into a specific eigenstate. The conversation also touches on the complexities of measurement in quantum mechanics, referencing the Copenhagen Interpretation and the role of energy infusion during observation. The discussion is framed from the perspective of a college freshman, providing foundational insights into quantum physics.

PREREQUISITES
  • Understanding of the Schrödinger Equation in quantum mechanics
  • Familiarity with wave-particle duality concepts
  • Knowledge of eigenstates and eigenfunctions in linear differential equations
  • Basic grasp of the Copenhagen Interpretation of quantum mechanics
NEXT STEPS
  • Study the mathematical formulation of the Schrödinger Equation
  • Explore the implications of wave-particle duality in quantum mechanics
  • Investigate the measurement problem and the role of observation in quantum systems
  • Learn about other quantum equations such as the Pauli, Klein-Gordon, and Dirac equations
USEFUL FOR

Students of physics, particularly those studying quantum mechanics, as well as educators and enthusiasts seeking to deepen their understanding of wave functions and the nature of particles.

beatlemaniacj
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One; how to determine a wave function of a particle ( let's use the muon as an example)

Two; an explanation of wave particle duality with reference to the Airy experiment and the fact that a particle is a wave until observed by a human.
 
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I'm new to quantum physics, too. But here is my take:
One. For a nonrelativistical particle, assuming only one, the wave equation can be solved using Schroedinger Equation, given a certain potential energy distribution. Many times, there are many eigensolutions to Schroedinger Equation, given a potential. In this case, these eigensolutions form a vector space of solutions (Schroedinger Equation is a linear differential equation after all), and any linear combinations of these solutions can be a solution. With certain boundary conditions, one can often determine a unique solution. Each eigenstate composing the entire solution has a certain probability showing up when a measurement is made, where the probability is the magnitude square of its linear coefficient, given that all eigenfunctions are normalized.

Two. I'm not sure whether what you said was completely right. After all, definitions of a "particle" or a "wave" are ill-defined. But if you want to attribute "existing everywhere" to a wave and "being local" to a particle, then as I mentioned above, before a measurement, a particle doesn't have a definite position or energy or any macroscopic physics parameter. That's wave-like. After a measurement, you've collapsed the wave function, thus only one eigenstate will describe the behavior of the particle. This is particle-like. As for why do measurements have such "magical" powers to a particle, this is still a open question. Classical Copenhagen Interpretation explains measurement problem this way: when a measurement happens macroscopic observation devices will have to infuse new energy to the system, thereby localizing a particle's physical property. But does infusing new energy cause the collapse of wave function? I am confused, too. Maybe I will learn it next year.

--Only a college freshman speaking. Hopefully this helps.
 
One: usually you have an equation like Schrödinger eq., Pauli eq., Klein-Gordon eq., Dirac eq. etc. which contains both the wave function and coupling terms like a potential, an el.-mag. field, etc. In non-relativistic or relativistic QM the wave function is a solution of such an equation.
 

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