Quantum Measurements of L2 in a Wave Function: Calculations and Probabilities

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Homework Help Overview

The problem involves a particle described by a wave function in quantum mechanics, specifically focusing on the measurement of the operator L2 and its possible values and associated probabilities. The context is rooted in quantum mechanics and wave functions.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to understand how to express the wave function in spherical coordinates and the role of spherical harmonics (Ylm) in the expansion of the wave function. Some participants suggest using Ylm in Cartesian coordinates and refer to the relationship between L2 and the wave function.

Discussion Status

The discussion is ongoing, with participants exploring different aspects of the problem. Some guidance has been offered regarding the use of spherical harmonics and the relationship between L2 and the wave function, but there is no explicit consensus on the next steps or methods to solve the problem.

Contextual Notes

Participants express confusion about the spherical harmonics and their application in this context. There is a mention of potential resources that might clarify the steps involved in the problem.

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Homework Statement


A particle is in a state described by a wave function of the form ψ(r) = (x+y+z)f(r).
What are the values that a measurement of L2 can yield? What is probability for all these results?

Homework Equations

The Attempt at a Solution


I feel this problem shouldn't be too hard but I've been struggling with quantum since last semester so any guidance would be nice. I think i should probably write the function in spherical terms to start off with. but I'm not too clear on where to go from there. I also know that i need to use Ylm too but again, I'm pretty confused.
 
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It will be helpful to use the spherical harmonics written in Cartesian coordinates. Your task is to find ##Y_{lm}##'s in which the given ##\psi(\mathbf{r})## is expanded, $$\psi(\mathbf{r}) = f(r)\sum_{lm} c_{lm} Y_{lm}(\hat{r})$$
 
ok ill try to do some work with that. I'm still pretty lost on what the whole Ylm thing is about but hopefully i can make some sense of it.
 
I don't know what book you're studying out of, but most go through the steps to show that L2Ψ=ħ2l(l+1)Ψ That might help make the problem a bit easier.
 

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