I Use of an Essentially Ubiquitous Equation

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The discussion centers around a specific equation in quantum mechanics, which is acknowledged as important in multiple textbooks but has not been observed in practical use by the original poster. The equation relates to the Schrodinger-Pauli equation, which is a key component in quantum mechanics. The poster expresses curiosity about the equation's applications, indicating a gap between theoretical knowledge and practical understanding. The conversation highlights the need for clarity on how foundational equations are utilized in real-world quantum mechanics scenarios. This underscores the importance of bridging theory with application in the study of quantum physics.
topsquark
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TL;DR
I've always seen this equation derived in my QM classes, but I've never actually seen it used.
##( \sigma \cdot \textbf{A} ) ( \sigma \cdot \textbf{B} ) = \textbf{A} \cdot \textbf{B} + i \sigma \cdot ( \textbf{A} \times \textbf{B} )##
I've taken three intro QM classes, and I have four textbooks that cover the derivation of this equation:
##( \sigma \cdot \textbf{A} ) ( \sigma \cdot \textbf{B} ) = \textbf{A} \cdot \textbf{B} + i \sigma \cdot ( \textbf{A} \times \textbf{B} )##

All of them say this equation is very important, but I just realized yesterday that I've never actually seen the thing used.

What is this equation actually used for?

Thanks!

-Dan
 
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renormalize said:
Look at the Schrodinger-Pauli equation: https://en.wikipedia.org/wiki/Pauli_equation
Ah! Yes, I have run into that before, but I never spent much time with it. I never recognized the form.

Thanks!

-Dan
 
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...

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