Commutation of angular momentum operators

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The discussion focuses on proving that the angular momentum operators Lx and Ly do not commute, specifically showing that [Lx, Ly] = i(h-cross)Lz. The definitions of the operators Lx, Ly, and Lz are provided, highlighting their dependence on partial derivatives. Participants discuss using commutator identities to simplify the calculations. The conversation emphasizes the importance of understanding the non-commutativity of these operators in quantum mechanics. The proof ultimately illustrates the fundamental relationships between angular momentum components.
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Homework Statement



None of the operators Lz, Ly and Lx commute. Show that [Lx,Ly] = i(h-cross)Lz


Homework Equations



Where Lx is defined as Lx=-ih ( y delta/delta x - z delta/delta y)
Where Ly is defined as Ly=-ih ( z delta/delta x - x delta/delta z)
Where Lz is defined as Lz=-ih ( x delta/delta y - y delta/delta x)

The Attempt at a Solution

 
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Use the following commutator identities:

<br /> \begin{align*}<br /> &amp; [A,B+C]=[A,B]+[A,C]<br /> \\<br /> &amp; [A,BC]=[A,B]C+B[A,C]<br /> \end{align*}<br />
 

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