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FarticleFysics
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When solving for the spherical harmonic equations of the orbital angular momentum this textbook I'm reading..
Does this mean that there must be a max value of Lz which is denoted by |ll>? Normally the ket would look like |lm>, and since m is maxed at m=l then |ll> is the ket consisting of the eigenvectors for the max values of the orbital angular momentum.
Also how do we know the associated eigenvalues of Lz look like l h_bar?
Does this mean that there must be a max value of Lz which is denoted by |ll>? Normally the ket would look like |lm>, and since m is maxed at m=l then |ll> is the ket consisting of the eigenvectors for the max values of the orbital angular momentum.
Also how do we know the associated eigenvalues of Lz look like l h_bar?