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Orbital angular momentum and spherical harmonics

Orbital angular momentum is associated with rotational motion in three-dimensional [Pg.144]

Here 6 and 4 are the spherical polar angles (only two angles are required to define the orientation of the vector r in space). Since these operators are the same as the infinitesimal rotation operators, all the results of the previous sections apply. The eigenfunctions of and Lz axe known as the spherical harmonics, [Pg.144]

For a single-valued solution, m must be an integer (and so therefore must ). The functions 0fa(6 ) can be found by solving [Pg.145]

The spherical harmonics are normalised with respect to integration [Pg.145]

The explicit forms of the first few spherical harmonics are given in table 5.1. It is sometimes more convenient to use modified spherical harmonics C j, defined by [Pg.145]

Orbital angular momentum is associated with rotational motion in three-dimensional space. In terms of the operators representing the position r and linear momentum p of a particle, we have the important expression for the orbital angular momentum [Pg.144]


See other pages where Orbital angular momentum and spherical harmonics is mentioned: [Pg.144]    [Pg.144]   


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