Total angular momentum quantum number

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In quantum mechanics, the total angular momentum quantum number parameterises the total angular momentum of a given particle, by combining its orbital angular momentum and its intrinsic angular momentum (i.e., its spin).

If s is the particle's spin angular momentum and its orbital angular momentum vector, the total angular momentum j is

\mathbf j = \mathbf s + \boldsymbol {\ell}

The associated quantum number is the main total angular momentum quantum number j. It can take the following range of values, jumping only in integer steps:

|\ell - s| \le j \le \ell + s

where is the azimuthal quantum number (parameterizing the orbital angular momentum) and s is the spin quantum number (parameterizing the spin).

The relation between the total angular momentum vector j and the total angular momentum quantum number j is given by the usual relation (see angular momentum quantum number)

 \Vert \mathbf j \Vert = \sqrt{j \, (j+1)} \, \hbar

the vector's z-projection is given by

j_z = m_j \, \hbar

where mj is the secondary total angular momentum quantum number. It ranges from −j to +j in steps of one. This generates 2j + 1 different values of mj.

The total angular momentum corresponds to the Casimir invariant of the Lie algebra so(3) of the three-dimensional rotation group.

See also[edit]

References[edit]

  • Griffiths, David J. (2004). Introduction to Quantum Mechanics (2nd ed.). Prentice Hall. ISBN 0-13-805326-X. 

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