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What's the deal?

In general, if we have two angular momentum operators, tex2html_wrap_inline6257 and tex2html_wrap_inline6259 (where the tex2html_wrap_inline6261 could correspond to the sum of the orbital AM and the spin AM or the spin AM of 2 electrons etc.), we would like to know the possible values of the total AM tex2html_wrap_inline6263 can take where

equation3704

Assuming that tex2html_wrap_inline6257 and tex2html_wrap_inline6259 correspond to distinct degrees of freedom (for example if they correspond to the spin AM of 2 electron), they commute with each other:

equation3710

Together with the AM commutation relations for tex2html_wrap_inline6257 and tex2html_wrap_inline6259 individually, the commutation relations for tex2html_wrap_inline6263 are given by:

equation3716

So all the properties of AM and their eigenstates discussed in the sections above also hold for the total AM.

We start with states tex2html_wrap_inline6275 and tex2html_wrap_inline6277 where the two quantum numbers tex2html_wrap_inline6279 and tex2html_wrap_inline6281 are fixed and the tex2html_wrap_inline6283 take the values tex2html_wrap_inline6285 . The corresponding eigenvalue equations are:

eqnarray3728

From these states we construct the product states

equation3762

which are eigenfunctions of tex2html_wrap_inline6287 with eigenvalue tex2html_wrap_inline6289 but NOT eigenfunctions of tex2html_wrap_inline6291 since

equation3781

for i=1,2. These product states are eigenstates of the operators

equation3786

What we need to do is search for states in which tex2html_wrap_inline6291 is also diagonal; that is, we seek eigenfunctions

equation3791

of the four mutually commuting operators

equation3798

with eigenvalues tex2html_wrap_inline6297 . At the same time we have to find the values taken by j (the corresponding tex2html_wrap_inline6301 are then tex2html_wrap_inline6303 ), and we have to represent tex2html_wrap_inline6305 as a linear combination of the product states above. Before considering the general case, we first look at the addition of two spins and the addition of an orbital AM to a spin.



Gunaretnam Rajagopal
Tue Oct 15 17:55:22 BST 1996