252 Chapter Seven
the various electrons are coupled together into a single resultant L. The spin angular mo-
menta Siare also coupled together into another single resultant S. The momenta Land
Sthen interact via the spin-orbit effect to form a total angular momentum J. This scheme,
called LS coupling,can be summarized as follows:
L Li
LScoupling S Si (7.19)
JLS
The angular momentum magnitudes L,S,Jand their zcomponents Lz,Sz, and Jzare
all quantized in the usual ways, with the respective quantum numbers L, S, J, ML,
MS,and MJ. Hence
LL(L1)
LzML
SS(S1)
SzMS
JJ(J1)
JzMJ (7.20)
Both Land MLare always integers or 0, while the other quantum numbers are half-
integral if an odd number of electrons is involved and integral or 0 if an even number
of electrons is involved. When L S, Jcan have 2S1 values; when L S, Jcan
have 2L1 values.
Figure 7.18In the presence of an external magnetic field B,the
total angular-momentum vector Jprecesses about B.
B
The atom
S
Cone traced
out by J
L
J
B B
Figure 7.17The orbital and spin angular-momentum vectors Land
Sprecess about J.
J
Cone traced out by L
Cone traced out by S
The atom
S
L
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