Angular momenta couple.
The simplest scheme (appropriate for light atoms) is known as Russell-Saunders Coupling
Individual spin momenta couple => S = s1+s2, …, |s1-s2|
Individual orbital angular momenta couple => L = l1+l2, …, |l1-l2|
S and L now combine to give a total angular momentum=> J = L+S, …, |L-S|
The are 2S+1 values of J (L>S)=> the spin multiplicity provides an indication of the number of J subcomponents
Term symbols convey information about the configuration of a state
2P3/2 or 3D2
The term symbol gives 3 pieces of information
The letter indicates the total orbital angular quantum number, L.
L 0 1 2 3 4
letter S P D F G
The left superscript gives the multiplicity, 2S+1.
The right subscript is the value of the total angular momentum quantum number, J.
Examples:
d2:
l1 = 2, l2 = 2
l1 + l2 = 4, |l1 - l2| = 0 => L = 4, 3, …, 0 => G, F, D, P, S.
p3:
l1 = 1, l2 = 1, l3 = 1
Couple l1 to l2 => l1 + l2 = 2, |l1 - l2| = 0 => L’ = 2, 1, 0 Couple L’ to l3 L’ = 2 => L = 2+1, …, 1 = 3, 2, 1 L’ = 1 => L = 1+1, …, 0 = 2, 1, 0 L’ = 0 => L = 1+0 = 1 => 1 x F, 2 x D, 3 x P, 1 x S.
Na = [Ne] 3s1
single 3s electron
L = l = 0
S = s = ½
J = ½
=> Term symbol, 2S+1{L}J = 2S½
C = [He] 2s2 2p1 3p1
2p and 3p electrons
l1 + l2 = 2, |l1 - l2| = 0 => L = 2, 1, 0
s1 + s2 = 1, |s1 - s2| = 0 => S = 1, 0
Hence 3D, 1D, 3P, 1P, 3S & 1S
Hence term symbols:
3D: L = 2, S = 1 => J = 3, 2, 1 => 3D3, 3D2, 3D1
1D: L = 2, S = 0 => J = 2 => 1D2
3P: L = 1, S = 1 => J = 2, 1, 0 => 3P2, 3P1, 3P0
1P: L = 1, S = 0 => J = 1 => 1P1
3S: L = 0, S = 1 => J = 1 => 3S1
1S: L = 0, S = 0 => J = 0 => 1S0