From: A dynamic systems approach to fermions and their relation to spins
M
L = 1
2
3
4
1
su(2)
su(3)+u(1)
su(4)+ ∑ i = 1 2 su(2)+u(1)
su(6)+su(4)+ ∑ i = 1 2 su(2)+u(1)
su(4)+ ∑ i = 1 2 su(2)+ ∑ i = 1 2 u(1)
su(6)+su(4)+ ∑ i = 1 2 su(3)+ ∑ i = 1 3 u(1)
L = 5
6
su(8)+ ∑ i = 1 4 su(6)+u(1)
su(14)+ ∑ i = 1 2 su(11)+su(10)+ ∑ i = 1 2 su(9)+u(1)
su(8)+ ∑ i = 1 4 su(6)+ ∑ i = 1 2 u(1)
su(14)+ ∑ i = 1 2 su(11)+su(10)+ ∑ i = 1 2 su(9)+ ∑ i = 1 3 u(1)
su(8)+ ∑ i = 1 4 su(6)+ ∑ i = 1 4 u(1)
su(14)+ ∑ i = 1 2 su(11)+su(10)+ ∑ i = 1 2 su(9)+ ∑ i = 1 4 u(1)
5
su(14)+ ∑ i = 1 2 su(11)+su(10)+ ∑ i = 1 2 su(9)+ ∑ i = 1 5 u(1)