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Maths - Pauli matrices - 4D

The basis vectors can be represented by matrices, this algebra was worked out independently by Pauli for his work on quantum mechanics. Murray Gell-Mann defined an extention of Pauli matricies to 3x3 matricies:

e1=
0 1 0
1 0 0
0 0 0
e2=
0 -i 0
i 0 0
0 0 0
e3=
1 0 0
0 -1 0
0 0 0
e4=
0 0 1
0 0 0
1 0 0
e5=
0 0 -i
0 0 0
i 0 0
e6=
0 0 0
0 0 1
0 1 0
e7=
0 0 0
0 0 -i
0 i 0
e8= 1/√ 3 *
1 0 0
0 1 0
0 0 -2

The scalar would be the identity matrix.

1=
1 0 0
0 1 0
0 0 1

 

The structure constant is antisymmetric in the three indicies and has values:

f123 = 2

f147 = f165 = f246 = f257 = f345 = f376 = 1

f458 = f678 =√ 3

The bivectors can be calculated by multiplying the matrices:

e1e2=
0 1
1 0
*
0 -i
i 0
=
i 0
0 -i
e1e3=
0 1
1 0
*
1 0
0 -1
=
0 -1
1 0
e2e3=
0 -i
i 0
*
1 0
0 -1
=
0 i
i 0

The tri-vectors are:

e1e2e3=
i 0
0 -i
*
1 0
0 -1
=
i 0
0 i

 

So the complete geometric multiplication table is:

a*b
b.e b.e1 b.e2 b.e3 b.e12 b.e31 b.e23 b.e123
a.e
1 0
0 1
0 1
1 0
0 -i
i 0
1 0
0 -1
e12 e31 e23 e123
a.e1
0 1
1 0
1 0
0 1
e12 -e31
0 -i
i 0
-1 0
0 1
e123 e23
a.e2
0 -i
i 0
-e12
1 0
0 1
e23
0 -1
-1 0
e123
1 0
0 -1
e31
a.e3
1 0
0 -1
e31 -e23
1 0
0 1
e123
0 1
1 0
0 i
-i 0
e12
a.e12 e12
0 i
-i 0
0 1
1 0
e123
-1 0
0 -1
e23 -e31
-1 0
0 1
a.e31 e31
1 0
0 -1
e123
0 -1
-1 0
-e23
-1 0
0 -1
e12
0 i
-i 0
a.e23 e23 e123
-1 0
0 1
0 -i
i 0
e31 -e12
-1 0
0 -1
0 -1
-1 0
a.e123 e123 e23 e31 e12
-1 0
0 1
0 i
-i 0
0 -1
-1 0
-1 0
0 -1

which is equivalent to the table derived here.


Further Reading

Other uses of Pauli Matrix:

Related Concepts:


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see also:

 

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