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:
The scalar would be the identity matrix.
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:
The tri-vectors are:
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 |
|
|
|
|
e12 |
e31 |
e23 |
e123 |
a.e1 |
|
|
e12 |
-e31 |
|
|
e123 |
e23 |
a.e2 |
|
-e12 |
|
e23 |
|
e123 |
|
e31 |
a.e3 |
|
e31 |
-e23 |
|
e123 |
|
|
e12 |
a.e12 |
e12 |
|
|
e123 |
|
e23 |
-e31 |
|
a.e31 |
e31 |
|
e123 |
|
-e23 |
|
e12 |
|
a.e23 |
e23 |
e123 |
|
|
e31 |
-e12 |
|
|
a.e123 |
e123 |
e23 |
e31 |
e12 |
|
|
|
|
which is equivalent to the table derived here.
Further Reading
Other uses of Pauli Matrix:
Related Concepts:
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