The basis vectors can be represented by matrices, this algebra was worked out independently by Pauli for his work on quantum mechanics, we can define the following equivalents:
The scalar would be the identity matrix.
The bivectors can be calculated by multiplying the matrices:
The tri-vector is:
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 |
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a.e1 |
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a.e2 |
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a.e3 |
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a.e12 |
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a.e31 |
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a.e23 |
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a.e123 |
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which is equivalent to the table derived here.
Further Reading
Other uses of Pauli Matrix:
Related Concepts:
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