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:
| e1= |
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| e2= |
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| e3= |
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The scalar would be the identity matrix.
| 1= |
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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:
| e1= |
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| e2= |
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| e3= |
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The scalar would be the identity matrix.
| 1= |
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The bivectors can be calculated by multiplying the matrices:
| e1e2= |
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* |
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| e3e1= |
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* |
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| e2e3= |
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* |
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The tri-vector is:
| e1e2e3= |
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* |
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= |
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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 | ||||||||||||||||||||||||||||||||
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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.
Other uses of Pauli Matrix:
Related Concepts:
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| see also: |
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| Correspondence about this page | |
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Terminology and Notation Specific to this page here: |
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