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Quantum Mechanics → The Pauli Matrices
The Pauli MatricesThe Pauli Matrices are a set of 2×2 matrices which are indispensible in quantum mechanics. They are as follows:
They may also be expressed as components of the vector σ as follows:
σ = (σ1, σ2, σ3)
You might also see them referred to as σx, σy and σz. These are exactly the same as σ1, σ2 and σ3, it's simply a different convention for labelling the different components of the vector σ.
Algebraic PropertiesWarning: This section is not written in Plain English!
The Pauli matrices are hermitian and unitary. They have the following commutation and anti-commutation relations:
| [σi, σj] | = | 2iεijk | | {σi, σj} | = | 2δij |
Putting these relations together gives us an equation of what happens when we multiply any two Pauli matrices together:
σi σj = iεijk + δij
| Q | Wait! I don't quite see where you got this equation from! | | A | I
took the commutation [ , ] relation, the anti-commutation
relation { , }, added them together then divided by 2. Why? Because in general for two symbols A and B; commutation means [A, B] = AB - BA, and the anti-commutaion means: {A, B} = AB + BA. So [A, B] + {A, B} = AB - BA + AB + BA = 2AB Dividing this by 2 gives AB. |
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