The Pauli spin matrices
,
and
are central to the representation of spin-
particles in quantum mechanics. Their matrix products are given by
=
where I is the 2⨯2 identity matrix and
, the Levi-Civita permutation symbol. These products lead to the commutation and anticommutation relations
σiσl-σjσi=
ⅈ ϵijkσk and
σiσl+σjσi=2δij{I}, respectively. The Pauli matrices transform as a 3-dimensional pseuodovector (axial vector)
related to the angular-momentum operators for spin-
by
. These, in turn, obey the canonical commutation relations
.
The three Pauli spin matrices, along with the unit matrix I, are generators for the Lie group SU(2).
In
this Demonstration, you can display the products, commutators or
anticommutators of any two Pauli matrices. It is instructive to explore
the combinations
, which represent spin-ladder operators.
Snapshots 1, 2: You can derive the commutation relations for the ladder operators
and
.
Snapshots 3: The Pauli matrices mutually anticommute.
https://demonstrations.wolfram.com/PauliSpinMatrices/
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