The Pauli matrices σx,σy,σz are traceless Hermitian 2×2 matrices that, together with the identity, form a basis of the complex 2×2 matrices.
The Pauli matrices satisfyConsequently each squares to the identity, distinct Pauli matrices anticommute, and their products span M2(C).
σiσj=δijI+iεijkσk.
The identity follows because the identity matrix and the three Pauli matrices form an orthogonal basis of two-by-two matrices under the trace inner product. It rewrites a spin-vector bilinear square as a scalar four-fermion expression, with the Grassmann signs supplied when fields are reordered. This is the algebra behind a spin-vector Hubbard–Stratonovich decoupling.
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- Chiral gamma-matrix representation
- Elliptic system of differential equations
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