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Pauli matrices (Definition)

The Pauli matrices are a set of three Hermitian, unitary matrices used by Wolfgang Pauli in his theory of quantum-mechanical spin. They are given by:

$\displaystyle \sigma_1$ $\displaystyle = \begin{pmatrix}0 & 1\\ 1 & 0 \end{pmatrix}$    
$\displaystyle \sigma_2$ $\displaystyle = \begin{pmatrix}0 & -i\\ i & 0 \end{pmatrix}$    
$\displaystyle \sigma_3$ $\displaystyle = \begin{pmatrix}1 & 0\\ 0 & -1 \end{pmatrix}$    

They satisfy the following commutation and anticommutation identities:

$\displaystyle \left[ \sigma_i, \sigma_j \right]$ $\displaystyle = 2i\epsilon_{ijk} \sigma_k$where $ \epsilon_{ijk}$ is the Levi-Civita symbol    
$\displaystyle \lbrace \sigma_i, \sigma_j \rbrace$ $\displaystyle =2 \mathbf{I} \delta_{ij}$   where $ \mathbf{I}$ is the identity matrix and $ \delta_{ij}$ is the Kronecker delta    

Delta notation

With the identity matrix $ \textbf{I}$, the Pauli matrices form a group. When combined in this way, they are often given the symbols $ \delta_i$, as follows:
$\displaystyle \delta_0$ $\displaystyle = \begin{pmatrix}1 & 0\\ 0 & 1 \end{pmatrix}$    
$\displaystyle \delta_1$ $\displaystyle = \begin{pmatrix}0 & 1\\ 1 & 0 \end{pmatrix}$    
$\displaystyle \delta_2$ $\displaystyle = \begin{pmatrix}0 & -i\\ i & 0 \end{pmatrix}$    
$\displaystyle \delta_3$ $\displaystyle = \begin{pmatrix}1 & 0\\ 0 & -1 \end{pmatrix}$    

This choice is useful when writing the Dirac matrices.



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See Also: spinor, Schrödinger's wave equation, unitary group, Hermitian matrix, Dirac matrices, Dirac equation

Other names:  sigma matrices
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Cross-references: Dirac matrices, group, identity matrix, identities, theory, unitary matrices, Hermitian
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This is version 6 of Pauli matrices, born on 2008-03-28, modified 2008-04-17.
Object id is 10449, canonical name is PauliMatrices.
Accessed 577 times total.

Classification:
AMS MSC15A57 (Linear and multilinear algebra; matrix theory :: Other types of matrices )

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