Pauli spin matrices: Difference between revisions
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The '''Pauli spin matrices''' are a set of unitary [[Hermitian matrix|Hermitian matrices]] which form an orthogonal basis (along with the identity matrix) for the real [[Hilbert space]] of 2 × 2 Hermitian matrices and for the complex Hilbert spaces of all 2 × 2 matrices. They are usually denoted: | The '''Pauli spin matrices''' (named after physicist [[Wolfgang Ernst Pauli]]) are a set of unitary [[Hermitian matrix|Hermitian matrices]] which form an orthogonal basis (along with the identity matrix) for the real [[Hilbert space]] of 2 × 2 Hermitian matrices and for the complex Hilbert spaces of all 2 × 2 matrices. They are usually denoted: | ||
: <math>\sigma_x=\begin{pmatrix} | : <math>\sigma_x=\begin{pmatrix} |
Revision as of 06:54, 13 October 2008

The Pauli spin matrices (named after physicist Wolfgang Ernst Pauli) are a set of unitary Hermitian matrices which form an orthogonal basis (along with the identity matrix) for the real Hilbert space of 2 × 2 Hermitian matrices and for the complex Hilbert spaces of all 2 × 2 matrices. They are usually denoted:
Algebraic properties
For i = 1, 2, 3:
Commutation relations
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \sigma_2\sigma_3 = i\sigma_1\,\!}
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \sigma_i\sigma_j = -\sigma_j\sigma_i\mbox{ for }i\ne j\,\!}
The Pauli matrices obey the following commutation and anticommutation relations:
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \begin{matrix} [\sigma_i, \sigma_j] &=& 2 i\,\varepsilon_{i j k}\,\sigma_k \\[1ex] \{\sigma_i, \sigma_j\} &=& 2 \delta_{i j} \cdot I \end{matrix}}
- where is the Levi-Civita symbol, Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \delta_{ij}} is the Kronecker delta, and I is the identity matrix.
The above two relations can be summarized as:
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \sigma_i \sigma_j = \delta_{ij} \cdot I + i \varepsilon_{ijk} \sigma_k. \,}