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Pauli matrices
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=== Classical mechanics === {{Main|Quaternions and spatial rotation}} In [[classical mechanics]], Pauli matrices are useful in the context of the Cayley-Klein parameters.<ref name=Goldstein-1959> {{cite book |last=Goldstein |first=Herbert |year=1959 |title=Classical Mechanics |pages=109β118 |publisher=Addison-Wesley }} </ref> The matrix {{mvar|P}} corresponding to the position <math>\vec{x}</math> of a point in space is defined in terms of the above Pauli vector matrix, :<math>P = \vec{x} \cdot \vec{\sigma} = x\,\sigma_x + y\,\sigma_y + z\,\sigma_z .</math> Consequently, the transformation matrix {{math|''Q{{sub|ΞΈ}}''}} for rotations about the {{mvar|x}}-axis through an angle {{mvar|ΞΈ}} may be written in terms of Pauli matrices and the unit matrix as<ref name=Goldstein-1959/> :<math>Q_\theta = \boldsymbol{1}\,\cos\frac{\theta}{2} + i\,\sigma_x \sin\frac{\theta}{2} .</math> Similar expressions follow for general Pauli vector rotations as detailed above.
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