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Heisenberg Uncertainty Principle

A fundamental limitation on the precision with which certain pairs of physical properties of a particle, such as position and momentum, can be simultaneously known.
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The statement of the theorem

For any pair of non-commuting Hermitian operators A^\hat{A} and B^\hat{B} representing physical observables, the generalized uncertainty principle states: σAσB12[A^,B^]\sigma_{A} \sigma_{B} \ge \frac{1}{2} | \langle [\hat{A}, \hat{B}] \rangle | Specifically, for position x^\hat{x} and momentum p^\hat{p}: σxσp2\sigma_{x} \sigma_{p} \ge \frac{\hbar}{2} where σA=A^2A^2\sigma_{A} = \sqrt{\langle \hat{A}^2 \rangle - \langle \hat{A} \rangle^2} is the standard deviation.