Abstract

We analyze general uncertainty relations and we show that there can exist such pairs of non--commuting observables AA and BB and such vectors that the lower bound for the product of standard deviations ΔAΔA and ΔBΔB calculated for these vectors is zero: ΔA ⋅ ΔB≥0ΔA\,\cdot\,ΔB \geq 0. We show also that for some pairs of non--commuting observables the sets of vectors for which ΔA ⋅ ΔB≥0ΔA\,\cdot\,ΔB \geq 0 can be complete (total). The Heisenberg, Δt ⋅ ΔE≥ℏ/2Δt \,\cdot\, ΔE \geq \hbar/2, and Mandelstam--Tamm (MT), τA ⋅ ΔE≥ℏ/2 τ_{A}\,\cdot \,ΔE \geq \hbar/2, time--energy uncertainty relations (τAτ_{A} is the characteristic time for the observable AA) are analyzed too. We show that the interpretation τA=∞τ_{A} = \infty for eigenvectors of a Hamiltonian HH does not follow from the rigorous analysis of MT relation. We show also that contrary to the position--momentum uncertainty relation, the validity of the MT relation is limited: It does not hold on complete sets of eigenvectors of AA and HH.

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