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Indeed, complementarity can be simply substituted by the clear mathematical statement of the uncertainty principle,
$$\Delta A \Delta B \geq \frac{1}{2} |\langle \mathrm{i} [\hat{A},\hat{B}]|.$$
##A## and ##B## don't necessarily need to be canonically conjugated as are ##x## and ##p_x## but in the latter case it's most simply to discuss, because then ##[\hat{x},\hat{p}_x]=\mathrm{i} \hbar##, and you get
$$\Delta x \Delta p_x \geq \frac{\hbar}{2},$$
which says that if a particle is prepared in a well-localized state (i.e., ##\Delta x## "small") then necessarily ##\Delta p_x## is "large". You don't need complicated philosophical arguments about "complementarity" to understand this.
$$\Delta A \Delta B \geq \frac{1}{2} |\langle \mathrm{i} [\hat{A},\hat{B}]|.$$
##A## and ##B## don't necessarily need to be canonically conjugated as are ##x## and ##p_x## but in the latter case it's most simply to discuss, because then ##[\hat{x},\hat{p}_x]=\mathrm{i} \hbar##, and you get
$$\Delta x \Delta p_x \geq \frac{\hbar}{2},$$
which says that if a particle is prepared in a well-localized state (i.e., ##\Delta x## "small") then necessarily ##\Delta p_x## is "large". You don't need complicated philosophical arguments about "complementarity" to understand this.