How certain do we have to get about a particle's position ?

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The discussion centers on the relationship between a particle's position uncertainty and its wavelength, referencing Brian Cox's book *The Quantum Universe*. It establishes that if a particle exists within a range ΔX, this range must be less than one wavelength to avoid probability cancellation. The participant argues that a range less than half a wavelength would be more logical to ensure that probabilities do not cancel out. The foundational formula discussed is (\Delta x)(\Delta p) = h, where h represents Planck's constant, approximately 6.26 × 10-34 Joule seconds.

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i was reading brian cox's book about *the quantum universe *
and he said something interesting
if for instance we know that a particle exists in ΔX , then this delta has to be less than one wavelength * he did it with clocks * to know the probability of its existence somewhere else in the universe , because if it was more than one wavelength , probabilities would cancel each other out at this point that i want to know the probability of the existence of the particle at
but i think it would make more sense if it was actually less than HALF a wavelength , because if my certainty in the position of the particle was less than half a wavelengths , then there is going to be no chance that probabilities will cancel out , right ?
 
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The basic formula is "([itex]\Delta x)(\Delta p)= h[/itex]) where [itex]\Delta x[/itex] is the uncertainty in the position, [itex]\Delta p[/itex] is the uncertainty in the momentum and "h" is "Plank's constant", about [itex]6.26\times 10^{-34}[/itex] "Joule seconds".
 

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