Heisenberg Uncertainty Principle question

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The discussion centers on determining which of the two unnormalized wave functions, Y1(x) and Y2(x), is more localized in space based on the Heisenberg Uncertainty Principle. To evaluate localization, integrals for the normalization constant A, the expectation values ⟨x⟩ and ⟨x²⟩ are calculated over a finite interval (-L/2 to L/2). The uncertainty in position, Δx, is derived from these values, specifically Δx = √(⟨x²⟩ - ⟨x⟩²). The impact of extending the interval to infinity (L → ∞) on the uncertainty is also considered, highlighting the relationship between wave function behavior and localization. Understanding these calculations is essential for grasping the implications of the Heisenberg Uncertainty Principle in quantum mechanics.
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given 2 unnormalized wave functions:

Y1(x)=e^i(x/m)

Y2(x)=1/2*[e^2i(x/m) + e^3i(x/m) + e^-2i(x/m) + e^-3i(x/m)]

if the positions of the particles were measured, which would be found to be more localized in space? (that is, which has a position known more precisely?)

to my understanding, i understand the principle if you know position specifically, then you know nothing about the momentum, etc.
 
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Hint: Take the x-axis to be of finite extent ( -L/2 \le x \le L/2). this will make all your integrals converge. Then evaluate:

<br /> A = \int_{-L/2}^{L/2}{|\psi(x)|^{2} \, dx}<br />

<br /> A \, \langle x \rangle = \int_{-L/2}^{L/2}{x \, |\psi(x)|^{2} \, dx}<br />

<br /> A \, \langle x^{2} \rangle = \int_{-L/2}^{L/2}{x^{2} \, |\psi(x)|^{2} \, dx}<br />

Then, once you have calcualated \langle x \rangle and \langle x^{2} \rangle, you can evaluate the uncertainty in the position by:

<br /> \Delta x = \sqrt{\langle (\Delta x)^{2} \rangle} = \sqrt{\langle x^{2} \rangle - \langle x \rangle^{2}}<br />

What happens to this number if you set L \rightarrow \infty?
 
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