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\[f(u)=A_0e^{-u^2/2}, g(u)=2uA_1e^{-u^2/2}\] Where both A's have a value so that\[\int\limits_{-\infty}^{\infty}f(u)du=\int\limits_{-\infty}^{\infty}g(u)du=1\] Show that\[A_1=\frac{A_0}{\sqrt{2}}\] From where I'm reading, it says: "Do not evaluate at A_0, but give a value for the particle'smean square position when in the second (quantum) state: \[=\int\limits_{-\infty}^{\infty}u^2g(u)^2du\]"
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Normalize those functions ... using this property |dw:1345989124482:dw|
What does 'do not evaluate at A_0'mean?
I don't know ... most probably ... you are asked to find the weighted averate.
|dw:1345989312374:dw| In this way you can avoid evaluating A_0
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