Normalizing Wave Functions Over Multiple Regions

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SUMMARY

The discussion focuses on normalizing a wave function for a finite square well potential, specifically the piecewise function defined as \(\Psi(x) = Ae^{k_{1}x}\) for \(x < -a/2\), \(\Psi(x) = C\sin(k_{2}x)\) for \(-a/2 \leq x \leq a/2\), and \(\Psi(x) = De^{-k_{1}x}\) for \(x > a/2\). The normalization condition requires integrating the squared modulus of the wave function across all regions and setting the total equal to 1. The correct approach involves calculating separate integrals for each region and summing them to satisfy the normalization condition.

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SHISHKABOB
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Homework Statement



I need to normalize the following wave function in order to determine the value of the coefficients. This is from the basic finite square well potential.

\Psi(x) = Ae^{k_{1}x},for \ x &lt; -a/2
\Psi(x) = Csin(k_{2}x),for \ -a/2 \leq x \leq a/2
\Psi(x) = De^{-k_{1}x}, for \ x &gt; a/2

Homework Equations



\int\left|\Psi(x)\right|^{2} dx = 1

The Attempt at a Solution



Do I do an integral for each region, with the limits of integration being the boundaries of each region, and that integral normalized to 1 for each of those regions? Or do I add up those integrals with the same limits of integration and then set that equal to 1?
 
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You use the fact that the wavefunction is continuous at each connecting point,
(-a/2), a/2, to write C and D in terms of A.

Then you integrate the piecewise-function squared over the whole interval to tell
you what A should be.

[also this might be a solution to the finite square well but it's not the most general solution, which
allows cos(kx) in the middle as well. <-- totally meant this to be punny
]
 
SHISHKABOB said:
Or do I add up those integrals with the same limits of integration and then set that equal to 1?

This. More explicitly:

$$\int_{-\infty}^{+\infty} {|\Psi|^2 dx} = 1 \\
\int_{-\infty}^{-a/2} {|\Psi_1|^2 dx}
+ \int_{-a/2}^{+a/2} {|\Psi_2|^2 dx}
+ \int_{+a/2}^{+\infty} {|\Psi_3|^2 dx} = 1$$

This is the same thing as if you were to integrate a single function over the entire range from -∞ to +∞, by splitting up that range into three pieces and doing those as separate integrals for whatever reason.
 

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