Eigenstates of a Particle in a Box at x = a/2?

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SUMMARY

The eigenstates of a particle in a box with boundaries at x = -a/2 and x = a/2 are defined as \varphi_n = \sqrt{\frac{2}{a}} \sin \frac{n \pi (x + a/2)}{a}. This formulation confirms that the eigenstates can be expressed without concern for negative signs, as they do not affect the overall solution. The discussion clarifies that the eigenstates remain valid regardless of the sign in the sine function, reinforcing the robustness of the mathematical representation.

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What are the eigenstates of a particle in a box whose bounds are [tex]x = -a/2[/tex] and [tex]x = a/2[/tex]?

Solution
Well, the eigenstates where [tex]x = 0, a[/tex] are just

[tex]\varphi_n = \sqrt{\frac{2}{a}} \sin \frac{n \pi x}{a}[/tex],

so why wouldn't the eigenstates just be

[tex]\varphi_n = \sqrt{\frac{2}{a}} \sin \frac{n \pi (x+a/2)}{a} = \sqrt{\frac{2}{a}}\sin \left(\frac{n \pi x}{a} + \frac{n \pi}{2}}\right)[/tex]

?
 
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No reason at all; those are the eigenstates!
 
Yes, I just figured out the reason... I was slightly afraid of the negative sign that resulted in my answer for the Sin x solution, but it doesn't matter... negative signs don't have any effect on eigenstates.
 

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