Parity - Particle In A Box (Infinite Potential)

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The discussion focuses on deriving the wavefunctions for a particle in a box with boundaries at -a/2 and a/2. The user compares the solutions for even and odd quantum numbers (n), noting that for even n, the wavefunction simplifies to a sine function, while for odd n, it becomes a cosine function. There is confusion regarding the selection of positive values for the cosine and sine terms, which may relate to normalization. The energy eigenfunctions are discussed, emphasizing that n only holds physical significance for positive integers, with E0 representing the ground state energy. Clarification on these points is sought to resolve the user's confusion.
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I am trying to work out the wavefunctions for a particle in a box between -a/2 and a/2.I have already gone through the solution for a box between 0 and a and got the solution \sqrt{\frac{2}{a}}sin(\frac{n\pi x}{a} )So I can see that for -a/2 to a/2 I have \sqrt{\frac{2}{a}}sin(\frac{n\pi(x+\frac{a}{2})}{a})Which by some trig leads to \sqrt{\frac{2}{a}}sin(\frac{n\pi x}{a})cos(\frac{n\pi}{2})+\sqrt{\frac{2}{a}}cos(\frac{n\pi x}{a})sin(\frac{n\pi}{2})Now i can see it differs for even and odd n as for even n sin(\frac{n\pi}{2})=0 for odd n cos(\frac{n\pi}{2})=0.

(NOT SURE WHATS HAPPENED WITH LATEX HERE :()Therefore even n leads to \sqrt{\frac{2}{a}}sin(\frac{n\pi x}{a})cos(\frac{n\pi}{2}) odd n leads to \sqrt{\frac{2}{a}}cos(\frac{n\pi x}{a})sin(\frac{n\pi}{2})From research I have found that the wavefunction for n even is in fact just \sqrt{\frac{2}{a}}sin(\frac{n\pi x}{a}) and odd n just \sqrt{\frac{2}{a}}cos(\frac{n\pi x}{a})This is were I am confused because the cos(\frac{n\pi}{2}) for even n is positive or negative 1 and sin(\frac{n\pi}{2}) for odd n is positive or negative 1.Why is only the positive chosen, is this to do with normalistion?Any help is much appreciated.Thank you.
 
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n only has physical meaning for positive values because if you evaluate the energy eigenfunctions, you find that

E_n = \frac{n^2 \pi^2 \hbar^2}{2ma^2}

Mathematically, at least, it is unnecessary for n to be less than 0. Going by this equation, E0 is by definition the lowest possible energy state, or ground state.
 

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