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I'm working in Liboff, 4e, QM, page 114, problem 4.35.
An electron in a 1-D box with walls at x= 0,a is in the state \psi(x) = A for x\in (0,a/2) and \psi(x) = -A for x\in (a/2,a). What is the lowest possible energy that can be measured?
From my understanding, the answer to this question will be the integer of first nonzero coefficient in the expansion \psi = \Sigma \limits_{n=1}^{\infty} a_n \phi_n, where \phi_n = \sqrt{\frac{2}{a}}\sin(\frac{n\pi x}{a}) are the basis functions given in eq (4.15) from the book (the eigenstates for the 1D box Hamiltonian). I do this and I get a_n = \frac{\sqrt{2}}{n\pi}(1+\cos(n\pi) - 2\cos(n\pi/2)). Now correct me if I'm wrong, but is it not true that \psi(x)=A for x\in (0,a) represents the same state since only the square of the wavefunction is given significance? In that case, however, I get a_n=\frac{\sqrt{2}}{n\pi}(1-\cos(n\pi)). It is my understanding that a_n^2 represents the probability of measuring the particle to be in the state \phi_n. But in these two cases, we will get different a_n^2 indicating that the two states are physically different.
Can anyone point out my mistake?
An electron in a 1-D box with walls at x= 0,a is in the state \psi(x) = A for x\in (0,a/2) and \psi(x) = -A for x\in (a/2,a). What is the lowest possible energy that can be measured?
From my understanding, the answer to this question will be the integer of first nonzero coefficient in the expansion \psi = \Sigma \limits_{n=1}^{\infty} a_n \phi_n, where \phi_n = \sqrt{\frac{2}{a}}\sin(\frac{n\pi x}{a}) are the basis functions given in eq (4.15) from the book (the eigenstates for the 1D box Hamiltonian). I do this and I get a_n = \frac{\sqrt{2}}{n\pi}(1+\cos(n\pi) - 2\cos(n\pi/2)). Now correct me if I'm wrong, but is it not true that \psi(x)=A for x\in (0,a) represents the same state since only the square of the wavefunction is given significance? In that case, however, I get a_n=\frac{\sqrt{2}}{n\pi}(1-\cos(n\pi)). It is my understanding that a_n^2 represents the probability of measuring the particle to be in the state \phi_n. But in these two cases, we will get different a_n^2 indicating that the two states are physically different.
Can anyone point out my mistake?