Wavefunction in the energy representation

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The discussion revolves around finding the wavefunction in the energy representation for a given superposition of normalized energy eigenfunctions. The participants suggest that the wavefunction can be expressed as a linear combination of energy eigenstates, leading to the formulation |ψ⟩ = (3/5)|E₁⟩ + (4/5)|E₃⟩. They explore the concept of representing the wavefunction as a function of energy, ψ(E), and relate it to the completeness of states. The idea of using delta functions or Kronecker deltas to express probabilities of finding specific energies is also considered. Overall, the conversation highlights the complexities of transitioning between position and energy representations in quantum mechanics.
dave4000
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Homework Statement



\psi(x)=\frac{3}{5}\chi_{1}(x)+\frac{4}{5}\chi_{3}(x)

Both \chi_{1}(x) \chi_{3}(x) are normalized energy eigenfunctions of the ground and second excited states respectivley. I need to find the 'wavefunction in the energy representation'


The Attempt at a Solution



I can find the expectation value of the energy but what is the wavefunction in the energy representation?
 
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It looks like it is given in the energy representation already. Except I'd write it as:

\left|\psi\right> = \frac{3}{5}\left|E_1\right>+\frac{4}{5}\left|E_3\right>
 
I'm not so sure. I think what they are after is \psi(E) i.e. a function of energy. I suppose in analogy with \psi(x) = \left<x|\psi\right> it would be \psi(E) = \left<E|\psi\right>. Completeness of states could be of help. I suspect you should get delta functions.
 
phsopher said:
I'm not so sure. I think what they are after is \psi(E) i.e. a function of energy. I suppose in analogy with \psi(x) = \left<x|\psi\right> it would be \psi(E) = \left<E|\psi\right>. Completeness of states could be of help. I suspect you should get delta functions.
I wouldn't have thought of that, but yeah, that might be it.
 
My guess at what they want: (I think it's the same as what Phsopher said, but possibly a bit more intuitive)

By completeness, you can represent any wave-function:

\Psi (x) = \sum_{n=1}^{\infty} c_n\psi_n(x)

Where the \psi_n represent energy eigenfunctions. The energy representation of the wave function would probably then just be the coefficients c_n at different energies. The probabilities of finding a specific energy would be |c_n|^2. This is a bit weird, because it's not any real function that I can think of (dirac deltas can't really be squared properly...as far as I know...so I don't think ).

I'm sort of stumped on this one too!

EDIT:

Oh, I just thought, maybe instead of using Dirac Deltas, you can use Kronecker deltas...

Perhaps:

\Psi(E) = \frac{3}{5}\delta_{E, E_1} + \frac{4}{5}\delta_{E, E_3}

Not 100% on this though.
 
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