How can I define what is the wavefunction

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SUMMARY

The wavefunction can be defined as a linear combination of eigenvectors when given eigenvectors V1, V2,...Vn and corresponding energies E1, E2,...En. The construction involves creating an invertible matrix P from the eigenvectors and a diagonal matrix D from the eigenvalues, leading to the operator A represented as A = PDP-1. In quantum physics, if the eigenvectors correspond to a compact self-adjoint operator, any Hilbert space vector can serve as a valid wavefunction. The uniqueness of the coefficients in the linear combination is guaranteed by the orthogonality and normalization of the eigenvectors.

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  • Understanding of linear algebra concepts, particularly eigenvectors and eigenvalues.
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  • Knowledge of quantum mechanics fundamentals, specifically wavefunctions.
  • Ability to manipulate matrices, including invertible matrices and diagonal matrices.
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Mancho
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How can I define what is the wavefunction if I'm given eigenvectors V1, V2,...Vn and energies E1, E2,. ..En.
I know that it must be a linear combination but how about constants?
 
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I'm not expert in physics but in Linear Algebra, If we know the eigenvalues (energies here) and corresponding eigenvectors, we can construct the invertible matrix P, having those eigenvectors as columns, and the diagonal matrix D, having the corresponding eigenvalues on the diagonal then the matrix (operator) itself is given by
[tex]A= PDP^{-1}[/tex].

I'm sure there is something similar for quantum physics.
 


If the eigenvectors pertain to a compact selfadjoint operator, then any Hilbert space vector in which the operator acts can be chosen as a valid <wavefunction>. As for the uniqueness of the constants, well, it's very easy to prove, because the eigenvectors are perpendicular one to another and can be normalized to modulus 1, so that from (the sum in RHS converges weakly to the vector in the LHS)

[tex]\Psi = \sum_k a_k \psi_k[/tex]

it follows that, for example,

[tex]a_3 = \langle \psi_3, \Psi\rangle[/tex]
 

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