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In a course that I follow, we use the perturbation method to find the eigenvectors and energies to an Hamiltonian written $ H_0 + V $ where $V$ is a weak perturbation.

It is written that as $V$ is a weak perturbation, we can write the perturbed eigenvectors as a combination of the eigenvectors of the unperturbed hamiltonian.

But I thought that as we know the eigenvectors of the unperturbed Hamiltonian, then we have a basis of the Hilbert space so there is no need of this assumption (we always can write any vector as a linear combination of eigenvectors of the unperturbed hamiltonian).

Can you help me to understand this?

Qmechanic
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StarBucK
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