1. Projection
Consider , where the unperturbed states satisfy
. We partition the Hilbert space using projection operators
and
.
Adopting intermediate normalization , the exact state
is decomposed as:
2. Wavefunction
From the Schrödinger equation , projecting onto
yields the recursive relation
. By substituting this relation into the exact state decomposition:
We can iteratively substitute this expression for back into the right-hand side. The first iteration yields:
By continuing this process, we obtain the infinite series expansion in terms of the unperturbed state :
3. Energy Correction
The energy shift is given by . Substituting the series for
into this expression, we can derive the corrections at various orders:
-
First-order correction:
-
Second-order correction:
Note: In Brillouin-Wigner theory, the energy appears on both sides of the equation, making it an implicit equation that typically requires numerical methods to solve.
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