Let . Hermiticity gives
so in the ordered basis ,
For a nondegenerate unperturbed level, the first-order nondegenerate perturbation theory formulas are
The diagonal matrix elements vanish, so both linear energy corrections are zero. The state corrections are
Thus, through linear order,
Normalization changes only at quadratic order.
The characteristic equation is
Hence the imaginary-coupled two-level Hamiltonian has exact energies
Choose a real angle satisfying
Normalized exact eigenstates are
Since
these states and energies reproduce exactly the linear-order perturbative results from part (i).
The exact energies and mixing coefficients contain
As a function of complex , its nearest branch points to the origin occur when its argument vanishes:
Their distance from the expansion point determines the radius of convergence. Therefore
The real-axis perturbation series converges for .

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