Remove the common nonzero factor and expand in the small parameter . To first order, the modified Laplacian contributes only its derivatives: its derivative term has the extra factor . The regular perturbation expansion therefore gives
Thus the two residuals are and , respectively. Subscripts after a comma denote partial derivatives. We retain , as appropriate to the oscillatory wave and the elimination below.
Insert the proposed leading relation into the two zeroth-order residuals. It gives
and, since ,
Hence . The same relation is forced by when ; its derivative then automatically gives .
The first-order condition , combined with , gives
Differentiate this expression with respect to and insert it into . The terms cancel, leaving
Thus the compatibility partial differential equation is
It is exactly . Integrating with respect to therefore gives
where the integration constant may be any function of . Conversely, differentiating this last equation with respect to recovers the compatibility equation.
For separation of variables matching the boundary Fourier mode, take with . Because , the reduced ordinary differential equation is
Therefore
The decay of a Fourier mode in a third-order spatial evolution equation requires a sign check: this satisfies the requested limit at positive infinity precisely when . For it remains identically one, while for its amplitude grows exponentially. Hence for those nonpositive values there is no separated solution meeting both prescribed boundary conditions; the printed assumption that is merely real needs this additional restriction for decay.

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