For a localized traveling wave put with , and require at infinity. The modified KdV equation integrates once to . Multiplying by and integrating again gives
A nonzero decaying real solution requires . Separating on the rising or falling half of the wave and using the indicated inverse-hyperbolic-secant integral yields
The signs and translations are arbitrary. Differentiating the sech profile verifies directly. The relevant antiderivative is the inverse hyperbolic secant, since for .
The scaling of the equation suggests , , for . Substitution gives
Integrating in gives the scaled Painlevé II equation
where is an arbitrary integration constant. If the standard normalization is desired, set and . Then and
The direct scaled equation avoids introducing imaginary variables when a real is required.
The given Riccati ansatz is . Differentiating it and substituting for shows
It therefore selects in the preceding scaled Painleve equation. Write . The quadratic terms cancel in the ansatz, leaving
Thus every nonzero solution of the indicated Airy equation gives the local mKdV solution
on intervals where . For example , with constants not both zero, has the required equation. This branch is generally complex and meromorphic; the printed ansatz itself includes . A real on a real interval would require simultaneously and , which is impossible on an interval. Hence this particular ansatz does not furnish a nontrivial real-valued mKdV profile.

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