Set , , and use the gauge reduction of a third-order half-line equation
The spatial differential operator acting on is obtained by replacing with . Its second-derivative coefficient vanishes. The first-derivative coefficient is , and the constant coefficient is . The time derivative supplies , so all constant terms cancel and the remaining equation is .
The transformed initial condition and Dirichlet boundary data are therefore
Compatibility at the corner is preserved. Since , this exponential gauge improves the spatial decay of the initial data, which supports convergence of its Half-range Fourier transform.