Write with and . Then
while
Equating imaginary parts gives
and equating real parts and differentiating in gives
Thus
This is the hydrodynamic form of the Defocusing nonlinear Schrödinger equation.
For a stationary gas with constant phase, is real and time independent. The field equation reduces to
A positive constant solution obeys , so
The travelling-wave substitution gives
Write
Its real part satisfies
For , the imaginary part also gives
With and a translation chosen so that the notch is centred at zero,
Its limiting modulus is , as required. The same expression at is obtained directly from the second-order equation.
The dark soliton density is
For ,
a stationary notch reaching zero at its centre. For ,
a shallower notch with minimum . Since , the first profile remains fixed and the second translates rigidly to the right at speed .

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