To first order, and . Equating real and imaginary parts of the Gross–Pitaevskii equation therefore gives
Differentiate the second equation in time and use the first to eliminate :
For a Fourier mode with , the dispersion relation is
This is the normalized Bogoliubov spectrum. At small wavenumber the positive branch has sound speed ; at large wavenumber it approaches the free-particle quadratic dispersion. The linear frequencies are real, confirming stability of the repulsive uniform bulk.

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