We find stationary excited states of a one-dimensional
system of $N$ spinless point bosons with repulsive interaction and
zero boundary conditions by numerically solving the time-independent
Gross-Pitaevskii equation. The solutions are compared with the exact
ones found in the Bethe-ansatz approach. We show that the $j$th
stationary excited state of a nonuniform condensate of atoms
corresponds to a Bethe-ansatz solution with the quantum numbers
$n_{1}=n_{2}=\ldots =n_{N}=j+1$. On the other hand, such values of
$n_{1},\ldots,n_{N}$ correspond to a condensate of $N$ elementary
excitations (the Bogoliubov quasiparticles) with the quasimomentum
$\hbar \pi j/L$, where $L$ is the system size. Thus, each
stationary excited state of the condensate is \textquotedblleft
doubly coherent\textquotedblright, since it corresponds
simultaneously to a condensate of $N$ atoms and a condensate of $N$
elementary excitations. We find the energy $E$ and the particle
density profile $\rho (x)$ for such states. The possibility of
experimental production of these states is also
discussed.