We investigate the properties of a three-dimensional homogeneous dipolar Bosegas in a weak random potential with a Gaussian correlation function at finitetemperature. Using the Bogoliubov theory (beyond the mean field), we calculatethe superfluid and the condensate fractions in terms of the interactionstrength on the one hand and in terms of the width and the strength of thedisorder on the other. The influence of the disordered potential on the secondorder correlation function, the ground state energy and the chemical potentialis also analyzed. We find that for fixed strength and correlation length of thedisorder potential, the dipole-dipole interaction leads to modify both thecondensate and the superfluid fractions. We show that for a strong disorderstrength the condensed fraction becomes larger than the superfluid fraction. Wediscuss the effect of the trapping potential on a disordered dipolar Bose inthe regime of large number of particles.
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