  The yields of the K*(892)$^{0}$ and $\Phi$(1020) resonances are measured in
Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV through their hadronic
decays using the ALICE detector. The measurements are performed in multiple
centrality intervals at mid-rapidity (|$y$|<0.5) in the transverse-momentum
ranges 0.3 < $p_{\rm T}$ < 5 GeV/$c$ for the K*(892)$^{0}$ and 0.5 < $p_{\rm
T}$ < 5 GeV/$c$ for the $\Phi$(1020). The yields of K*(892)$^{0}$ are
suppressed in central Pb-Pb collisions with respect to pp and peripheral Pb-Pb
collisions (perhaps due to rescattering of its decay products in the hadronic
medium), while the longer lived $\Phi$(1020) meson is not suppressed. These
particles are also used as probes to study the mechanisms of particle
production. The shape of the $p_{\rm T}$ distribution of the $\Phi$(1020)
meson, but not its yield, is reproduced fairly well by hydrodynamic models for
central Pb-Pb collisions. In central Pb-Pb collisions at low and intermediate
$p_{\rm T}$, the p/$\Phi$(1020) ratio is flat in $p_{\rm T}$, while the p/$\pi$
and $\Phi$(1020)/$\pi$ ratios show a pronounced increase and have similar
shapes to each other. These results indicate that the shapes of the $p_{\rm T}$
distributions of these particles in central Pb-Pb collisions are determined
predominantly by the particle masses and radial flow. Finally, $\Phi$(1020)
production in Pb-Pb collisions is enhanced, with respect to the yield in pp
collisions and the yield of charged pions, by an amount similar to the
$\Lambda$ and $\Xi$.
