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The production of the hypertriton nuclei $^{3}_{\Lambda}\mathrm H$ and$^{3}_{\bar{\Lambda}} \overline{\mathrm H}$ has been measured for the firsttime in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV with the ALICEexperiment at LHC energies. The total yield, d$N$/d$y$ $\times\mathrm{B.R.}_{\left( ^{3}_{\Lambda}\mathrm H \rightarrow^{3}\mathrm{He},\pi^{-} \right)} = \left( 3.86 \pm 0.77 (\mathrm{stat.}) \pm0.68 (\mathrm{syst.})\right) \times 10^{-5}$ in the 0-10% most centralcollisions, is consistent with the predictions from a statistical thermal modelusing the same temperature as for the light hadrons. The coalescence parameter$B_3$ shows a dependence on the transverse momentum, similar to the $B_2$ ofdeuterons and the $B_3$ of $^{3}\mathrm{He}$ nuclei. The ratio of yields $S_3$= $^{3}_{\Lambda}\mathrm H$/($^{3}\mathrm{He}$ $\times \Lambda/\mathrm{p}$) wasmeasured to be $S_3$ = 0.60 $\pm$ 0.13 (stat.) $\pm$ 0.21 (syst.) in 0-10%centrality events; this value is compared to different theoretical models. Themeasured $S_3$ is fully compatible with thermal model predictions. The measured$^{3}_{\Lambda}\mathrm H$ lifetime, $ \tau = 181^{+54}_{-39} (\mathrm{stat.})\pm 33 (\mathrm{syst.})\ \mathrm{ps}$ is compatible within 1$\sigma$ with theworld average value.

$^{3}_{\Lambda}\mathrm H$ and $^{3}_{\bar{\Lambda}} \overline{\mathrm H}$ production in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV