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Materials Data on Li2MoO4 by Materials Project

Li2MoO4 crystallizes in the trigonal P3_2 space group. The structure is three-dimensional. there are twelve inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four LiO4 tetrahedra and corners with four MoO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.96–2.02 Å. In the second Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four LiO4 tetrahedra and corners with four MoO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.98–2.03 Å. In the third Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four LiO4 tetrahedra and corners with four MoO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.97–2.03 Å. In the fourth Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four LiO4 tetrahedra and corners with four MoO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.97–2.01 Å. In the fifth Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four LiO4 tetrahedra and corners with four MoO4 tetrahedra. There is three shorter (1.98 Å) and one longer (2.00 Å) Li–O bond length. In the sixth Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four LiO4 tetrahedra and corners with four MoO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.97–2.03 Å. In the seventh Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four LiO4 tetrahedra and corners with four MoO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.98–2.01 Å. In the eighth Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four LiO4 tetrahedra and corners with four MoO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.96–2.03 Å. In the ninth Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four LiO4 tetrahedra and corners with four MoO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.97–2.00 Å. In the tenth Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four LiO4 tetrahedra and corners with four MoO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.96–2.01 Å. In the eleventh Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four LiO4 tetrahedra and corners with four MoO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.96–2.03 Å. In the twelfth Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four LiO4 tetrahedra and corners with four MoO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.98–2.03 Å. There are six inequivalent Mo6+ sites. In the first Mo6+ site, Mo6+ is bonded to four O2- atoms to form MoO4 tetrahedra that share corners with eight LiO4 tetrahedra. There are a spread of Mo–O bond distances ranging from 1.79–1.81 Å. In the second Mo6+ site, Mo6+ is bonded to four O2- atoms to form MoO4 tetrahedra that share corners with eight LiO4 tetrahedra. There is one shorter (1.79 Å) and three longer (1.80 Å) Mo–O bond length. In the third Mo6+ site, Mo6+ is bonded to four O2- atoms to form MoO4 tetrahedra that share corners with eight LiO4 tetrahedra. All Mo–O bond lengths are 1.80 Å. In the fourth Mo6+ site, Mo6+ is bonded to four O2- atoms to form MoO4 tetrahedra that share corners with eight LiO4 tetrahedra. There is one shorter (1.79 Å) and three longer (1.80 Å) Mo–O bond length. In the fifth Mo6+ site, Mo6+ is bonded to four O2- atoms to form MoO4 tetrahedra that share corners with eight LiO4 tetrahedra. All Mo–O bond lengths are 1.80 Å. In the sixth Mo6+ site, Mo6+ is bonded to four O2- atoms to form MoO4 tetrahedra that share corners with eight LiO4 tetrahedra. There is two shorter (1.79 Å) and two longer (1.80 Å) Mo–O bond length. There are twenty-four inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the second O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the third O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the fourth O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the fifth O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the sixth O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the seventh O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the eighth O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the ninth O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the tenth O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the eleventh O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the twelfth O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the thirteenth O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the fourteenth O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the fifteenth O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the sixteenth O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the seventeenth O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the eighteenth O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the nineteenth O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the twentieth O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the twenty-first O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the twenty-second O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the twenty-third O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom. In the twenty-fourth O2- site, O2- is bonded in a trigonal planar geometry to two Li1+ and one Mo6+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Li2MoO4 by Materials Project

Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

36 MATERIALS SCIENCE↗

Characterization of cubic Li$_{2}$$^{100}$MoO$_4$ crystals for the CUPID experiment

The CUPID Collaboration is designing a tonne-scale, background-free detector to search for double beta decay with sufficient sensitivity to fully explore the parameter space corresponding to the inverted neutrino mass hierarchy scenario. One of the CUPID demonstrators, CUPID-Mo, has proved the potential of enriched Li$_{2}$$^{100}$MoO$_4$ crystals as suitable detectors for neutrinoless double beta decay search. In this work, we characterised cubic crystals that, compared to the cylindrical crystals used by CUPID-Mo, are more appealing for the construction of tightly packed arrays. We measured an average energy resolution of (6.7$\pm$0.6) keV FWHM in the region of interest, approaching the CUPID target of 5 keV FWHM. We assessed the identification of $\alpha$ particles with and without a reflecting foil that enhances the scintillation light collection efficiency, proving that the baseline design of CUPID already ensures a complete suppression of this $\alpha$-induced background contribution. We also used the collected data to validate a Monte Carlo simulation modelling the light collection efficiency, which will enable further optimisations of the detector.

100Mo↗