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Materials Data on Na3Bi by Materials Project

Na3Bi is Sodium arsenide structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are two inequivalent Na sites. In the first Na site, Na is bonded in a 1-coordinate geometry to four equivalent Bi atoms. There are one shorter (3.25 Å) and three longer (3.56 Å) Na–Bi bond lengths. In the second Na site, Na is bonded in a trigonal planar geometry to three equivalent Bi atoms. All Na–Bi bond lengths are 3.17 Å. Bi is bonded in a 5-coordinate geometry to eleven Na atoms.

36 MATERIALS SCIENCE↗

Materials Data on Na3Bi(BO3)2 by Materials Project

Na3Bi(BO3)2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are three inequivalent Na1+ sites. In the first Na1+ site, Na1+ is bonded in a 4-coordinate geometry to four O2- atoms. There are a spread of Na–O bond distances ranging from 2.28–2.46 Å. In the second Na1+ site, Na1+ is bonded in a 4-coordinate geometry to four O2- atoms. There are a spread of Na–O bond distances ranging from 2.25–2.48 Å. In the third Na1+ site, Na1+ is bonded in a trigonal pyramidal geometry to four O2- atoms. There are a spread of Na–O bond distances ranging from 2.21–2.37 Å. There are two inequivalent B3+ sites. In the first B3+ site, B3+ is bonded in a trigonal planar geometry to three O2- atoms. There is two shorter (1.39 Å) and one longer (1.41 Å) B–O bond length. In the second B3+ site, B3+ is bonded in a trigonal planar geometry to three O2- atoms. There are a spread of B–O bond distances ranging from 1.38–1.40 Å. Bi3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Bi–O bond distances ranging from 2.32–2.93 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a 1-coordinate geometry to two Na1+, one B3+, and two equivalent Bi3+ atoms. In the second O2- site, O2- is bonded in a 1-coordinate geometry to two Na1+, one B3+, and one Bi3+ atom. In the third O2- site, O2- is bonded in a 1-coordinate geometry to two Na1+, one B3+, and one Bi3+ atom. In the fourth O2- site, O2- is bonded in a distorted single-bond geometry to three Na1+, one B3+, and one Bi3+ atom. In the fifth O2- site, O2- is bonded in a 1-coordinate geometry to one Na1+, one B3+, and two equivalent Bi3+ atoms. In the sixth O2- site, O2- is bonded in a 4-coordinate geometry to two Na1+, one B3+, and one Bi3+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Na3Bi by Materials Project

Na3Bi is alpha bismuth trifluoride structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. there are two inequivalent Na sites. In the first Na site, Na is bonded to four equivalent Na and four equivalent Bi atoms to form a mixture of distorted edge, face, and corner-sharing NaNa4Bi4 tetrahedra. All Na–Na bond lengths are 3.34 Å. All Na–Bi bond lengths are 3.34 Å. In the second Na site, Na is bonded in a 8-coordinate geometry to eight equivalent Na and six equivalent Bi atoms. All Na–Bi bond lengths are 3.85 Å. Bi is bonded in a body-centered cubic geometry to fourteen Na atoms.

36 MATERIALS SCIENCE↗

Progress in Epitaxial Thin-Film Na 3 Bi as a Topological Electronic Material

Trisodium bismuthide (Na 3 Bi) is the first experimentally verified topological Dirac semimetal, and is a 3D analogue of graphene hosting relativistic Dirac fermions. Its unconventional momentum-energy relationship is interesting from a fundamental perspective, yielding exciting physical properties such as chiral charge carriers, the chiral anomaly, and weak anti-localization. It also shows promise for realizing topological electronic devices such as topological transistors. Herein, an overview of the substantial progress achieved in the last few years on Na 3 Bi is presented, with a focus on technologically relevant large-area thin films synthesized via molecular beam epitaxy. Key theoretical aspects underpinning the unique electronic properties of Na 3 Bi are introduced. Next, the growth process on different substrates is reviewed. Spectroscopic and microscopic features are illustrated, and an analysis of semiclassical and quantum transport phenomena in different doping regimes is provided. Furthermore, the emergent properties arising from confinement in two dimensions, including thickness-dependent and electric-field-driven topological phase transitions, are addressed, with an outlook toward current challenges and expected future progress.

36 MATERIALS SCIENCE↗