Search NASA⌕ Search

SEARCH · Search NASA

Results for “Se-V”

Search indexed NASA NTRS and DOE OSTI research on propulsion, heat transfer, battery materials and energy systems. Follow report and document links to the original sources.

Quote a phrase for an exact phrase match. Source license links do not imply unrestricted reuse.

Negative linear compressibility in Se at ultra-high pressure above 120 GPa

A series of in situ synchrotron X-ray diffraction (XRD) measurements were carried out, combined with first-principles calculations, to study structural phase transitions of selenium at high pressures and room temperature. Several phase transitions were observed, among which an isostructural phase transition was found at around 120 GPa for the first time. Evolved from the rhombohedral (space group R$\bar{3}$m) structure (Se-V), the new phase (Se-V') exhibited an interesting increase of lattice parameter a at pressures from 120 to 148 GPa, known as negative linear compressibility (NLC). The discovery of NLC behavior observed in this work is mainly attributed to the accuracy and fine steps controlled by the membrane system for in situ XRD data collected with an exposure time of 0.5 s. After 140 GPa, a body-centered cubic (b.c.c.) structure Se-VI (space group Im$\bar{3}$m) was formed, which remains stable up to 210 GPa, the highest pressure achieved in this study. The bulk moduli of phases Se-V, Se-V' and Se-VI were estimated to be 83 ± 2, 321 ± 2 and 266 ± 7 GPa, respectively, according to the P–V curve fit by the third-order Birch–Murnaghan equation of state. The Se-V' phase shows a bulk modulus almost 4 times larger than that of the Se-V phase, which is mainly due to the effect of its NLC. NLC in a higher pressure range is always more significant in terms of fundamental mechanism and new materials discovery, yet it has barely been reported at pressures above 100 GPa. This will hopefully inspire future studies on potential NLC behaviors in other materials at ultra-high pressure.

36 MATERIALS SCIENCE↗

Materials Data on V3Se4 by Materials Project

V3Se4 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent V+2.67+ sites. In the first V+2.67+ site, V+2.67+ is bonded to six Se2- atoms to form a mixture of distorted edge, face, and corner-sharing VSe6 octahedra. The corner-sharing octahedra tilt angles range from 51–57°. There are a spread of V–Se bond distances ranging from 2.44–2.77 Å. In the second V+2.67+ site, V+2.67+ is bonded to six Se2- atoms to form a mixture of edge, face, and corner-sharing VSe6 octahedra. The corner-sharing octahedra tilt angles range from 51–57°. There are two shorter (2.53 Å) and four longer (2.58 Å) V–Se bond lengths. There are two inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a 4-coordinate geometry to four V+2.67+ atoms. In the second Se2- site, Se2- is bonded in a 5-coordinate geometry to five V+2.67+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on V2Se9 by Materials Project

V2Se9 crystallizes in the monoclinic C2/c space group. The structure is one-dimensional and consists of two V2Se9 ribbons oriented in the (1, 0, 1) direction. V5+ is bonded in a 8-coordinate geometry to eight Se+1.11- atoms. There are a spread of V–Se bond distances ranging from 2.53–2.64 Å. There are five inequivalent Se+1.11- sites. In the first Se+1.11- site, Se+1.11- is bonded in a distorted single-bond geometry to one V5+ atom. In the second Se+1.11- site, Se+1.11- is bonded in a 2-coordinate geometry to two equivalent V5+ atoms. In the third Se+1.11- site, Se+1.11- is bonded in a 2-coordinate geometry to two equivalent V5+ atoms. In the fourth Se+1.11- site, Se+1.11- is bonded in a 2-coordinate geometry to two equivalent V5+ atoms. In the fifth Se+1.11- site, Se+1.11- is bonded in a distorted L-shaped geometry to two equivalent V5+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on VSe by Materials Project

VSe is Molybdenum Carbide MAX Phase-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. V2+ is bonded to six equivalent Se2- atoms to form a mixture of edge, face, and corner-sharing VSe6 octahedra. The corner-sharing octahedral tilt angles are 49°. All V–Se bond lengths are 2.61 Å. Se2- is bonded in a 6-coordinate geometry to six equivalent V2+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on VSe by Materials Project

VSe is Tungsten Carbide-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. V2+ is bonded to six equivalent Se2- atoms to form a mixture of distorted edge and corner-sharing VSe6 pentagonal pyramids. All V–Se bond lengths are 2.63 Å. Se2- is bonded to six equivalent V2+ atoms to form a mixture of edge, face, and corner-sharing SeV6 octahedra. The corner-sharing octahedral tilt angles are 45°.

36 MATERIALS SCIENCE↗

Materials Data on VSe by Materials Project

VSe is Vulcanite structured and crystallizes in the tetragonal P4/nmm space group. The structure is two-dimensional and consists of one VSe sheet oriented in the (0, 0, 1) direction. V2+ is bonded in a 4-coordinate geometry to four equivalent Se2- atoms. All V–Se bond lengths are 2.50 Å. Se2- is bonded in a 4-coordinate geometry to four equivalent V2+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on VSe2 by Materials Project

VSe2 is trigonal omega structured and crystallizes in the trigonal P-3m1 space group. The structure is two-dimensional and consists of one VSe2 sheet oriented in the (0, 0, 1) direction. V4+ is bonded to six equivalent Se2- atoms to form edge-sharing VSe6 octahedra. All V–Se bond lengths are 2.50 Å. Se2- is bonded in a 3-coordinate geometry to three equivalent V4+ atoms.

36 MATERIALS SCIENCE↗