Search NASA⌕ Search

DOE OSTI · 1701049

Materials Data on Cs3Sm7Te12 by Materials Project

Abstract

Cs3Sm7Te12 crystallizes in the orthorhombic Pmn2_1 space group. The structure is three-dimensional. there are three inequivalent Cs1+ sites. In the first Cs1+ site, Cs1+ is bonded in a 7-coordinate geometry to seven Te2- atoms. There are a spread of Cs–Te bond distances ranging from 3.89–4.02 Å. In the second Cs1+ site, Cs1+ is bonded in a 7-coordinate geometry to seven Te2- atoms. There are a spread of Cs–Te bond distances ranging from 3.79–4.04 Å. In the third Cs1+ site, Cs1+ is bonded in a 6-coordinate geometry to six Te2- atoms. There are a spread of Cs–Te bond distances ranging from 3.75–4.24 Å. There are seven inequivalent Sm3+ sites. In the first Sm3+ site, Sm3+ is bonded to six Te2- atoms to form a mixture of edge and corner-sharing SmTe6 octahedra. The corner-sharing octahedral tilt angles are 1°. There are a spread of Sm–Te bond distances ranging from 3.10–3.28 Å. In the second Sm3+ site, Sm3+ is bonded to six Te2- atoms to form a mixture of edge and corner-sharing SmTe6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are a spread of Sm–Te bond distances ranging from 3.09–3.27 Å. In the third Sm3+ site, Sm3+ is bonded to six Te2- atoms to form a mixture of edge and corner-sharing SmTe6 octahedra. The corner-sharing octahedra tilt angles range from 1–9°. There are a spread of Sm–Te bond distances ranging from 3.09–3.24 Å. In the fourth Sm3+ site, Sm3+ is bonded to six Te2- atoms to form a mixture of edge and corner-sharing SmTe6 octahedra. The corner-sharing octahedra tilt angles range from 0–10°. There are a spread of Sm–Te bond distances ranging from 3.09–3.25 Å. In the fifth Sm3+ site, Sm3+ is bonded to six Te2- atoms to form a mixture of edge and corner-sharing SmTe6 octahedra. The corner-sharing octahedra tilt angles range from 9–10°. There are a spread of Sm–Te bond distances ranging from 3.11–3.19 Å. In the sixth Sm3+ site, Sm3+ is bonded to six Te2- atoms to form edge-sharing SmTe6 octahedra. There are a spread of Sm–Te bond distances ranging from 3.11–3.28 Å. In the seventh Sm3+ site, Sm3+ is bonded to six Te2- atoms to form edge-sharing SmTe6 octahedra. There are a spread of Sm–Te bond distances ranging from 3.08–3.30 Å. There are twelve inequivalent Te2- sites. In the first Te2- site, Te2- is bonded in a 5-coordinate geometry to two equivalent Cs1+ and three Sm3+ atoms. In the second Te2- site, Te2- is bonded to two equivalent Cs1+ and three Sm3+ atoms to form distorted TeCs2Sm3 square pyramids that share corners with two equivalent TeCsSm4 trigonal bipyramids, edges with four TeSm5 square pyramids, and an edgeedge with one TeCsSm4 trigonal bipyramid. In the third Te2- site, Te2- is bonded in a 6-coordinate geometry to three Cs1+ and three Sm3+ atoms. In the fourth Te2- site, Te2- is bonded to two equivalent Cs1+ and three Sm3+ atoms to form distorted TeCs2Sm3 square pyramids that share corners with four TeSm5 square pyramids, corners with three TeCsSm4 trigonal bipyramids, edges with three TeSm5 square pyramids, and edges with two equivalent TeCs2Sm3 trigonal bipyramids. In the fifth Te2- site, Te2- is bonded in a 6-coordinate geometry to three Cs1+ and three Sm3+ atoms. In the sixth Te2- site, Te2- is bonded in a 5-coordinate geometry to two equivalent Cs1+ and three Sm3+ atoms. In the seventh Te2- site, Te2- is bonded to one Cs1+ and four Sm3+ atoms to form distorted TeCsSm4 trigonal bipyramids that share corners with two equivalent TeCs2Sm3 square pyramids, corners with three TeCsSm4 trigonal bipyramids, and edges with two equivalent TeSm5 square pyramids. In the eighth Te2- site, Te2- is bonded to one Cs1+ and four Sm3+ atoms to form distorted TeCsSm4 trigonal bipyramids that share corners with three TeCs2Sm3 square pyramids, corners with three TeCsSm4 trigonal bipyramids, edges with three TeSm5 square pyramids, and edges with two equivalent TeCs2Sm3 trigonal bipyramids. In the ninth Te2- site, Te2- is bonded to five Sm3+ atoms to form TeSm5 square pyramids that share corners with two equivalent TeCs2Sm3 square pyramids, corners with two equivalent TeCs2Sm3 trigonal bipyramids, edges with three TeSm5 square pyramids, and edges with two equivalent TeCsSm4 trigonal bipyramids. In the tenth Te2- site, Te2- is bonded to five Sm3+ atoms to form TeSm5 square pyramids that share corners with two equivalent TeCs2Sm3 square pyramids, corners with two equivalent TeCs2Sm3 trigonal bipyramids, edges with four TeSm5 square pyramids, and edges with three TeCsSm4 trigonal bipyramids. In the eleventh Te2- site, Te2- is bonded to two equivalent Cs1+ and three Sm3+ atoms to form distorted TeCs2Sm3 trigonal bipyramids that share corners with four TeSm5 square pyramids, edges with three TeSm5 square pyramids, and edges with four TeCsSm4 trigonal bipyramids. In the twelfth Te2- site, Te2- is bonded in a 5-coordinate geometry to two equivalent Cs1+ and three Sm3+ atoms.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-05-02. Materials Data on Cs3Sm7Te12 by Materials Project. https://doi.org/10.17188/1701049

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related reports

Cyclic moisture reactivation of calcium sorbents for long duration thermochemical energy storage

The transition to a flexible and reliable energy infrastructure, using electro-thermal energy generation technologies such as geothermal, concentrated solar power, and nuclear, usually demands simultaneous advancement of thermal energy storage (TES) to support on-demand electricity generation and industrial applications while mitigating the inherent intermittency of renewable energy sources and power outages from direct energy generation. Among TES technologies, thermochemical energy storage (TCES) based on calcium looping emerges as a compelling high-power energy storage candidate due to its high reaction enthalpy, compatibility with elevated operating temperatures, and abundance of low-cost materials. However, the long-term durability of calcium-based sorbents for TCES is hindered by surface sintering and particle aggregation, leading to performance degradation over repeated thermal cycles. This study explores a moisture hydration-based strategy to regenerate a degraded calcium sorbent and mitigate performance degradation for long duration TCES. The addition of moisture transforms calcium oxide into calcium hydroxide and produces intercalation water layers, associated with a regenerated surface area and reduced calcium oxide crystallite size. Both these effects are beneficial in restoring the sorbents' reactivity for carbonization. Additionally, an optimized hydration-assisted reactivation protocol balances the recovered energy storage capacity with heating penalty required for moisture removal from hydrated samples, resulting in an enhanced energy storage capacity up to 176% compared to benchmark sorbents that undergo cycling without reactivation after 60 cycles. In conclusion, these results highlight the potential of hydration-assisted reactivation to enhance the long-term performance of TCES, providing an effective pathway to advancing electro-thermal storage technologies.

36 MATERIALS SCIENCE↗