oxygen framework
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Author(s):  
Pengfei Wang ◽  
Yan Meng ◽  
Yujue Wang ◽  
Lu Chen ◽  
Zhaokun Zhang ◽  
...  

Author(s):  
Bingkai Zhang ◽  
Zhiwei He ◽  
Jiajie Zhong ◽  
Luyi Yang ◽  
Zhan Lin ◽  
...  

Li10MP2S12 (LMPS, M = Ge, Sn, or Si) share an underlying body-centered cubic (bcc) anion framework enabling their high Li-ion conductivity. To take full use of the high conductivity of...


2019 ◽  
Vol 46 (9) ◽  
pp. 4971-4979 ◽  
Author(s):  
C. C. Womack ◽  
E. E. McDuffie ◽  
P. M. Edwards ◽  
R. Bares ◽  
J. A. Gouw ◽  
...  

MRS Advances ◽  
2019 ◽  
Vol 4 (14) ◽  
pp. 813-820 ◽  
Author(s):  
Marnik Bercx ◽  
Levi Slap ◽  
Bart Partoens ◽  
Dirk Lamoen

ABSTRACTLithium-rich layered oxides such as Li2MnO3 have shown great potential as cathodes in Li-ion batteries, mainly because of their large capacities. However, these materials still suffer from structural degradation as the battery is cycled, reducing the average voltage and capacity of the cell. The voltage fade is believed to be related to the migration of transition metals into the lithium layer, linked to the formation of O-O dimers with a short bond length, which in turn is driven by the presence of oxygen holes due to the participation of oxygen in the redox process. We investigate the formation of O-O dimers for partially charged O1-Li2MnO3 using a first-principles density functional theory approach by calculating the reaction energy and kinetic barriers for dimer formation. Next, we perform similar calculations for partially charged O1-Li2IrO3, a Li-rich material for which the voltage fade was not observed during cycling. When we compare the stability of the oxygen framework, we conclude that the formation of O-O dimers is both thermodynamically and kinetically viable for O1-Li0.5MnO3. For O1-Li0.5IrO3, we observe that the oxygen lattice is much more stable, either returning to its original state when perturbed, or resulting in a structure with an O-O dimer that is much higher in energy. This can be explained by the mixed redox process for Li2IrO3, which is also shown from the calculated magnetic moments. The lack of O-O dimer formation in O1-Li0.5IrO3 provides valuable insight as to why Li2IrO3 does not demonstrate a voltage fade as the battery is cycled, which can be used to design Li-rich battery cathodes with an improved cycling performance.


2018 ◽  
Vol 386 ◽  
pp. 149-155 ◽  
Author(s):  
Maria Knjazeva ◽  
Yurii Bronwald ◽  
Daria Andronikova ◽  
Georgiy Lityagin ◽  
Alexey Bosak ◽  
...  

Lead hafnate single crystals were characterized using single crystal x-ray diffraction under simultaneous application of hydrostatic pressure and high temperatures. The information on the structure of two intermediate phases, situated between antiferroelectric and paraelectric phases in the pressure-temperature phase diagram, has been obtained. The lower-temperature intermediate phase is characterized by incommensurate displacive modulations in Pb sublattice. The higher-temperature intermediate phase is characterized by oxygen framework distortion, primarily in the form of anti-phase tilts of the oxygen octahedra, which is also present in the lower-temperature intermediate phase.


2017 ◽  
Vol 72 (3) ◽  
pp. 215-223
Author(s):  
Teresa S. Ortner ◽  
Daniel Schildhammer ◽  
Martina Tribus ◽  
Bastian Joachim ◽  
Hubert Huppertz

AbstractThree novel mixed alkali borate-nitrates Na3−xKx[B6O10]NO3(x=0.5, 0.6, 0.7) were synthesized hydrothermally; their crystal structures were determined through Rietveld analyses, and supported through EDX as well as vibrational spectroscopy. The phases represent solid solutions of the alkali borate-nitrate Na3(NO3)[B6O10], which was reported in 2002 as a “New type of boron-oxygen framework in the Na3(NO3)[B6O10] crystal structure” (O. V. Yakubovich, I. V. Perevoznikova, O. V. Dimitrova, V. S. Urusov,Dokl. Phys.2002,47, 791). Only two of the three crystallographically independent Na+positions in the new structures are partially substituted by K+; a pure potassium borate-nitrate was not formed until now. The cell parameters of the novel phases vary froma=1261.72(5)–1267.12(5),b=1004.19(5)–1007.96(4),c=770.55(3)–774.38(3) pm, andV=0.97630(6)–0.98905(6) nm3in the orthorhombic space groupPnma(no. 62), in alignment with increasing K+content.


2016 ◽  
Vol 72 (10) ◽  
pp. 716-719 ◽  
Author(s):  
Akihiko Nakatsuka ◽  
Kazumasa Sugiyama ◽  
Makio Ohkawa ◽  
Osamu Ohtaka ◽  
Keiko Fujiwara ◽  
...  

The Sr–Ge–O system has an earth-scientific importance as a potentially good low-pressure analog of the Ca–Si–O system, one of the major components in the constituent minerals of the Earth's crust and mantle. However, it is one of the germanate systems that has not yet been fully examined in the phase relations and structural properties. The recent findings that the SrGeO3high-pressure perovskite phase is the first Ge-based transparent electronic conductor make the Sr–Ge–O system interesting in the field of materials science. In the present study, we have revealed the existence of a new high-pressure strontium germanate, SrGe2O5. Single crystals of this compound crystallized as a co-existent phase with SrGeO3perovskite single crystals in the sample recovered in the compression experiment of SrGeO3pseudowollastonite conducted at 6 GPa and 1223 K. The crystal structure consists of germanium–oxygen framework layers stacked along [001], with Sr atoms located at the 12-coordinated cuboctahedral site; the layers are formed by the corner linkages between GeO6octahedra and between GeO6octahedra and GeO4tetrahedra. The present SrGe2O5is thus isostructural with the high-pressure phases of SrSi2O5and BaGe2O5. Comparison of these three compounds leads to the conclusion that the structural responses of the GeO6and GeO4polyhedra to cation substitution at the Sr site are much less than that of the SrO12cuboctahedron to cation substitution at the Ge sites. Such a difference in the structural response is closely related to the bonding nature.


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