ライフサイエンスコーパス: spinel

1 ation into a copper aluminate phase (CuAl2O4 spinel).

2 egative P-T slope for its formation from the spinel.

3 or electrochemical performance of disordered spinel.

4 nominal charges of the atomic species in the spinel.

5 y of CoAl(2)O(4), a highly frustrated A-site spinel.

6 , attributed to iron oxide-bearing aluminous spinel.

7 cifically in the magnesium scandium selenide spinel.

8 e origin of the markedly superior ability of spinel {111} facets, resulting from strong interactions

9 cation to CoO and to Fe(2)SiO(4) olivine and spinel, a quenched high pressure phase metastable at amb

10 Spinels (AB(2)O(4)) form a highly important family of ma

11 addition, the adjacent octahedral centers in spinel act cooperatively in promoting the fast OER kinet

12 yite), Mn3O4 (hausmannite), and lambda-MnO2 (spinel), all containing Mn(III) possessing longer Mn-O b

13 orated into the matrix of magnesio aluminate spinel-alumina (MA-A) via infiltration of a porous prefo

14 ambient-pressure alpha-Li(3)ScCl(6) and its spinel analog with cubic closed packing (ccp) of anions.

15 Here we determine the post-spinel and akimotoite-bridgmanite transition boundaries

16 Spinel and diopside in the CAI cores are 16O-rich (Delta

17 the cubic close packed subarray of Fe(3)O(4) spinel and gamma-Fe(2)O(3).

18 omplex-oxide materials including perovskite, spinel and garnet crystal structures with varying crysta

19 d electronically distinct fragments of cubic-spinel and monoclinic Co(3)O(4) can serve as tractable y

20 e of topical materials encompassing layered, spinel and polyanionic framework compounds such as LiCoO

21 logical Clapeyron slopes of the (Mg,Fe)2SiO4 spinel and postspinel transformations.

22 remains intact and prevents the formation of spinel and rock-salt phases, which eliminates intra-part

23 ation reaction present near 3 V in a regular spinel and turns it into a solid solution.

24 or the cation ordering in LiNi(0.5)Mn(1.5)O4 spinels and correlate the stress patterns, phase evoluti

25 , with the brittle mode more dominant in the spinels and the quasi-plastic mode more dominant in the

26 ase in the lattice structure of high voltage spinel, and its effect on the charge transport propertie

27 tal structures, and test the formula against spinel- and olivine-group minerals that have well-constr

28 nanoparticles (AuNPs) supported on MgCuCr2O4-spinel are highly active and selective for the aerobic o

29 However, spinels are prone to formation of an admixture of invers

30 Experiments with doped spinels at 700 degrees C provide quantitative confirmati

31 computations, we show that the formation of spinel-based oxide layers on superalloy promotes sustain

32 tional design of NiCo(2) O(4) for developing spinel-based spintronic applications.

33 The post-spinel boundary has almost no temperature dependence, wh

34 ns, based on the assumption of a linear post-spinel boundary in pressure and temperature.

35 e find a pronounced nonlinearity in the post-spinel boundary, with its slope ranging from -4 MPa/K at

36 ons of the relative stability of layered and spinel bulk phases of Co oxides, as well as the stabilit

37 on the cation sublattice that are present in spinel but not in pyrochlore.

38 rovides a framework by which the behavior of spinel can be more accurately modeled under the extreme

39 ed that the local structure of Mg1-xNixAl2O4 spinel cannot be understood as simply being due to catio

40 The Cu-Mn spinel catalyst is robust and reused three times under o

41 damental understanding and developing robust spinel catalysts are discussed.

42 Here we report a Mn-Co spinel cathode that can deliver greater power, at high c

43 h-nickel layered cathode and 5-V cobalt-free spinel cathode.

44 Based on the radii ratio of spinel cations, a simple model is proposed to predict po

45 evaluate damage accumulation in alumina and spinel ceramics with different pre-form grain morphologi

46 A strategy is now developed to create a spinel Co(3) O(4) /perovskite La(0.3) Sr(0.7) CoO(3) int

47 hene oxide sheets and cation substitution of spinel Co(3)O(4) nanoparticles, a manganese-cobalt spine

48 ey composition is cobalt (Co)-Mn oxide (CMO) spinel, Co(x)Mn(3-x)O(4), that, despite exemplary perfor

49 arly identical to those obtained using 20 nm spinel-Co(3)O(4) nanocrystals, but 15 times more rapidly

50 of these results to those from a pure phase spinel Co3O4 catalyst supports this interpretation and r

51 of the Co(OH)2 and partial conversion of the spinel Co3O4 phases to CoO(OH) under precatalytic electr

52 diated growth, high-quality and monodisperse spinel cobalt ferrite, CoFe(2)O(4), nanocrystals can be

53 ity of LT-LiCoO2 is higher than that of both spinel cobalt oxide and layered lithium cobalt oxide syn

54 oxide nanoparticles supported on mesoporous spinel cobalt oxide, which catalyses the conversion of c

55 tion in the physical properties of different spinel compositions.

56 apacitance (in excess of 500%) for the cubic spinel compound CdCr2S4 and related isomorphs, concludin

57 pyrochlores, the amorphization resistance of spinel compounds correlates directly with the energy to

58 Here we show that a series of lacunar spinel compounds, GaM4X8 (M=Nb, Mo, Ta and W and X=S, Se

59 Most studies of spinels concern powder materials, and this challenges de

60 s the activity descriptor for the ORR/OER of spinels, consolidating the role of electron orbital fill

61 ypothesis that glass-infiltrated alumina and spinel core ceramics are resistant to damage accumulatio

62 origin of the unusual spin structure of the spinel CoV2O4, which stands at the crossover from insula

63 characterize the magnetic properties of the spinel (Cr, Mn, Fe, Co, Ni)(3)O(4) and study the evoluti

64 (III) and the formation of a Cr-incorporated spinel, Cr2O3, and Cr(OH)3 phases.

65 The spinel crystallographic structure, first solved by Bragg

66 eling of chromium-aluminum interdiffusion in spinel crystals provides a record of long-term magmatic

67 xygen carrier can avoid the formation of the spinel CuAl(2)O(4) and significantly reduce carbon depos

68 anoclusters of the room-temperature magnetic spinel CuCr(2)S(4) have been synthesized using a facile

69 In the ferromagnetic spinel CuCr2Se4-xBrx, the resistivity rho (at low temper

70 On the other hand, the spinel CuGa(2)O(4) displays spin glass behavior at ~ 2.5

71 At first sight, the quenched tetragonal spinel CuMn(2)O(4) can be formulated with Cu(2+) and Mn(

72 A magnetic transition in iron silicate spinel, detected previously by Mossbauer spectroscopy, i

73 -rich minority phase linking the crystalline spinel domains in the as-prepared state.

74 , it forms a nanomosaic of partially ordered spinel domains of 3-7 nm in size, which impinge on each

75 ing atmosphere leads to the formation of the spinel Fe3O4 phase which displays a distinct ferrimagnet

76 The inverse spinel ferrimagnetic NiCo(2) O(4) presents a unique mode

77 elimination of APBs in other members of the spinel ferrite family, such as Fe3 O4 and CoFe2 O4 , whi

78 action indicated that, during oxidation, the spinel ferrite lattice remains intact while structural F

79 Magnetic cobalt spinel ferrite nanoparticles coated with biocompatible p

80 Spinel ferrite NiFe2 O4 thin films have been grown on th

81 ontrast, Cd(II) ions either did not form the spinel ferrite structure or were not incorporated into t

82 al structure for the essentially defect-free spinel ferrite ZnFe(2)O(4), which is a widely studied fr

83 high-quality single crystalline high entropy spinel ferrites (Mg(0.2)Mn(0.2)Fe(0.2)Co(0.2)Ni(0.2))(x)

84 ion of technetium into a family of synthetic spinel ferrites that have environmentally durable natura

85 d of the divalent oxide and expansion of the spinel field appear to be general phenomena.

86 ough Mg substitution in the mesoporous Co3O4 spinel, followed by a Mg-selective leaching process.

87 vine, which does not completely transform to spinel for over a million years, suddenly transform duri

88 by a series of cation redistributions in the spinel framework, which were further supported by densit

89 The spinel from the white rind has an isotopic composition s

90 gallium oxohydroxide (GaOOH) and the defect spinel, gamma-gallium oxide (gamma-Ga(2)O(3)).

91 The lacunar spinel GaTa4Se8 was theoretically predicted to form the

92 From spinel gemstone (MgAl(2)O(4)) to layered double hydroxid

93 for content of micrometeoritic relict chrome-spinel grains (>32 um).

94 increase in the flux of L-chondritic chrome-spinel grains to Earth.

95 sulfide phases: bulk and nanophase Fe(3)S(4) spinel (greigite), and its high-pressure monoclinic phas

96 Manganese ferrite spinel has been synthesized by using low grade manganese

97 and understanding the cation distribution in spinels has been one of the most interesting problems in

98 Tc(IV) incorporation in spinels has been proposed as a novel method to increase

99 ow that ferrimagnetic order is robust in the spinel HEO.

100 ORR/OER activities of other transition-metal spinels, including Mnx Co3-x O4 (x = 2, 2.5, 3), Lix Mn2

101 Further evidence of a spinel inclusion is provided by analysis of the magnetic

102 8 eV (2.07 eV form XANES), consistent with a spinel inclusion.

103 The formation of stable spinel inclusions in a QD has not been previously report

104 ons leads to formation of small ZnCr(2)Se(4) spinel inclusions within the cubic sphalerite lattice of

105 s calculations for multicomponent AAl(2)O(4) spinels indicate that the band gap narrowing arises from

106 to spinel-like structures, transformation of spinels into active oxyhydroxides, and changes in the de

107 oxyhydroxides, and changes in the degree of spinel inversion in the course of the activation treatme

108 PLQY is surprising as the Al(III) site in a spinel is centrosymmetric, which should lead to poor per

109 inum/magnesium in circumstellar corundum and spinel is considered to reflect various stages of back-r

110 ained isothermal bulk modulus of Mg(2)TiO(4) spinel is K(T0) = 148(3) GPa when K(T0)' = 6.6, or K(T0)

111 High voltage spinel is one of the most promising next-generation coba

112 ent of the (electro)chemical behavior of the spinel is undertaken without forming a conductive compos

113 rporation of Tc(IV) has little effect on the spinel lattice structure.

114 zation of synthesized CuLaFe(2)O(4) revealed spinel lattice with average surface charge of -26.83 mV.

115 mation of an admixture of inverse and normal spinel lattices when the cation size ratio is not optima

116 s rarely coexist in geometrically-frustrated spinel lattices.

117 ina solid-solution covered by an MgCr(2)O(4) spinel layer.

118 ural-engineered lithium manganese oxide with spinel-layered heterostructures (designated as LMO-SH),

119 Li(2)MnO(3) near the surface and almost pure spinel Li(x)Mn(2)O(4) near the core.

120 on diffraction on the ordered stoichiometric spinel Li(x)Ni(0.5)Mn(1.5)O(4) within 0 < x < 2.5 in ord

121 However, it converts to the defect spinel LiFe5O8 on cycling.

122 of H2O, thus converting LiFeO2 to the defect spinel LiFe5O8 on cycling.

123 s a FeO/MnO like structure in the core and a spinel like structure in the shell.

124 ce morphology and composition giving rise to spinel-like and amorphous surface structures, respective

125 Bimetallic transition-metal oxides, such as spinel-like Co(x)Fe(3-x)O(4) materials, are known as att

126 ycles, which coincides with the emergence of spinel-like domains within the long-range DRX structure

127 ere capacity and voltage fade because of the spinel-like phase, decoding the failure mechanisms of PC

128 al insights into the ability to nanoengineer spinel-like phases.

129 cles are Co/Fe rich, and remarkably, adopt a spinel-like structure with a reduced valence of Co ions.

130 to the conversion of disordered oxides into spinel-like structures, transformation of spinels into a

131 ed that prior to the onset of OER, the Co/Fe spinel-like surface promotes the formation of the highly

132 location TEM analyses reveal that the Co/Fe spinel-like surface retains a stable chemical environmen

133 Nanocrystalline spinel LiMn(2)O(4) has been prepared and treatment of Li

134 attice mismatch between the involved phases, spinel LiMn1.5Ni0.5O4 is capable of fast rate even at la

135 , and Li2GeO3, Li4NiTeO6 and Li2MnO3 for the spinel LiMn2O4 cathodes.

136 ambda-MnO2, where the latter is derived from spinel LiMn2O4 following partial Li(+) removal.

137 As a high-voltage spinel, LiNi(0.5)Mn(1.5)O(4) (LNMO) is a promising candi

138 TiO2 followed by post-annealing treatment on spinel LiNi0.5 Mn1.5 O4 (LNMO) cathode material is devel

139 Spinel LiNi0.5Mn1.5O4 is shown to have a uniform distrib

140 n behaviors from ultradilute solutions using spinel lithium manganese oxide as the model electrode.

141 he reaction of TiO(2) and Li(2)CO(3) to form spinel lithium titanate (Li(4)Ti(5)O(12))-an anode mater

142 Zero-strain electrodes, such as spinel lithium titanate (Li4/3Ti5/3O4), are appealing fo

143 Spinels (M(3)O(4)) commonly have lower surface energies

144 intercalation/deintercalation of Li-ions in spinel materials enables not only energy storage but als

145 amond lattice, realized physically in A-site spinel materials.

146 e for the different performance of these two spinel materials.

147 des, and silicates with specific emphasis on spinel metal oxides and recently emerged 2D metal chalco

148 e rind consisting of diopside, hedenbergite, spinel (MgAl(2)O(4)), nepheline, and forsterite.

149 gV(x) O(y) -type phases (delta-MgV(2) O(5) , spinel MgV(2) O(4) , and MgVO(3) ) containing V(3+) or V

150 ane fuel cells, the Mn valence state, within spinel Mn(3)O(4)/C, increases to above 3+, adopting an o

151 Mn nanoparticles buried inside them to form spinel Mn-Co oxide nanoparticles partially embedded in t

152 Co(3)O(4) nanoparticles, a manganese-cobalt spinel MnCo(2)O(4)/graphene hybrid was developed as a hi

153 ree standing and carbon-free architecture of spinel MnCo2O4 oxide prepared using facile and cost effe

154 Spinel (modeled as Fe3O4), goethite (alpha-FeOOH), and f

155 The monolithically integrated spinel nanoarrays exhibit tunable catalytic performance

156 nide, Ln(III), incorporated into ZnAl(2)O(4) spinel nanocrystals can achieve PLQYs of 50% for down-sh

157 tic method for small, colloidally stable CMO spinel nanocrystals with tunable composition and low dis

158 nally designed Mn-doped cobalt ferrite (MCF) spinel nanocrystals, with an optimal composition Mn(0.8)

159 systematic study of 15 different AB(2)O(4)/C spinel nanoparticles with well-controlled octahedral mor

160 demonstrate this for 4 nm sized CoFe(2)O(4) spinel nanoparticles.

161 , which reversibly transforms into a layered-spinel nanostructured multiphase upon cell charging, fac

162 Here, with a model system of inverse spinel NiCo(2) O(4) , an increase in system temperature

163 The sensor was developed by fabricating spinel NiCo(2)O(4) nanoflowers (NCO) using a hydrotherma

164 ctions and creating oxygen vacancy (V(O)) in spinel NiCo(2)O(4).

165 magnetic properties of mixed-valent inverse spinel NiCo2O4(NCO) thin films.

166 Here, magnetically soft epitaxial spinel NiZnAl-ferrite thin films with an unusually low G

167 cteristic order-disorder temperatures in 3-2 spinels (nominal charges Z(A) = 3 and Z(B) = 2) are appr

168 We also show that inversion in isometric spinel occurs by a similar process.

169 n mobility is possible in other chalcogenide spinels, opening the door for the realization of other m

170 for the halogenation of phenols using Cu-Mn spinel oxide as a catalyst and N-halosuccinimide as halo

171 In the presence of Cu-Mn spinel oxide B, both electron-withdrawing and electron-d

172 Our finding demonstrates that spinel oxide can exhibit low COF values at temperatures

173 A promising high-voltage spinel oxide cathode material MgCrMnO(4) with 18% Mg/Mn

174 Precious-metal-free spinel oxide electrocatalysts are promising candidates f

175 o X-ray absorption spectroscopic study of Mn spinel oxide electrocatalysts in an operating fuel cell

176 d the high electro-catalytic activity of the spinel oxide enables excellent performance of the oxygen

177 ty and chemical ordering in a "high entropy" spinel oxide fabricated via a conventional solid-state r

178 The large spinel oxide family is widely studied due to their low c

179 hybrids results in covalent coupling between spinel oxide nanoparticles and N-doped reduced graphene

180 tal bonds between N-doped graphene oxide and spinel oxide nanoparticles.

181 unique compound in that it is the only known spinel oxide superconductor.

182 r clusters stabilized on a defective ZnGa2O4 spinel oxide surface, providing hydrogen productivity of

183 arrowing emerges in a high-entropy aluminate spinel oxide, (Fe(0.2)Co(0.2)Ni(0.2)Cu(0.2)Zn(0.2))Al(2)

184 Spinel oxides are an ideal setting to explore the interp

185 The crystal structures of A(2)BO(4) spinel oxides are classified as either normal or inverse

186 Spinel oxides can be tuned seamlessly from the low-entro

187 Here, a descriptor study on the ORR/OER of spinel oxides is presented.

188 e demonstrate that surface reconstruction of spinel oxides originates from the metal-oxygen covalency

189 Furthermore, various spinel oxides preferentially expose octahedral-occupied

190 of NiAl(2)O(4), CoAl(2)O(4), and CuAl(2)O(4) spinel oxides with varying Ni(2+), Co(2+), or Cu(2+) tet

191 s, lithium-rich layered oxides, high-voltage spinel oxides, and high-voltage polyanionic compounds.

192 able controlling the electronic structure of spinel oxides, the TM geometric effect on OER is discuss

193 3D compositional distribution of mixed Co-Fe spinel oxides, which gives atomic-scale insights into ac

194 ce nitrate catalyzed by ZnFe(x) Co(2-x) O(4) spinel oxides.

195 is narrower than the band gaps of all parent spinel oxides.

196 boost the oxygen evolution reaction (OER) in spinel oxides.

197 om pressures (~0.7-2 GPa) at the plagioclase-spinel peridotite facies boundary to the surface.

198 nite-perovskite-wustite (type 2) and olivine-spinel-perovskite (type 3) xenoliths in kimberlites from

199 The TMO-like spinel phase also alleviates the electrolyte decompositi

200 (II) were removed by the formation of MFe2O4 spinel phase and partially through their structural inco

201 o sluggish kinetics at room temperature, the spinel phase coexists with the tetragonal phase between

202 e formation of a subunit of the ZnCr(2)Se(4) spinel phase known to form as inclusions during peritect

203 ed to result from the breakdown of the gamma-spinel phase of olivine to magnesium-perovskite and magn

204 coupling with the dissociation of the gamma-spinel phase of olivine.

205 ed to the formation of a TiMn2 O4 (TMO)-like spinel phase resulting from the reaction of TiO2 with th

206 nce of Cr(III) results in the formation of a spinel phase that is a solid solution between magnetite

207 60 km are assumed to be caused by olivine -> spinel phase transformation (PT).

208 cycling, which is associated with layered-to-spinel phase transition and oxygen redox reaction.

209 tings prevented surface-initiated layered-to-spinel phase transitions in coated materials which were

210 lithium-rich layered phase to a lithium-poor spinel phase via an intermediate lithium-containing rock

211 al capable of forming a medium-entropy state spinel phase with partial cation disordering after initi

212 patterns confirmed the formation of the pure spinel phase without any impurities.

213 e scale, alloys must develop a scale without spinel phase.

214 s of Li-ion batteries with lithium manganate spinel positive and graphite negative electrodes chemist

215 idelines to navigate the cation selection in spinel pre-catalysts design.

216 vestigations of oxyhydroxides generated from spinel pre-catalysts with the same reconstruction abilit

217 prediction of the reconstruction ability of spinel pre-catalysts, based on which the reconstruction

218 rast, the isolated tetrahedral TM centers in spinel prohibit the OER mediated by dual-metal sites.

219 e are metallic Fe and Fe-Si beads, aluminous spinel rinds on the Al-Cu-Fe alloys, and Al2O3 enrichmen

220 he transformation of (Mg,Fe)2SiO4 from gamma-spinel (ringwoodite) to (Mg,Fe)SiO3-perovskite and (Mg,F

221 In perovskite/spinel self-assembled oxide nanocomposites, the substrat

222 Three major classes are spinels, sheet-like layered structures, and three-dimens

223 variety of compositions adopt the isometric spinel structure (AB2O4), in which the atomic-scale orde

224 is a semiconducting nanocomposite which has spinel structure and Halloysite nanotube (HNT) is an eco

225 esized iron oxide nanoparticles have a cubic spinel structure as characterized by HRTEM, SAED, and XR

226 ct of Mn and Co, while Fe helps preserve the spinel structure during cycling.

227 Inorganic compounds with the AB2X4 spinel structure have been studied for many years, becau

228 Consequently, the simple spinel structure is more complicated than previously tho

229 we have developed a new class of ultra-thin spinel structure Li(0.5)Al(1.0)Fe(1.5)O(4) (LAFO) films

230 The results shows the presence of spinel structure manganese ferrite (MnFe(2)O(4)) as the

231 (XPS) results confirm the crystallinity and spinel structure of the prepared Fe(3)O(4) samples and p

232 4)) nanoparticles (ca. 25 nm) of the inverse-spinel structure prepared by the hydrothermal method.

233 These excellent findings are due to spinel structure suppression, electrochemical stress opt

234 us Fe(3)O(4) with crystalline walls (inverse spinel structure) has been synthesized for the first tim

235 gnated as LT-LiCoO2) that adopts a lithiated spinel structure, as an inexpensive, efficient electroca

236 ement leads to an elegant description of the spinel structure, but represents an increase in complexi

237 tion of the framework, while maintaining the spinel structure, lambda-MnO(2).

238 le Fe works to maintain the integrity of the spinel structure, likely contributing to the remarkable

239 itially closer to the ideal crystallographic spinel structure, never reached such a state and require

240 t into the defect chemistry of ringwoodite's spinel structure, which not only accounts for a potentia

241 ing along the [110] direction in the inverse spinel structure.

242 in the tetrahedral sites of the gamma-Fe2O3 spinel structure.

243 with a significant amount of defects in the spinel structure.

244 into nanocrystalline forms with the inverse spinel structure.

245 2)O(4)(001) barrier with a cation-disordered spinel structure.

246 Ni(0.5)Mn(1.5)O(4) (LNMO) is a high-capacity spinel-structured material with an average lithiation/de

247 In fact, most published spinel structures have dubious atomic displacement param

248 ctional population of the inverse and normal spinel structures within Tb(x)ZnAl(2-x)O(4).

249 , a simple model is proposed to predict post-spinel structures.

250 report a well-defined cuboctahedral MgAl2O4 spinel support material that is capable of stabilizing p

251 ized at the surface of the ternary MgCuCr2O4-spinel support.

252 , resulting from strong interactions between spinel surface oxygens and epitaxial platinum {111} face

253 polaron transport model is tested by using a spinel system with mixed cation oxidation states (Mn(x)

254 Nickel-manganese-cobalt tetragonal spinel ternary oxide nanocomposite (NMC-TSO) was synthes

255 c pathways for the relaxation of disorder in spinel that are absent in pyrochlore.

256 compact and continuous nanocrystalline Co3O4 spinel that is impervious to phase transformation and im

257 ion resistance and disordering energetics in spinel, the opposite of that observed in pyrochlores.

258 In some spinels, the space group symmetry is debated, and in gen

259 -Fe(2)O(3) (corundum structure) to Fe(3)O(4) spinel then to gamma-Fe(2)O(3) by oxidation, while prese

260 has been used as a conducting layer for the spinel thin films based devices and the search for a p-t

261 tely an order of magnitude lower than in 2-4 spinels, thus explaining why typical 3-2 samples exhibit

262 hat the pressure and temperature of the post-spinel transformation in Mg2SiO4 is consistent with seis

263 n measurements showed that cubic Mg(2)TiO(4) spinel transforms to a high pressure tetragonal (I4(1)/a

264 The calorimetric entropy of the olivine-spinel transition in Fe(2)SiO(4) (-16 +/- 5 J/mol.K) is

265 The post-spinel transition marks the upper-lower mantle boundary,

266 Spinel transition metal oxides (TMOs) have emerged as pr

267 Spinel transition metal oxides are important electrode m

268 ressure and temperature changes) of the post-spinel transition that do not allow a significant depres

269 time and space can therefore cause the post-spinel transition to have variable effects on mantle con

270 ite to bridgmanite plus ferropericlase (post-spinel transition)(1-3).

271 Lithium-ion (Li-ion) batteries based on spinel transition-metal oxide electrodes have exhibited

272 Spinel-type catalysts are promising anode materials for

273 case studies across Ni-rich layered oxides, spinel-type cathodes, and garnet-based electrolytes are

274 (2-x)Rh(x)O(4) metal oxide precursors with a spinel-type crystal structure.

275 Si(1-x),Ti(x))(3)N(4) with x = 0 < x < 1 and spinel-type crystal structure.

276 itions of 15-20 GPa and 1800-2000 degrees C, spinel-type gamma-Si(3)N(4) and rock salt-type c-TiN are

277 an be overcome, as demonstrated by nanosized spinel-type HEOs achieving reversible phase transformati

278 Spinel-type high entropy oxides (HEOs) have emerged as p

279 Reaction pathway studies show a Fe-rich spinel-type intermediate and indicate that competing che

280 en evolution reaction activities, making the spinel-type LT-Li0,5CoO2 a potential bifunctional electr

281 t our results will even impact other hydrous spinel-type materials, helping to understand properties

282 ng of the structure-property relationship in spinel-type materials.

283 al conductivity and viscosity of water-based spinel-type MnFe2O4 nanofluid.

284 al synthesis of approximately 5.5 nm inverse spinel-type oxide Ga2FeO4 (GFO) nanocrystals (NCs) with

285 xygen that results in nanosized particles of spinel-type oxide LiMn(2)O(4), one of the leading cathod

286 tly theoretically predicted, some classes of spinel-type oxide materials can be intrinsically doped b

287 ndings underscore the potential relevance of spinel-type oxides as p-type transparent conductive oxid

288 is conditions and is analyzed to exhibit the spinel-type structure with ca. 8 atom% of Ti.

289 The change of crystal structure from beta to spinel was determined using reciprocal space mapping in

290 between the cubic and tetragonal/monoclinic spinel was driven by stress and temperature during high

291 s from PMS induced by a magnetic CuFe(2)O(4) spinel was studied.

292 surface is composed of a Co- and/or Ni-rich spinel with antisite defects.

293 CuAl(2)O(4) is a ternary oxide spinel with Cu(2+) ions ([Formula: see text]) primarily

294 compared two structurally equal Co(2)FeO(4) spinels with nominally identical stoichiometry and subst

295 The sensor was created by embedding spinel zinc ferrite nanospheres (ZnFe(2)O(4)) on three-d

296 triggers conversion of adsorbed Zn(II) into spinel Zn(II)1-xMn(II)xMn(III)2O4 precipitates at pH 7.5

297 rustrated magnetic interactions in the cubic spinel ZnCr(2)O(4).

298 croscopy to probe the lithiation behavior of spinel ZnFe(2)O(4) as a function of particle size.

299 Spinel ZnGa(2)O(4) is an ultra-wide bandgap material tha

300 For spinel ZnGaO samples, five deconvoluted peaks were obser