ライフサイエンスコーパス: solid solution

1 y homogeneous, forming a completely miscible solid solution.

2 increased surface area and roughness of the solid solution.

3 crystallization of barite into a Ba1-xRaxSO4 solid solution.

4 ween sections 5 and 6, due to formation of a solid solution.

5 hains move smoothly apart to accommodate the solid solution.

6 s Li-Pt liquid alloy was quenched into Li-Pt solid solution.

7 totype system: the hexagonal YMnO(3)-YInO(3) solid solution.

8 as a conglomerate, and even more rarely as a solid solution.

9 to those of certain concentrated binary FCC solid solutions.

10 rization of room-temperature LixMn1.5Ni0.5O4 solid solutions.

11 limited to the goal of creating single-phase solid solutions.

12 ction lies a short-range-order mechanism for solid solutions.

13 roteins) is also displayed with multipeptide solid solutions.

14 stoichiometric compounds as models of dilute solid solutions.

15 ompared to the well-known PbTe(1)(-)(x)Se(x) solid solutions.

16 f that the systems (AgSbTe2)(1-x)(PbTe)x are solid solutions.

17 mber of compositions possible through M-site solid solutions.

18 ses of ordered intermetallics and disordered solid solutions.

19 sitive through the formation of single-phase solid solutions.

20 question has remained as to how random these solid solutions actually are, with the influence of shor

21 show that the indium and gold layers form a solid solution after annealing at 200 degrees Celsius an

22 as matrices for organic-based substitutional solid solutions allows for the incorporation of multiple

23 accounts for the compositional dependence of solid-solution alloy critical potentials.

24 We find the surprising result that solid solution alloys become less likely as the number o

25 cific elements, in single-phase concentrated solid solution alloys can lead to substantial reduction

26 e nickel metal and single-phase concentrated solid solution alloys of 50%Ni50%Co (NiCo) and 50%Ni50%F

27 t MgH2 can indeed be destabilized by forming solid solution alloys of magnesium with group III and IV

28 ures in equiatomic single-phase concentrated solid solution alloys, and more importantly, reveals its

29 ared to the corresponding PbTe(1)(-)(x)Se(x) solid solution alloys.

30 Single-phase concentrated solid-solution alloys (SP-CSAs) have recently gained unp

31 dazole-3-oxide-1-oxyl (BImNN) crystallize as solid solutions (alloys) across a wide range of binary c

32 ting for the compositional regions of single solid solution and composite phases.

33 tigate competition between an entropy-driven solid solution and enthalpy-driven phase separation.

34 two stable polymorphs in the TaSe(2-x)Te(x) solid solution and find that the 3R polytype shows a sup

35 lerated with the recent discovery of several solid solution and ordered phases involving at least two

36 ehaves as a coexistence of point-defect rich solid solution and phase separation.

37 -equilibration of the solid to a Ba1-xRaxSO4 solid solution and visible effects on the particle size

38 lloy falls between those of analogous simple solid solutions and amorphous materials and test the eff

39 th BaF2, to create nanostructured Ba1-xCaxF2 solid solutions and increased its ionic conductivity by

40 rmation is absent in the constituent oxides, solid solutions and larger period superlattices.

41 GaP-ZnS solid solutions and multilayered structures have a tunab

42 as phase ions that form the Ce(x)Zr(1-x)O(2) solid solutions and those that condense to delta-Al(2)O(

43 diffraction, the simultaneous occurrence of solid-solution and two-phase reactions after deep discha

44 ent occurrence of and transition between the solid-solution and two-phase reactions.

45 insic charge storage mechanism (two-phase vs solid-solution) and localization of charge give rise to

46 adius) in a face-centered cubic (FCC) CoFeNi solid solution, and a chemical ordering tendency leading

47 ich forms a single-phase face-centered cubic solid solution, and found it to have exceptional damage

48 es significantly, the system deviates from a solid solution, and phase separation of the GeS1-xSex (5

49 ods of technologically important Pb(Zr,Ti)O3 solid solutions, and demonstrate the existence of previo

50 well for multiphase composites, single phase solid solutions, and equivalent ionic substituted single

51 terials in solution, spin-coated thin films, solid solutions, and Langmuir films.

52 The prominent comprehensive properties of solid-solution- and intermetallic-based Ti alloys are de

53 These catalysts were synthesized using a solid solution approach by controlled substitution of 1-

54 rs at x = 0.1, but the conductivities of the solid solutions are enhanced and the activation energies

55 Gallium nitride (GaN) and its solid solutions are excellent photocatalytic materials;

56 c metastability, anatase-type TiO(2) -IrO(2) solid solutions are generally hard to synthesize.

57 Alloy and nitride solid solutions are prominent for structural, energy and

58 TaC, HfC and their solid solutions are promising candidate materials for th

59 w considers defect chemistry of TiO2 and its solid solutions as well as defect-related properties ass

60 HEAs is considerably higher than traditional solid solutions, as the many constituents lead to a rugg

61 roach we form a novel rocksalt Mg0.4 Fe0.6 N solid solution at between 15 and 23 GPa and up to 2500 K

62 anocrystals behave as metastable homogeneous solid solutions at room temperature and tend to phase se

63 s a result of the formation of NaNbO3-NaTaO3 solid solutions at temperatures above 700 degrees C.

64 owth of a strained epitaxial Pb-rich calcite solid-solution at the calcite (104)-water interface.

65 n between entropically driven atomic mixing (solid solution behavior) and enthalpy-driven phase separ

66 als no 2-phase transformations, but a single solid-solution behavior during battery cycling.

67 c ordering within the Mn(1-x)Sn(x)Bi(2)Se(4) solid-solutions below 50 K switches from antiferromagnet

68 RD measurements indicated the formation of a solid solution between AFm-I(2) and AFm-SO(4) for the I-

69 The formation of a solid solution between AFm-I(2) and AFm-SO(4), with a sh

70 in the formation of a spinel phase that is a solid solution between magnetite (Fe3O4) and chromite (F

71 proposition that the LAST family behaved as solid solutions between the PbTe and AgSbTe2 compounds.

72 ype precipitates have been used to reinforce solid-solution body-centered-cubic iron for high-tempera

73 0.2Ta0.2Cr0.2Ti0.2)B2, possess virtually one solid-solution boride phase of the hexagonal AlB2 struct

74 nd (Pb(0.95)Sn(0.05)Te)(1-x)(PbS)(x) are not solid solutions but phase separate into PbTe-rich and Pb

75 time, a bulk metastable Al-Mg supersaturated solid solution by the diffusion bonding of separate Al a

76 standing and controlling the compositions of solid solutions by separately tuning their nucleation an

77 tes that single-crystalline Mg(3) (Sb,Bi)(2) solid solutions can exhibit higher zT compared to polycr

78 is readily soluble in Fe represents an ideal solid-solution case to better understand the light-eleme

79 We show that the Ni/MgO solid-solution catalyst that we reported in 1995, which

80 777) ignore the reported efficient Ni/MgO solid-solution catalysts and overstate the novelty and i

81 In Pb1-xSb2x/3Se solid solutions, cation vacancies are intentionally intr

82 ightly hypostoichiometric TaC, HfC and three solid solution compositions (Ta1-xHfxC, with x = 0.8, 0.

83 Such polytypism can create a multiphase solid-solution compound with a large number of interface

84 responsive properties by the mixed component solid-solution concept are included, and as well example

85 ositions across the (Mg,Fe)O magnesiowustite solid solution confirms that ferrous iron (Fe(2+)) under

86 gate the ground-state structures of PbTiO(3) solid solutions containing Ni, Pd, and Pt.

87 The free energy of the solid solution continuously varies with the enantiomeric

88 hat the alloys form an inner chromia-alumina solid-solution covered by an MgCr(2)O(4) spinel layer.

89 the c lattice parameter in the AlB(2) -type solid solution Cr(1-) (x) Mo(x) B(2) (x = 0, 0.25, 0.4,

90 h CsCl and CuAu-I symmetries, or disordered, solid solution crystals when slowly cooled.

91 nt variables in composition of these ternary solid solution crystals.

92 Control studies on solid-solution crystals reveal that the third [100] orie

93 hips of these materials, we have synthesized solid-solution Cs2Sn1-xTexI6.

94 be the synthesis and characterization of the solid solution Cu(2)Zn(1-x)Fe(x)GeSe(4).

95 nto Au occurs, and the atomically disordered solid solution Cu(x)Au(1)(-)(x) exists.

96 bility, and thermoelectric properties of the solid solutions Cu(2+x)Zn(1-x)GeSe(4) (x = 0-0.1) are re

97 tituting Cu into the Fe lattice, forming the solid-solution Cu(y)Fe(1-y)F(2), reversible Cu and Fe re

98 ed for essentially by phonon scattering from solid solution defects rather than the assistance of end

99 ed via core structural transition from cubic solid solution [denoted as face centered cubic (fcc)] st

100 olled cation non-stoichiometry combined with solid-solution doping by metals supervalent to Li+ incre

101 ring lithiation, and moreover stabilizes the solid solution during lithiation.

102 aces of readily available SrTiO(3) -SrIrO(3) solid solutions during electrocatalysis in acidic soluti

103 that both nanostructures and point defects (solid solution) effectively scatter phonons in this syst

104 nditions facilitating the fast attainment of solid-solution equilibria (e.g., in stagnant waters), Fe

105 Lattice parameters of the solid solutions evidently follow Vegard's Law.

106 es to an important non-relaxor ferroelectric solid solution exhibiting the so-called composition-indu

107 The existence of the TZF solid solution explains the absence of eutectic melting

108 fluences, followed by gradual transitions to solid solution fcc-structured (M(n+1)A)X(n) phases.

109 gher valent transition metals to create wide solid-solutions fields with exceedingly rare and complex

110 hesized lead-free BiFeO(3)-BaTiO(3)-SrTiO(3) solid-solution films to realize the coexistence of rhomb

111 solubility, the production of supersaturated solid solutions followed by the segregation of elements

112 system where, neither an alloy nor a nitride solid solution form at ambient conditions and bulk MgN a

113 t were obtained by determining the extent of solid solution formation between a graphite source and a

114 This failed, however: solid solution formation of the stacked loop form is usu

115 such as LiCoO2, lithiation proceeds through solid-solution formation, whereas in other materials suc

116 nd the rearrangement of X anions, disordered solid solution gamma-(M(n+1)A)X(n) phases are formed at

117 A solid-solution growth methodology of aromatic molecular

118 bulk solution was found to be controlled by solid-solution growth rates.

119 of multiple strengthening mechanisms such as solid solution hardening, forest dislocation hardening,

120 anced functional properties in semiconductor solid solutions has attracted vast scientific interest f

121 chalcogenides PbTe, PbSe, and PbS (and their solid solutions) have been preferred high-performance th

122 the development of homogeneous single-phase solid-solution HEAs and 2) the ambiguity in describing t

123 vianite, thus forming a vivianite-symplesite solid solution identified as Fe3(PO4)1.7(AsO4)0.3.8H2O.

124 n of composition in the magnetite-ulvospinel solid solution, important uncertainties remain about the

125 condly on suppressing the formation of RE-Ba solid solution in a controlled manner within large grain

126 xpansion of the CaBa(1-x)Pb(x)Zn(2)Ga(2)O(7) solid solution in fact is a macroscopic performance of t

127 The solid solution in the P21/n space group was found to be

128 ious reports of the occurrence of a complete solid solution in this system.

129 to rationalize the formation of high-entropy solid solutions in these metal diborides.

130 In a recent neutron total scattering study, solid solutions in this system were reported to feature

131 tead involves two thermodynamically distinct solid solutions in which the Li exclusively occupies the

132 NiO-MgO solid solution interacted with ZrO(2) support was found

133 t affected by the immobilized charges at the solid-solution interface and those resulted from the app

134 strates a lowered free energy barrier at the solid-solution interface in the presence of CA.

135 mer-decorated phospholipid monolayers at the solid-solution interface was investigated using neutron

136 istics of the electrical double layer at the solid-solution interface, blocking surface sites, or pro

137 ure dependence of a chemical reaction at the solid/solution interface is studied by scanning tunnelin

138 Understanding the atomic-scale growth at solid/solution interfaces is an emerging frontier in mol

139 This solid solution is a kinetic product of crystallization m

140 Bi(0).(5)Na(0).(5)TiO(3)-based solid solution is among the most promising lead-free pie

141 of all possible chemical environments for a solid solution is challenging.

142 and 1800 K show that while no Re-Zn alloy or solid solution is formed, a novel Re(3)ZnN(x) ordered so

143 ution is formed, a novel Re(3)ZnN(x) ordered solid solution is formed, at 20 GPa, with nitrogen occup

144 rhard, and the bulk modulus of the 48 atom % solid solution is nearly identical to that of pure ReB2.

145 The Pb(Zr,Ti)O3 (PZT) disordered solid solution is widely used in piezoelectric applicati

146 candidates; however, depolarization of these solid solutions is a longstanding obstacle for their pra

147 The formation of mixed linker solid solutions is likely a general strategy for the con

148 kel to binary and to more complex quaternary solid solutions is observed.

149 A key signature of relaxor-ferroelectric solid solutions is the existence of polar nanoregions, a

150 argyrodite lithium superionic conductors, as solid solutions Li(6+x)M(x)Sb(1-x)S(5)I (M = Si, Ge, Sn)

151 the crystalline peroxide via a Li deficient solid solution (Li(2-x)O2) phase.

152 meter-scale state-of-charge heterogeneity in solid-solution Li1- x Ni1/3 Co1/3 Mn1/3 O2 secondary par

153 Here we report that the 50/50 solid solution, Li1+x(V0.5Ti0.5)S2, delivers a reversibl

154 The lattice parameters for the solid solutions linearly increase along both the a- and

155 d proposes a method for the synthesis of new solid solution (M(n+1)A)X(n) phases by tailoring the dis

156 Furthermore, 7-9 can also form crystalline solid solutions (M,M')(NPBA)2(NO3)2(MeOH)2 (M, M' = Co2+

157 -stage kinetic process involving mixed quasi-solid solution/macroscopic two-phase transformations ove

158 which form a combination of a nanostructured/solid solution material as determined by transmission el

159 With these, a solid solution material, [Zr6 O4 (OH)4 (L1)2.6 (L2)0.4 ]

160 om a solid solution of alpha-LiAl, revealing solid solution-mediated crystallization of beta-LiAl.

161 We discovered a Type II solid solution (mixed crystal) of the enantiomers of the

162 9, we present a critical review of the famed solid solution model first disclosed in 1959.

163 not be explained on the basis of a classical solid solution model.

164 s with a fresh look on this well-established solid solution model.

165 trecker reaction illustrate the potential of solid solution MOFs to provide the ability to address th

166 metal in equivalent crystallographic sites (solid solution MOFs) exhibit catalytic activity, which i

167 cally investigated three interrelated binary solid-solution MXene systems based on Ti, Nb, and/or V a

168 The macroscopic electrical conductivity of solid solution MXenes can be controllably varied over 3

169 The pyrochlore solid solution (Na(0.33)Ce(0.67))2(Ir(1-x)Ru(x))2O7 (0</

170 architectures on the atomic scale (Na and M solid solution), nanoscale (MSe nanoprecipitates), and m

171 lly show this with porous SrTiO(3) -SrIrO(3) solid-solution nanotubes synthesized by a facile synthet

172 nd subsequently converting them into CoMP(x) solid-solution NRs through thermal post-treatment are es

173 organic films was found to be controlled by solid-solution nucleation rates; instead, the Sr-poor ba

174 A solid solution of a ferroelectric and a spin-glass perov

175 nfirm the transformation of beta-LiAl from a solid solution of alpha-LiAl, revealing solid solution-m

176 he formation of an electronically conductive solid solution of chromium(iii) and aluminium oxides in

177 arge-trap flash memory element is based on a solid solution of copper and zirconium oxides (Cu-ZrO2)

178 Single microcrystals of a 1:1 solid solution of n-C32H66/n-C36H74 have been grown by e

179 e layer was granular consisting of grains of solid solution of Ti(Zr)ON segregated by amorphous ZrO(2

180 The carbide is a substitutional solid solution of Zr-Ti containing carbon vacancies that

181 By doping ZrN into the TiN layer, solid solution of ZrTiN was formed and the lattice const

182 ly homogeneous thin films that are amorphous solid solutions of Al2O3 and transition metal oxides (TM

183 Mesoporous solid solutions of anatase-based titanium-vanadium oxide

184 ion model that included pure Pb minerals and solid solutions of calcite (Ca (x)Pb(1- x)CO(3)) and apa

185 Solid solutions of Ce1-x Ndx O2-0.5x , Ce1-x Smx O2-0.5x

186 Similar solid solutions of enantiomers may exist in other system

187 High-entropy alloys, near-equiatomic solid solutions of five or more elements, represent a ne

188 is view, as these materials are single-phase solid solutions of generally equiatomic mixtures of meta

189 kite solar cells based on alloyed perovskite solid solutions of methylammonium tin iodide and its lea

190 ulting crystalline heterobimetallic MOFs are solid solutions of Ru(2) and Cu(2) sites housed within [

191 Here, we report solid solutions of SnTe with NaSbTe(2) and NaBiTe(2) (Na

192 nsition explains the difficulty in preparing solid solutions of the P2(1)/n form with guests of formu

193 Solid solutions of the rare earth (RE) cations Pr(3+), N

194 rides, we have synthesized and characterized solid solutions of this material with tantalum (Ta), man

195 he ReB2-type structure can be maintained for solid solutions of tungsten in ReB2 with tungsten conten

196 xagonal symmetry, attempts were made to form solid solutions of UICs containing guests from the two c

197 Motivated by these results, ternary solid solutions of WB(4) were produced, keeping the conc

198 rs with the concept of mixed-component MOFs (solid solutions) offers very rich additional dimensions

199 may warrant further studies into additional solid solutions or ternary compounds taking this structu

200 thode where delithiation occurs via either a solid-solution or a two-phase mechanism, the pathway tak

201 s us to identify candidates that are alloys, solid-solutions, or compounds with statistical vacancies

202 y of TZF to simultaneously form racemate and solid solution originates from its conformational flexib

203 tions and reaction pathways in the long term solid-solution partitioning and solid-phase distribution

204 ting phases, the tendency for a single-phase solid-solution pathway with exceptional reaction kinetic

205 n-germanium triiodide (CsSn(0.5)Ge(0.5)I(3)) solid-solution perovskite as the light absorber in PSCs,

206 eal the existence of a continuous metastable solid solution phase during rapid lithium extraction and

207 n many cases their structure is not a single solid solution phase, and that the rules may not accurat

208 Cu nanoparticles are synthesized in a single solid-solution phase with robust control over the Co/Mo

209 tion, as is well known in microdroplets; ii) solid/solution phase, where such acceleration appears to

210 Here we report a generalizable solid/solution-phase strategy for the synthesis of discr

211 opy Alloys (HEAs), with predominantly single solid solution phases are a current area of focus in all

212 Here we report new halide-rich solid solution phases in the argyrodite Li(6) PS(5) Cl f

213 emonstrated its capability in predicting HEA solid solution phases with or without intermetallics in

214 entropy alloys, with lamellar arrangement of solid solution phases, represent a new paradigm for simu

215 ntropy increases the stability of disordered solid solution phases.

216 ence due to the elusive metastable nature of solid solution phases.

217 that such catalytically active anatase-type solid-solution phases can be created in situ on the surf

218 ng of a lamellar arrangement of L1(2) and B2 solid-solution phases.

219 Ceria and its solid solutions play a vital role in several industrial

220 nal phonon scattering centers such as excess solid solution point defects and grain boundaries.

221 to phonon scattering by entropically driven solid solution point defects rather than conventional en

222 ace-charge theory applicable to concentrated solid solutions (Poisson-Cahn theory) was applied to des

223 es in thin films, as well as in concentrated solid solutions (polyisobutylene matrix), with peak abso

224 All the solid solutions possess high specific surface areas, up

225 es, we show that anatase-type TiO(2) -IrO(2) solid solutions possess more active iridium catalytic si

226 harge transfer is possible by exploiting the solid-solution properties of MOFs together with electron

227 This work suggests that concentrated solid-solution provides an effective way to enhance radi

228 SrSiO3 (C12/C1) is shown to provide a larger solid solution range (0 < x </= 0.45) in Sr1-xNaxSiO3-0.

229 The solid-solution range, which is reduced at higher current

230 cation is inserted reversibly over a finite solid-solution range.

231 doped with an array of tungsten levels as a solid solution ranging from 0.38-13.8 W/Ti atom % was fo

232 ed Zn at each pH over a 10-fold range in the solid/solution ratio.

233 e number of mobile oxygen vacancies in these solid solutions reaches a maximum near those composition

234 The sufficient Na and complete solid-solution reaction are critical to realizing high-p

235 ge, crack healing is possible in the reverse solid-solution reaction occurring during discharge.

236 ervation was revealed to be initiated by the solid-solution reaction of the LiMO2 phase on charge to

237 ealing being principally associated with the solid-solution reaction of the LiMO2 phase.

238 The complete solid-solution reaction over a wide voltage range ensure

239 d the relationship between the two-phase and solid-solution reactions remain controversial.

240 The phase at the limit of the solid solution regime, Li(5.5) PS(4.5) Cl(1.5) , exhibit

241 eering the atomic structure that extends the solid-solution region and suppresses phase transformatio

242 We were able to pinpoint that the extended solid-solution region with suppressed phase transformati

243 system at 400 degrees C reveal five separate solid solution regions that show three distinct substitu

244 The crystal structure of this solid solution resembles that of the enantiomorph but ha

245 itions that span the MoSe2-WSe2 and WS2-WSe2 solid solutions, respectively.

246 ounts of the larger molecular rotor 2 in the solid solution results in significant dynamic perturbati

247 imulations of jerky flow in W-O interstitial solid solutions reveal three dynamic regimes emerging fr

248 ermal transport calculations of the complete solid solution series Cu2ZnGeSe(4-x)S(x) (x = 0-4).

249 Here, we report the first solid solution series incorporating both A and A' cation

250 ous end-member of the merrillite-whitlockite solid solution series.

251 c ordering within the Mn(1-x)Sn(x)Bi(2)Se(4) solid-solution series can be rationalized by taking into

252 mpositions of manganese-tin-bismuth selenide solid-solution series, Mn(1-x)Sn(x)Bi(2)Se(4) (x = 0, 0.

253 gh piezoelectricity in relaxor-ferroelectric solid solution single crystals is a breakthrough in ferr

254 on document the recovery of a Ge(0.9)Sn(0.1) solid solution (space group P4(3)2(1)2, a = 6.014 (1) A,

255 entropy as high as that of an ideally mixed solid solution (SS) of multiple elements in near-equal p

256 n become the driving force for cubic nitride solid solution stability.

257 reaction proceeds through a Na2-xLixMg2P3O9N solid solution (stage 1) followed by a two-phase reactio

258 ive or more major elements may stabilize the solid-solution state relative to multiphase microstructu

259 from massive substitutional and interstitial solid solution strengthening as well as from the composi

260 e-temperature space: one resembling standard solid solution strengthening, another one mimicking solu

261 ers vary systematically, we demonstrate that solid-solution strengthening can be effectively employed

262 ility known from advanced steels and massive solid-solution strengthening of high-entropy alloys.

263 tion of the best suited element mix for high solid-solution strengthening using the simple electroneg

264 stent barite: (1) formation of a Ba1-xRaxSO4 solid solution surface layer on the barite or (2) a comp

265 ing channel consisting of an amorphous Ta(O) solid solution surrounded by nearly stoichiometric Ta(2)

266 ly large band gap narrowing in the NixMg1-xO solid solution system.

267 t the synthesis of a mesoporous Mn0.5Ce0.5Ox solid solution that is highly active for the selective o

268 gh-performance piezoelectrics are lead-based solid solutions that exhibit a so-called morphotropic ph

269 mixed-cationic Cs(2)Bi(1-x)In(x)AgCl(6) HDP solid solutions that span the indirect to direct band-ga

270 We note that, for undoped ceria and its solid solutions, the relationship between short range or

271 Similar to the (Zr,Hf)NiSn based solid solutions, the unsubstituted ZrNiSn compound also

272 y used here should be equally applicable for solid solution thermoelectrics and provides a strategy f

273 commodating lithium continuously by means of solid-solution transformation because they have few kine

274 In contrast, a solid-solution transformation dominates the early stages

275 The end members and 10 solid solutions UxTh(1-x)SiO4 with x = 0.12-0.92 were su

276 Substitution renders the solid solutions visible-light active.

277 Understanding the kinetic implication of solid-solution vs. biphasic reaction pathways is critica

278 dulus of 335 +/- 3 GPa for the hardest WB(4) solid solution, W(0.93)Ta(0.02)Cr(0.05)B(4), and showed

279 The T(c) of the Zr(0.5)Y(0.5)B(12) solid solution was suppressed to 2.5 K.

280 ated on the basis of preparation of (U,Th)O2 solid solutions, was obtained.

281 Using the example of a Cu-Au solid solution, we demonstrate that compositional variat

282 The lattice parameters of the solid solutions were calculated using their XRD patterns

283 The solid solutions were have been characterized by XRD, SEM

284 CrCoNi, as a single-phase face-centred cubic solid solution, which displays strength-toughness proper

285 l Li-ion dynamics and atomic disorder in the solid solutions, which are correlated to the ionic diffu

286 pplications are usually complex, engineered, solid solutions, which complicates their manufacture as

287 4(2-) and SeO4(2-) have a propensity to form solid solutions, which limits the selectivity between th

288 ized properties, such as a simple binary NiV solid solution whose yield strength exceeds that of the

289 ttributed to the formation of a Mn0.5Ce0.5Ox solid solution with an ultrahigh manganese doping concen

290 on stoichiometry leads to the formation of a solid solution with dual sublattice mixing.

291 A solid solution with the AgCN structure exists in the (Cu

292 The obtained Ce(0.7)Zr(0.3)O(2) powders are solid solutions with a cubic phase.

293 (2-x)Sn(x)S(2) nanocrystals are single phase solid solutions with cubic NaCl-type structure.

294 HEAs are single or multiphase crystalline solid solutions with high ductility.

295 Se(m+3n) nanomaterials behave as homogeneous solid solutions with lattice parameter trending as a fun

296 that the high electromechanical coupling in solid solutions with lead titanate is due to tuning of t

297 d us to prepare organic-based substitutional solid solutions with tunable chromaticity regulated only

298 A MoS2(1-x) P(x) solid solution (x = 0 to 1) is formed by thermally annea

299 space group at 42 and 41 K respectively, the solid solutions (y = 1 to 7) retain cubic symmetry down

300 Single-phase metal dodecaboride solid solutions, Zr(0.5)Y(0.5)B(12) and Zr(0.5)U(0.5)B(1