ライフサイエンスコーパス: cubic

1 n most cases, garnet does not initially grow cubic.

2 fcc-2H-fcc gold nanorods (fcc: face-centred cubic; 2H: hexagonal close-packed with stacking sequence

3 Mesoscopy combined with the novel CUBIC Acid-Fast (CAF) staining procedure enables a quant

4 Ni Cantor alloy(2) and of a new face-centred cubic alloy, CrFeCoNiPd.

5 However, the black-phase CsPbI(3) (cubic alpha-CsPbI(3) and orthorhombic gamma-CsPbI(3) pha

6 isordered, consisting of random sequences of cubic and hexagonal ice layers.

7 order in the form of complex combinations of cubic and hexagonal stacking motifs.

8 The simultaneous cubic and quadratic nonlinear processes are implemented

9 omposition fluctuations and a coexistence of cubic and rhombohedral phases in favor of exceptional fi

10 effectively giving local structures that are cubic and tetragonal like from the point of view of the

11 thermal Gruneisen parameters (gamma(th)) of cubic and tetragonal Mg(2)TiO(4) phases are 1.01 and 0.6

12 xotic periodic lattices like gyroid, rotated cubic, and diamond structures.

13 ncluding cubic-closest packed, body-centered cubic, and interpenetrating networks, bridged by interst

14 ured optical metamaterials possess a chiral, cubic, and triply periodic bulk morphology that exhibits

15 o such designs confirm the presence of a 420 cubic angstromngstrom chamber defined by the top of the

16 tic shape anisotropy and that the underlying cubic anisotropy makes a significant contribution to the

17 Isoreticular with MOF-5, CUB-5 adopts a cubic architecture but features aliphatic, rather than a

18 s with shapes ranging from spherical towards cubic are used for a first plausibility test.

19 The centrosymmetric complexes contain a cubic arrangement of iron(II) centers, with bis-bidentat

20 c sides are joined by 4 Ag(+) ions to give a cubic array and no Ag(+) ions were found inside the clus

21 ssembly and disassembly of the base-centered cubic (bcc) and face-centered cubic (fcc) crystalline na

22 close-packed (hcp) Au(30) and body-centered cubic (bcc) Au(38) NCs protected by the same type of cap

23 les, was noted in a metastable body-centered cubic (bcc) beta-titanium alloy on tensile deformation.

24 ndergo an interconversion from body-centered cubic (bcc) close-packed micelles to a succession of Fra

25 o types of colloidal crystals: body-centered cubic (BCC) crystals and face-centered cubic (FCC) cryst

26 faces were established between body-centered cubic (BCC) crystals and their liquid using charged coll

27 Body-centered cubic (bcc) HEAs, particularly those based on refractory

28 cc) metals but rarely found in body-centered cubic (Bcc) metals under room temperature and slow strai

29 face-centered cubic (FCC) and body-centered cubic (BCC) metals.

30 sicrystalline (DQC) phase, and body-centered cubic (BCC) phase, is reported.

31 A single-phase body-centered-cubic (BCC) refractory HEA, NbTaTiVZr, using thermodynam

32 n energies in binary alloys of body-centered-cubic (bcc) refractory metals (such as W and Ta) with tr

33 expanded lattice in the Fe(0) body-centered-cubic (BCC) structure and lower electron-transfer resist

34 ) and Au(38) S(2) (SR)(20) with body-centred cubic (bcc) structure, and isostructural [Au(38) L(20) (

35 ernating nanometer layers of a body-centered-cubic (BCC) structure.

36 of the final SL structure from body-centered cubic (BCC) to face-centered cubic (FCC) through a serie

37 ing plastic deformation in the body-centered cubic (bcc) variants of these alloys.

38 igh-temperature epsilon phase (body-centered cubic; bcc) of plutonium is predicted utilizing first-pr

39 isostructural La member crystallizes in the cubic bipartite sodalite structure (Type-VII clathrate)

40 including thermotropic LCs (cholesteric LCs, cubic blue phases, achiral bent-core LCs, etc.) and lyot

41 We grew cubic boron nitride (cBN) crystals with controlled abund

42 During the sintering process, cubic boron nitride particles incorporated into the hBN

43 electronic properties of hexagonal (h-) and cubic (c-) phase AlGaInN quaternary alloys are investiga

44 le range (IQR) increase [9,200 particles per cubic centimeter (cc)] relative UFP exposure was 1.04 [9

45 itude, with a lowest value of 2 x 10(11) per cubic centimeter and most of the deep traps located at c

46 ing 5.6 +/- 1.2 percentage injected dose per cubic centimeter at 40-60 min and rapid clearance from b

47 eved a high energy density of 112 joules per cubic centimeter with a high energy efficiency of ~80%.

48 storage densities as high as ~133 joules per cubic centimeter with efficiencies exceeding 75%.

49 Its bulk density, 1.19 +/- 0.02 grams per cubic centimeter, indicates a high-porosity (>50%) inter

50 ltralow densities down to ~0.1 milligram per cubic centimeter, superelasticity up to 95%, and near-ze

51 ble at densities of 10(7) to 10(8) grams per cubic centimeter.

52 d flow of H(2) gas at a rate of 150 standard cubic centimeters per minute (sccm).

53 We assessed changes in thigh muscle volume (cubic centimeters) as the primary endpoint along with 6-

54 measured within a flare subvolume of ~10(28) cubic centimeters.

55 anometers and sample volumes on the order of cubic centimeters.

56 e in a sensing volume of approximately three cubic centimeters.

57 pressure, reach densities of 10(7) grams per cubic centimetre in their cores(2).

58 d a density of [Formula: see text] grams per cubic centimetre, similar to Earth's.

59 hydrogen density of about 10(5) to 10(6) per cubic centimetre, with the values being sensitive to the

60 n density in near-Earth space-2 x 10(-9) per cubic centimetre-confirming theoretical estimates.

61 -proceeding via topotactic reaction with the cubic close packed oxygen-anion framework retained.

62 U(84) assembles into superlattices including cubic-closest packed, body-centered cubic, and interpene

63 MOF-5, with its open cubic connectivity of Zn(4)O clusters joined by two-dime

64 Using a cubic-core hexagonal-branch mechanism to form highly mon

65 tribution of the widely studied face-centred cubic CrMnFeCoNi Cantor alloy(2) and of a new face-centr

66 ycle and typically displays a highly ordered cubic crystal structure.

67 The electroplated films have cubic crystal structures and the preferred orientation w

68 , pure metals that freeze into face-centered cubic crystals with little to no activation energy, are

69 oes not seem to be possible for face-centred-cubic crystals(3,13).

70 ers with retracted sticky patches, colloidal cubic diamond can be self-assembled using patch-patch ad

71 Self-assembling colloidal particles in the cubic diamond crystal structure could potentially be use

72 Cubic diamond is preferred for these applications over m

73 he colloidal particles in the self-assembled cubic diamond structure are highly constrained and mecha

74 scopy revealed nanoscale twinning within the cubic diamond structure.

75 h-dielectric-contrast photonic crystals with cubic diamond symmetry.

76 t-neighbour particles, which is required for cubic diamond(15,17).

77 altering patterns of cholesterol units on a cubic DNA scaffold dramatically changes its interaction

78 igh-Benard convection of Newtonian fluids in cubic enclosures have been analysed using Direct Numeric

79 Mg-doped GaN cubic epitaxial layers grown under optimized conditions

80 s) contain a brightly fluorescent stratified cubic epithelium enclosed in a pigmented sheath and in c

81 er-diffuse, ultimately forming face-centered-cubic equiatomic CoCrFeNi alloy.

82 enium nanocrystals with both a face-centered cubic ( fcc) structure and well-controlled facets are at

83 the complete transformation of face-centered cubic (fcc) Ag-NPs into monoclinic Ag(2)S-NPs.

84 ypal dislocation mechanisms in face-centered cubic (FCC) and body-centered cubic (BCC) metals.

85 4)Ni(6) alloy, comprising both face-centered cubic (fcc) and hexagonal closed packed (hcp) phases.

86 its larger atomic radius) in a face-centered cubic (FCC) CoFeNi solid solution, and a chemical orderi

87 create an interface between a face-centered cubic (FCC) crystal and its liquid.

88 base-centered cubic (bcc) and face-centered cubic (fcc) crystalline nanoparticle lattices.

89 tered cubic (BCC) crystals and face-centered cubic (FCC) crystals.

90 to the Pd lattice, the overall face centered cubic (FCC) lattice is maintained; however, short-range

91 ormation of low stacking-fault face-centered cubic (Fcc) metals but rarely found in body-centered cub

92 ation of Pd nanomaterials from face-centered-cubic (fcc) phase into amorphous phase without destroyin

93 hich the original single-phase face-centered-cubic (FCC) structure partially transforms into alternat

94 l a polymorphic transition from face-centred-cubic (fcc) structure to hexagonal-close-packing (hcp) s

95 pically stable as a solid in a face-centered cubic (FCC) structure under ambient conditions; however,

96 a monotwinned/stacking-faulted face-centered-cubic (fcc) structure.

97 m body-centered cubic (BCC) to face-centered cubic (FCC) through a series of body-centered tetragonal

98 linker and the metal node in a face-centered cubic (fcu) MOF, we tune the adsorption of CO(2), pore o

99 ion disorder) leads to larger amounts of the cubic Fd3m phase resulting in the observed photoluminesc

100 In a magnetic field, cubic Fe(3) O(4) nanoparticles exhibit assembly behavior

101 o better tune the face-to-face interactions, cubic Fe(3) O(4) nanoparticles were functionalized with

102 es, we had previously integrated mesoporous, cubic ferritin crystals with hydrogel networks, resultin

103 ase changes the structure from the primitive cubic ([Formula: see text]) to the double diamond phase

104 examer (U(6)) oxoclusters into body-centered cubic frameworks, while smaller Ln(III) (Ln = Er-Lu and

105 crown-like dendrimers self-organize a Pm3 n cubic (Frank-Kasper A15) phase which exhibits chirality

106 We have studied the Mg doping of cubic GaN grown by plasma-assisted Molecular Beam Epitax

107 icrometer-scale single-crystal body-centered cubic gold nanoparticle superlattices, with dye molecule

108 e in the Cantor alloy and other face-centred cubic high-entropy alloys, are promoted by pronounced fl

109 f liquid water as well as hexagonal (Ih) and cubic (Ic) ice are predicted based on density functional

110 ced phase transformation from a body-centred-cubic ice phase (probably ice X) to a novel face-centred

111 romechanical response of crystalline phases (cubic iron oxide and alpha-quartz) inherently present wi

112 crystalline phases were observed wherein the cubic iron oxide crystals laterally expanded during the

113 n-Fermi-liquid behavior of the body-centered cubic iron phase, hence, reducing the EES; the total cal

114 Observations from the formation of a 0.8-cubic kilometer basaltic caldera at Kilauea Volcano in 2

115 tion was caused by lateral migration of >0.4 cubic kilometers of magma into the rift zone, extinguish

116 Several cubic kilometers of magma were stored in the reservoir,

117 e estimates are roughly equivalent-about 0.8 cubic kilometers.

118 orded place cells in rats as they explored a cubic lattice climbing frame which could be aligned or t

119 e two and three-state majority-vote model on cubic lattice networks.

120 his material crystallizes in a body-centered cubic lattice with the lattice constant a = 3.41(1) angs

121 ted as beads-on-a-string and stored in a 3 D cubic lattice.

122 [2.2.2]octane dicarboxylate linker in a Zn4O cubic lattice.

123 estrict the increase in permeability and the cubic law used to relate porosity and permeability in mo

124 ther premartensite (T1) phase with preserved cubic-like symmetry through an isostructural phase trans

125 ere, we report the first alternating network cubic liquid crystals.

126 rs co-organize into Ia3 d -type bicontinuous cubic liquid-crystalline mesophases through nanosegregat

127 ion of the crystal optic axis along a pseudo-cubic <111> direction.

128 The magnetic state of this cubic material is characterized by a 3-k non-collinear a

129 ral and tetragonal nanodomains embedded in a cubic matrix.

130 With a space density of about 2 x 10(-5) per cubic megaparsec (two orders of magnitude higher than ex

131 a co-moving number density up to 10(-3) per cubic megaparsec.

132 is retained in a broad class of face-centred cubic metals with low stacking fault energies when tunin

133 ate that energy use and carbon footprint per cubic meter of wastewater treated, varies markedly with

134 1-unit increase in PM2.5 (in micrograms per cubic meter) was associated with a 3.53% decrease in bas

135 in Gale crater is 1680 +/- 180 kilograms per cubic meter.

136 n the island of Hawai'i injected millions of cubic meters of molten lava into the nutrient-poor water

137 ctivity in 2014 and an estimated 4.5 billion cubic meters of total gas volume flared over the study p

138 Lava erupted at rates exceeding 100 cubic meters per second, eventually covering 35.5 square

139 stimated to be approximately 20 000 trillion cubic meters.

140 ly high number density (more than 10(24) per cubic metre) and small size (about 2.7 +/- 0.2 nanometre

141 tical clocks occupy volumes of more than one cubic metre, and it is a substantial challenge to enable

142 at the case study breaks-even at $0.2944 per cubic metre.

143 The Raman measurements showed that cubic Mg(2)TiO(4) spinel transforms to a high pressure t

144 iffraction experiment, transformation of the cubic Mg(2)TiO(4) to the tetragonal structure was comple

145 The results show that the cubic microlattice has mechanical strength comparable to

146 he cell volume decreases by several thousand cubic micrometers, corresponding to large pressure chang

147 n at platelet-count thresholds of 50,000 per cubic millimeter (high-threshold group) or 25,000 per cu

148 limeter (high-threshold group) or 25,000 per cubic millimeter (low-threshold group).

149 e in the CD4+ T-cell count was 139 cells per cubic millimeter and 64 cells per cubic millimeter, resp

150 ording to blood eosinophil count (>/=150 per cubic millimeter at screening or >/=300 per cubic millim

151 cubic millimeter at screening or >/=300 per cubic millimeter during the previous year).

152 at a platelet-count threshold of 50,000 per cubic millimeter had a significantly higher rate of deat

153 ee dimensional (3D) microvascular imaging of cubic millimeter to centimeter size volumes often requir

154 men; the median CD4+ count was 470 cells per cubic millimeter, and half the patients were receiving a

155 cells per cubic millimeter and 64 cells per cubic millimeter, respectively.

156 rs, and the mean CD4 count was 337 cells per cubic millimeter.

157 at a platelet-count threshold of 25,000 per cubic millimeter.

158 d had CD4+ T-cell counts below 100 cells per cubic millimeter.

159 eosinophil count of at least 1000 cells per cubic millimeter; all the patients were receiving stable

160 nsional (3D) multicolor imaging over several cubic millimeters as well as brain-wide serial 2D multic

161 Garnet is the archetypal cubic mineral, occurring in a wide variety of rock types

162 SD and tensile strength responses; while the cubic model demonstrated a good relation between indepen

163 m MOFs, obtaining pure hexagonal PCN-223 and cubic MOF-525 phases in 20-60 min of milling.

164 ts between 2007 and 2017(15), we find that a cubic moment-duration scaling law is more likely.

165 This cubic n-type phase has promising thermoelectric properti

166 ble water oxidation electrocatalyst based on cubic nanocages with a composition of Ir(44) Pd(10) , to

167 e, which yields highly textured body-centred cubic nanograins above a transition temperature.

168 he smallest, monodisperse cage-shaped silica cubic nanoparticle, is exceptionally interfacially activ

169 particles) with a large-pore (~40 nm) single cubic network (Pm3m).

170 templating strategy using sacrificial double cubic network polymer cubosomes (Im3m) to synthesize ord

171 ass of the rBC cores was proportional to the cubic of their d(mob).

172 s the structure than the originally proposed cubic one.

173 u2Se nanocrystals were synthesized in either cubic or hexagonal (metastable) crystal structures and u

174 me (mass) or surface area and hence follow a cubic or square relationship with the cell radius.

175 TPA) occuring in silicon carbide with either cubic or wurtzite structure.

176 rough a series of phase transitions from the cubic P2(1)3, through orthorhombic P2(1)2(1)2(1) and mon

177 t is the most compact and close to the ideal cubic packing among the Al-B-C phases containing B(12)-t

178 For cubic particles, the contribution of the higher-order mo

179 PFWO should be described by a partly ordered cubic perovskite (i.e. Fm - 3m), (2) the weak ferromagne

180 om its hexagonal non-perovskite phase to the cubic perovskite polymorph, where the growth kinetics ar

181 hough they are based on the nominally simple cubic perovskite structure, these compounds are in fact

182 ovided by Al(2)O(3)(0001) and (111) oriented cubic perovskites, are promising candidates for epitaxy

183 e roles of Co and Fe in the OER mechanism of cubic perovskites, two prospective perovskite oxides, La

184 membrane protein (MP) properties in lipidic cubic phase (LCP) is important for studying complicated

185 e use of lipids capable of forming a lipidic cubic phase (LCP).

186 y stable nanoparticles formed from the lipid cubic phase and stabilized by a polymer based outer coro

187 ce the structure distortion to stabilize the cubic phase at the few-nanometer size.

188 Cubic phase CsPbI(3) quantum dots (alpha-CsPbI(3) QDs) a

189 The trigonal R-phase is formed from the cubic phase during cooling to room temperature and subse

190 , enhanced disorder and stabilization of the cubic phase even for a small amount of dimethylammonium

191 l structure of pristine GeTe transforms into cubic phase in (GeTe)(100-x)(AgBiSe(2))(x) for x >= 25,

192 The first single-diamond cubic phase in a liquid crystal is reported.

193 Our results show that the cubic phase is a suitable alternative to generate a high

194 the phase transition from the tetragonal to cubic phase near T(C) is a change in the surroundings of

195 Theory predicts a dense face-centred-cubic phase of cobalt, which would be nonmagnetic.

196 iodide passivation strategy to stabilize the cubic phase of CsPbI(3), achieving the facile synthesis

197 en 300 K and 4800 K), only the face-centered cubic phase of platinum has been observed.

198 ontinuities can be explained by a tetragonal-cubic phase transition in Ti-bearing CaSiO(3) perovskite

199 o a reversible, photoinduced orthorhombic-to-cubic phase transition which is discernible at fluences

200 ng the occurrence of a phase transition to a cubic phase with higher symmetry than tetragonal.

201 ); whereas the Raman lines (forbidden in the cubic phase) remain until ca. 17 GPa, where a monoclinic

202 that CQDs keep the perovskite in its desired cubic phase, suppressing the transition to the undesired

203 more resistant in the monoclinic than in the cubic phase, which may be related to the lower bandgap o

204 ism of the transition from the tetragonal to cubic phase.

205 h may be related to the lower bandgap of the cubic phase.

206 h octahedral rotation is not possible in the cubic phase.

207 Here, we developed biocompatible cubic-phase (alpha-phase) erbium-based rare-earth nanopa

208 f proteins within lipid inverse bicontinuous cubic phases (Q(2)) has been widely studied for many app

209 Bicontinuous lipid cubic phases consist of a single lipid bilayer that form

210 lude crystallization in inverse bicontinuous cubic phases for membrane protein structure determinatio

211 membrane composition yields 3D bicontinuous cubic phases that swell up to lattice dimensions of 68 n

212 ng requirements of six possible bicontinuous cubic phases, that is, the single- and double-network ve

213 lipids and lipids promoting hexagonal II or cubic phases.

214 fluid and its properties are derived from a Cubic Plus Association (CPA) equation of state.

215 R[Formula: see text], orthorhombic Pbnm, and cubic Pm[Formula: see text]m respectively.

216 Response surface modeling using a cubic polynomial model of the bootstrapped sPLS-DA avera

217 pagates through diamond nanotwins of the 3C (cubic) polytype along {111} planes, via a zigzag path.

218 n plus Unbalanced Breeding-like Inter-Cross (CUBIC) population, consisting of 1404 individuals create

219 r tuning of the reaction conditions yields a cubic porous network compound (3) where {P(8) W(48) } cl

220 hexanuclear secondary building unit and form cubic, porous, and intrinsically conductive structures,

221 ype based on the pore-space partition of the cubic primitive minimal-surface net (MOF-14-type) has be

222 dopts ST-turn secondary structure, promoting cubic Pt nanocrystal formation at low concentration, and

223 The beta-sheet T7-Pt{100} specificity drives cubic Pt nanocrystals to self-assemble into large-area,

224 wer degree of electronic excitation than for cubic pyrochlore La(2)Zr(2)O(7).

225 transition from L(3) to inverse bicontinuous cubic (Q(2)) phase.

226 ndow analyses were best fit with quartic and cubic regression models for CT and FSSC/BSSC, respective

227 hods that relax the assumption of linearity: cubic regression splines and fractional polynomials.

228 Cubic-restricted splines and multivariable log-Poisson r

229 linearly with temperature, while below it, a cubic scaling is displayed.

230 hape at the beginning and transformed into a cubic shape afterward.

231 uring the Cu(2)O growth and dissolution, the cubic shape evolved with specific planes in the {100} fa

232 Cubic-shaped cobalt ferrite nanoparticles (Co-Fe NCs) se

233 compound (3) where {P(8) W(48) } clusters as cubic sides are joined by 4 Ag(+) ions to give a cubic a

234 Bulk analyses of each solid confirm a cubic sodalite-type structure (P43n, No.

235 A 2-dimensional interpolation with a cubic spline fits a response surface to determine the be

236 ng multivariable Cox modeling and restricted cubic spline function.

237 e relationships were modeled with restricted cubic spline functions that compared 7.5, 15.0, 22.5, an

238 -year OS or DFS was plotted using restricted cubic spline functions.

239 ated with descriptive plots using restricted cubic spline functions; associations were quantified usi

240 A restrictive cubic spline method was used to estimate the dose-respon

241 Natural cubic spline models indicated a mostly linear associatio

242 We applied restricted cubic spline models to evaluate the dose-response relati

243 Restricted cubic spline regression characterized dose-response rela

244 fit a dose-response curve using a restricted cubic spline regression model.

245 Nonlinearity was tested by restricted cubic spline regression.

246 as a continuous variable, using a restricted cubic spline with adjustment for the same covariates as

247 baseline PaO2/FIO2 (modeled with restricted cubic spline), baseline positive end-expiratory pressure

248 d in only two models (e.g., using restricted cubic spline).

249 inflammatory marker modeled as a restricted cubic spline, higher levels of IL-6 and TNF-alpha were m

250 inflammatory marker modeled as a restricted cubic spline, higher levels of IL-6 and TNF-alpha were m

251 yroxine (FT4) concentration using restricted cubic-spline regression models.

252 Restricted-cubic-spline regression, adjusting for a priori potentia

253 After log-transforming ACR and PCR, we used cubic splines and quantile regression to estimate the me

254 lity rates, and 95% CIs were estimated using cubic splines and quartile classifications adjusting for

255 btained hazard ratios (HRs) using restricted cubic splines based on Cox proportional hazards models.

256 ined using multivariable-adjusted restricted cubic splines based on Cox proportional hazards models.

257 We demonstrate that cubic splines can capture the shape of any PSF with high

258 Risk-adjusted restricted cubic splines modeled the probability of each complicati

259 Restricted cubic splines revealed a U-shape association between BMI

260 aim was to model volume by using restricted cubic splines to determine the association between volum

261 We used restricted cubic splines to relax linearity assumptions and bootstr

262 On the basis of the cubic splines, we created models using linear splines to

263 near associations were studied by restricted cubic splines.

264 s relationship was examined using restricted cubic splines.

265 Here, a pseudo-cubic SrCo(0.9)Ir(0.1)O(3-delta) perovskite, containing

266 embly of a Sierpinski triangular prism and a cubic star possessing three and six cavitand-based motif

267 apsule, a Sierpinski triangular prism, and a cubic star, could be readily obtained through dynamic co

268 her than the SCN(-) , maintaining the intact cubic structure and facilitating interparticle electrica

269 scale cuboidal particles with a bicontinuous cubic structure by amphiphilic poly(ionic liquid) dibloc

270 However, once the symmetry of the cubic structure is broken by substituting Ti for Zr, it

271 g rise to phase transitions from a nonchiral cubic structure to an incommensurate electric dipole and

272 materials are nanocrystalline (face-centered cubic structure) and show reversible voltage-driven ON-O

273 in addition to the well-known face-centered cubic structure, including hexagonal close-packed (hcp)

274 nerally attributed to internal strain of the cubic structure.

275 als show stability with the alpha-Sn diamond cubic structure.

276 lly conductive MOFs reported to date exhibit cubic structures that enable isotropic charge transport.

277 c characteristic of Ia3 d -type bicontinuous cubic structures that they are composed of intertwined r

278 f-assembled structures, such as face-centred-cubic structures(9,10), because diamond has a much wider

279 ase (probably ice X) to a novel face-centred-cubic, superionic ice phase, which we name ice XVIII(2,1

280 ng frames at their vertices, which result in cubic superlattices with a 48 nm unit cell.

281 Indeed, a non-cubic symmetry appears to be typical of common garnet th

282 ely, the solid solutions (y = 1 to 7) retain cubic symmetry down to 1.5 K.

283 termination of the gyroid surface breaks the cubic symmetry of the bulk lattice and gives rise to the

284 highlighted by interactions that disrupt the cubic symmetry of the GaAs lattice, resulting in quadrup

285 Here we show that common garnet with a non-cubic (tetragonal) crystal structure is much more widesp

286 owires) and controlled crystal phases (e.g., cubic, tetragonal and multi-phase).

287 trahedra template the Sn atoms into a chiral cubic three-connected net of the SrSi(2) type.

288 (seconds) of micrometre-sized, face-centred-cubic, three-dimensional nanocrystal superlattices durin

289 This slowness is even more severe than cubic-time free energy minimization due to a substantial

290 t 4, and the volume reduction on change from cubic to tetragonal phase is about 9%.

291 therwise suspended by diffusionless athermal cubic-to-rhombohedral phase transition at around 700 K.

292 lar, it is widely accepted that in a classic cubic-to-tetragonal phase transformation, with only thre

293 remain until ca. 17 GPa, where a monoclinic-cubic transition is known in lead titanate.

294 Pa, where a monoclinic (M(c)) but metrically cubic transition occurs from the ambient tetragonal P4 m

295 new type of Mn-rich Heusler compound with a cubic unit cell, a = 0.9150 nm in Ni-Mn-In and a = 0.905

296 notably, a crystal with 432 particles in the cubic unit cell.

297 We compute the one-loop corrections due to cubic vertices, finding additional terms that are absent

298 expansion produces an effective theory with cubic vertices.

299 analyzed with and without resampling to 2-mm cubic voxels.

300 Alkali PBAs are typically cubic with both MC(6) and M'N(6) octahedral coordination