ライフサイエンスコーパス: cubic

1 ly grown hexagonal zinc oxide (ZnO) films on cubic (001)-magnesium oxide (MgO) substrates using advan

2 s of tetragonal L10 FePt (001) easy-axis and cubic A1 FePt thin films via time-domain thermoreflectan

3 with 3D point spread functions using a least-cubic algorithm and collation.

4 ed dark-field (EDF) illumination and a least-cubic algorithm.

5 ion reveals a continuous transition from the cubic alpha-phase (Pm3 m, #221) to a tetragonal beta-pha

6 d 85Al alloys, and [am] --> [am + alpha-Al + cubic AlxMy (M = Y, Ni, Co, Fe, Pd)] --> [am + alpha-Al]

7 ely poor p-type thermoelectric material, the cubic analogue is calculated to have high efficiencies f

8 d compute the free energy difference between cubic and hexagonal ice interfaces with vapor.

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

10 ter model to show that the entropy of mixing cubic and hexagonal layers makes stacking-disordered ice

11 ication of unambiguous optical signatures of cubic and hexagonal phases in II-VI nanocrystals using a

12 selenide, which exist as two stable phases, cubic and hexagonal, each with distinct properties.

13 error rate estimation approach that employs cubic and robust smoothing splines to model the relation

14 lass of colloidal superstructures, including cubic and tetragonal colloidal crystals, with no known a

15 lectronic structure and superconductivity in cubic and tetragonal TiH2.

16 mprising internally V2 (inverse bicontinuous cubic) and H2 (inverse hexagonal) nanoarchitectures was

17 (Li2Fe)ChO (Ch = S, Se) possess cubic anti-perovskite crystal structures, where Fe and L

18 liquid states of matter that exhibit ordered cubic arrangements of topological defects.

19 f icy interstellar objects (2.4 x 10(-4) per cubic astronomical unit) suggests that some should have

20 sor state with the preserved symmetry of the cubic austenite phase.

21 (hexagonal close packed hcp) to body center cubic (bcc) crystal structure at ambient pressures.

22 own in entropically stabilized body-centered cubic (BCC) crystals due to the thermal excitations of t

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

24 ead of the previously reported body-centered cubic (BCC) or face-centered-cubic (FCC) types, the majo

25 ese spheres self-organize in a body-centered cubic (BCC) periodic array, rarely encountered for self-

26 ysis showed the formation of a body centered cubic (bcc) Pu4O7 structure on the goethite surface, con

27 = 42 degrees C, an equilibrium body-centered cubic (BCC) structure forms, whereas below TOOT the Fran

28 centered tetragonal (bct) and body centered cubic (bcc) structures.

29 face-centered-cubic (fcc) and body-centered-cubic (bcc) superlattice, respectively, at concentration

30 The recently discovered body-centered cubic (BCC) Ta-Nb-Hf-Zr-Ti high-entropy alloy supercondu

31 wo-material simple cubic (SC), body centered cubic (BCC), and face centered cubic (FCC) crystal struc

32 ll beta-brass CuZn alloy phase (body-centred cubic, bcc) which appears to greatly stabilise Cu atoms

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

34 atterned crystallographic orientation of the cubic blue phase, soft lattice.

35 n frustrated liquid-crystalline phases, like cubic blue phases, is a formidable task.

36 imensional Boron Nitride (BN) forms, namely, cubic-BN (c-BN) nanodots (NDs), offers a variety of nove

37 diamond with the higher thermal stability of cubic boron nitride (cBN) have broad potential value in

38 alent superhard materials such as diamond or cubic boron nitride.

39 m low temperature form the hexagonal C14 and cubic C15 Laves phases commonly found in metal alloys.

40 This cubic cage is flexible and compatible with aqueous media

41 on of tetrahedral Fe(II)4L6 cages instead of cubic cages.

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

43 tracer uptake (percentage injected dose per cubic centimeter, 0.95 +/- 0.04 vs. 1.87 +/- 0.11; P < 0

44 ensity of 7.7 +/- 1.1 x 10(23) particles per cubic centimeter, which is consistent with theoretical e

45 Plasma densities reached up to 1000 cubic centimeters, and electron temperatures were below

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

47 ity of 40 microgal per hertz(1/2) only a few cubic centimetres in size.

48 both the tetrahedral cation coordination and cubic close packed anion sublattice of digenite Cu2-x S.

49 cture of alpha-boron, or, equivalently, as a cubic close packing of B12 icosahedra with two oxygen at

50 lative to other accessible structures having cubic close-packed anions and/or octahedrally coordinate

51 ike lyotropic phases including hexagonal and cubic close-packed arrangements of spherical and cylindr

52 y the Dzyaloshinskii-Moriya interaction, the cubic compound FeGe exhibits helimagnetism with a relati

53 as was significantly higher than that of the cubic-containing zirconia (e.g., Zpex Smile) and lithia-

54 nd zirconias, including the most translucent cubic-containing zirconias.

55 Based on the integration of hexagonal-cubic core-shell architecture with nanorod morphology, t

56 Twin nucleation in a face-centered cubic crystal is believed to be accomplished through the

57 preserving the quantum dot in the desirable cubic crystal phase.

58 lectron microscopy (HAADF-STEM) revealed the cubic crystal structure and surface termination of the N

59 tation values, even in materials with simple cubic crystal structure such as Ba2NaOsO6.

60 synthesized perovskite NPLs exhibit a single cubic crystal structure, a 1.6-fold enhanced photolumine

61 In spite of the simple body-centered-cubic crystal structure, the elements of group V, vanadi

62 es formed between the materials with diamond cubic crystal structures studied in this work, the prese

63 es comprised of materials exhibiting diamond cubic crystal structures, higher conductances are observ

64 chanism of crystallization to a face-centred cubic crystal.

65 superconductivity in hole-doped diamond-like cubic crystalline hydrocarbon K 4-CH (space group I21/3)

66 Nanoclusters were crystallized as cubic crystals (</=0.5 mm in size) after solvothermal tr

67 NA bonding elements results in body-centered cubic crystals, whereas DNA functionalization of cystein

68 high as approximately 90 T-the highest among cubic crystals.

69 Here, a low-temperature procedure to form cubic CsPbI3 has been developed through a halide exchang

70 However, small-bandgap cubic CsPbI3 has been difficult to study due to challeng

71 The exposure of cubic Cu2Se nanocrystals to Pb(2+) cations led to the in

72 to the absence of preferred entry points in cubic Cu2Se.

73 ominant shear band starting with the diamond-cubic (dc) to diamond-hexagonal (dh) phase transition an

74 ectron-phonon coupling, as compared with the cubic delta-NbN counterpart.

75 tely 20 GPa and is significantly harder than cubic delta-NbN; it is as hard as sapphire, ultra-incomp

76 ctive accommodation of ductile body-centered cubic dendrites at 77 K, characteristic of the prevailin

77 ll-defined material but is instead defective cubic diamond formed under high pressure and high temper

78 ze, and optimized fractions of face-centered cubic (f.c.c., gamma) and hexagonal close-packed (h.c.p.

79 M8-SBU is composed of eight M(IV) ions in a cubic fashion linked by eight mu2-oxo and four mu2-OH gr

80 ne self-assemble into a single face-centered-cubic (fcc) and body-centered-cubic (bcc) superlattice,

81 and one sulfido ligand with a face-centered cubic (FCC) Au22 kernel.

82 s a superstructure composed of face-centered cubic (fcc) close-packing of near-spherical C60 superato

83 body centered cubic (BCC), and face centered cubic (FCC) crystal structures and show that in each of

84 equatomic CrMnFeCoNi with the face-centered cubic (FCC) structure is noteworthy because its ductilit

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

86 found to adopt a sodalite-like face-centered cubic (fcc) structure, stable above 200 GPa, and LaH8 a

87 d body-centered cubic (BCC) or face-centered-cubic (FCC) types, the major structure was found to show

88 The actual ground state is face-centered cubic (fcc).

89 icient layered analogue of the face-centered cubic fcu UiO-67(Hf).

90 ata and were linear for 9, quadratic for 25, cubic for 2, logarithmic for 6, and power law for 4 usin

91 were linear for 9 regions, quadratic for 13, cubic for 6, logarithmic for 12, power law for 7, and mo

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

93 ize, and closure rate can be modelled with a cubic function.

94 The complex consists of a central roughly cubic [FXN(42-210)]24.[ISCU]24 sub-complex with one symm

95 responses as functions of time of two n type cubic GaN Schottky diodes (200 mum and 400 mum diameters

96 The synthesis of the cubic gauche allotrope of high energy density polymeric

97 The long-sought cubic gauche phase of polymeric nitrogen (cg-PN) with ni

98 d stabilization of polymeric nitrogen in its cubic gauche phase under near-ambient conditions, via pl

99 Diamond-cubic germanium is a well-known semiconductor, although

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

101 The appropriate peaks for the face centred cubic gold were (111) and (200), as seen from X-ray diff

102 ooked-for hypothetical polybenzene (pbz) or "cubic graphite" structure, described 70 years ago.

103 parsity value search space as opposed to the cubic grid search required by other model selection meth

104 t the superconducting phase is body-centered cubic H3 S (Im3 m, a=3.089 A) resulting from the decompo

105 s with different equilibrium Wulff shapes: a cubic habit from cube-shaped nanoparticles, a rhombic do

106 Here we describe a cubic host obtained from the self-assembly of Fe(II) and

107 ict that the free energy penalty against the cubic ice interface should decrease strongly with temper

108 Cubic ice is disfavored with respect to hexagonal ice no

109 onclude that selective growth of the elusive cubic ice polymorph by manipulation of the interfacial p

110 by favoring the formation of nuclei rich in cubic ice, which, as demonstrated by us earlier, are mor

111 with the reentrance of the high-temperature cubic Im3 phase.

112 The emitters originate from cubic inclusions in hexagonal lattice and exhibit narrow

113 rsus applied magnetic field of the MR in the cubic intermetallic compound GdPd3.

114 load partitioning between the body-centered-cubic iron matrix and NiAl-type precipitates in a ferrit

115 We have synthesized cubic -KCl3 at 40-70 GPa and trigonal -KCl3 at 20-40 GPa

116 s of observational data showing that ~87,000 cubic kilometers of ice have accumulated at the poles si

117 volcanic super-eruptions of several hundred cubic kilometres or more generate long run-out pyroclast

118 mechanism for a unique catalytic behavior of cubic lambda-MnO2 .

119 o retain the P213 space group, though with a cubic lattice parameter of a = 9.11176(8) A that is sign

120 pressure and 298 K, Li forms a body-centered cubic lattice, which is common to all alkali metals.

121 [2.2.2]octane dicarboxylate linker in a Zn4O cubic lattice.

122 he extended Bose-Hubbard model on the simple cubic lattice.

123 with sulfur atoms arranged on a body-centred cubic lattice.

124 order and thermal fluctuations in the simple cubic lattice.

125 ing and tailoring the ordering of such soft, cubic lattices along predetermined or desired directions

126 en random walks and Hamiltonian subchains on cubic lattices, identifying a regime of open curves in w

127 stoichiometry, which are composed of simple cubic like phosphorus layers capped with hydrogen atoms

128 ated octahedral core with bulk face-centered cubic-like arrangement, yet a nanomolecule with a precis

129 Surprisingly, our data showed a cubic-like pattern of dependencies with positive and neg

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

131 Traditional 3D bicontinuous cubic lipid materials appear as a polycrystal of varying

132 bismuth sulphide were prepared from inverse cubic lipid mesophases.

133 g of a crystallographic direction of a soft, cubic liquid-crystal superstructure, exhibiting an alter

134 has been demonstrated with the synthesis of cubic LiZnSb by a low-temperature solution-phase method.

135 porphyrins with Fe(II) or Zn(II) gave a new cubic M(II)8L6 cage framework with electron-deficient wa

136 r reveal that [Yfh1]24.[Isu1]24 is a roughly cubic macromolecule consisting of one symmetric Isu1 tri

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

138 is method we shock-compress the body-centred-cubic material tantalum-an important material for high-e

139 ast to the 1/T(2) dependence found in pseudo-cubic materials such as SrTiO3 or KTaO3.

140 protein concentration in the bilayer of the cubic mesophase can be ramped up stepwise from less than

141 constitution of membrane proteins in lipidic cubic mesophases plays a prominent role in membrane prot

142 constitution of membrane proteins in lipidic cubic mesophases presents significant challenges related

143 ingle-crystal plasticity in the body-centred-cubic metal tantalum.

144 The results match the predicted cubic metallic phase of LaH10 having cages of thirty-two

145 thus be highly unfavorable in face-centered cubic metals with high twin-fault energy barriers, such

146 plasticity in heavily twinned face-centered cubic metals, with the potential for optimizing mechanic

147 th exposure to PM2.5 of less than 12 mug per cubic meter and ozone of less than 50 ppb, the same incr

148 dded NOx, SO2, PM2.5, and CO2 emissions on a cubic meter basis.

149 s will impose average net costs of $3.01 per cubic meter for chemical precipitation and biological wa

150 ted with exposure to increases of 10 mug per cubic meter for PM2.5 and 10 parts per billion (ppb) for

151 ological wastewater treatment and $11.26 per cubic meter for zero-liquid discharge wastewater treatme

152 he largest IHD health benefits per microgram/cubic meter from PM2.5 air pollution control may be achi

153 Increases of 10 mug per cubic meter in PM2.5 and of 10 ppb in ozone were associa

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

155 Approximately 150 billion cubic meters (BCM) of natural gas is flared and vented i

156 commonly used least-square method, the least-cubic method was more useful for finding the center in a

157 a core density of 2,460-2,900 kilograms per cubic metre (that is, composed of CI and CM chondrites),

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

159 tions of 10(-4.5) to 10(-0.5) micrograms per cubic metre).

160 ying the megathrust of 150-200 kilograms per cubic metre.

161 ty of the nucleus is 533 +/- 6 kilograms per cubic metre.

162 avitational point mass is GM = 666.2 +/- 0.2 cubic metres per second squared, giving a mass M = (9,98

163 ion; the median CD4+ count was 340 cells per cubic millimeter (interquartile range, 117 to 431).

164 The median CD4 count was 530 cells per cubic millimeter among 3490 primarily black African HIV-

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

166 a blood eosinophil count of at least 150 per cubic millimeter at screening or at least 300 per cubic

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

168 millimeter at screening or at least 300 per cubic millimeter during the previous year.

169 ecutive CD4+ counts fell below 250 cells per cubic millimeter or if an illness indicative of the acqu

170 enrollment (CD4+ count, 350 to 550 cells per cubic millimeter).

171 Plasmodium falciparum of >2500 parasites per cubic millimeter).

172 median baseline CD4+ count was 37 cells per cubic millimeter, but 854 patients (47.3%) were asymptom

173 ith a CD4+ count of fewer than 100 cells per cubic millimeter.

174 nce properties of these giant QDs, with only cubic nanocrystals sufficiently bright and stable to be

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

176 y can localize light to volumes well below 1 cubic nanometer ("picocavities"), enabling optical exper

177 ight to volumes typically on the order of 30 cubic nanometers.

178 Herein we present a simple way to prepare cubic nanoparticles of block copolymers by self-assembly

179 oliton gates) as they become possible in the cubic non-linear Schrodinger equation (3NLSE) domain, an

180 st in studying modulation instability in the cubic nonlinear Schrodinger equation, a generic model fo

181 lonomic, nonautonomous dynamical system with cubic nonlinearity.

182 thesized that the smaller microplastics, the cubic ones mostly, are fragmented much faster than the p

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

184 rritin-MOFs with the expected body-centered (cubic or tetragonal) lattice arrangements.

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

186 Up to cubic-order nonlinearities allow for an instantaneous es

187 ites under high pressure: during the drastic cubic-orthorhombic structural transformation at approxim

188 ion of central blocks evidently induce solid cubic particle formation.

189 racterization of packings of non-overlapping cubic particles.

190 separate dependencies described the original cubic pattern well.

191 ter vapor sorption studies on four primitive cubic, pcu, pillared square grid materials: SIFSIX-1-Cu,

192 The lipid cubic phase (in meso) method is an important approach fo

193 We used GPCR engineering and lipidic cubic phase (LCP) crystallization to determine the struc

194 The lipidic liquid-crystalline cubic phase (LCP) is a membrane-mimetic material useful

195 has previously been crystallized in lipidic cubic phase (LCP), structural differences in the Cmpd-1-

196 density of states at the Fermi level in the cubic phase arises from Ti-t2g states and leads to a str

197 ambient pressure transforms to a ReO3 -type cubic phase at 0.3 GPa.

198 are able to form an isotropic sphere in the cubic phase due to rapid molecular motion at high temper

199 The cubic phase has a large electron-phonon coupling paramet

200 rporating a component of optically isotropic cubic phase into the tetragonal structure.

201 Furthermore, the cubic phase is found to be the energetically favored pol

202 In the Y2O3 layer, the original cubic phase is observed to transform to the monoclinic p

203 le and a solvent, the ability to tune the 3D cubic phase nanostructure, lipid bilayer properties and

204 d organic cation halide perovskites, but the cubic phase of bulk CsPbI3 (alpha-CsPbI3)-the variant wi

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

206 hile usage of 1,4-benzoquinone preserves the cubic phase of CsPbI3 QD.

207 We demonstrate a cubic phase plate with a point spread function exhibitin

208 tition between ionic and covalent bonding in cubic phase providing a link between the chemical basis

209 with the tetragonal distortion, allowing the cubic phase to be stable at low temperatures.

210 n to undergo transitions from a parent gamma cubic phase to beta and alpha structures on cooling.

211 uble additives into the bicontinuous lipidic cubic phase under excess hydration are summarized.

212 he first incorporation of NKA into a lipidic cubic phase with consequent enzyme functionality and sta

213 he power exponent gamma = 1.4 +/- 0.1 in the cubic phase, indicating an acoustic-phonon-dominated car

214 orthorhombic Li2 OHCl to a room-temperature cubic phase, which shows electrochemical stability to 9

215 tudy due to challenges forming CsPbI3 in the cubic phase.

216 mposite electrolytes have been prepared with cubic-phase Li7 La3 Zr2 O12 (LLZO) garnet and polyethyle

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

218 A 900 nm thick TiO2 simple cubic photonic crystal with lattice constant 450 nm was

219 The intact samples (fresh and dried cubic pieces) released significantly more aroma compound

220 ic pieces, fresh puree) and two dried (dried cubic pieces, dried powder) products were prepared from

221 Two fresh (fresh cubic pieces, fresh puree) and two dried (dried cubic pi

222 tion and phase behavior are modeled with the cubic-plus-association equation-of-state.

223 It was found that CaCeTi2O7 (cubic pyrochlore) formed as an intermediate phase during

224 ed in Random Struct. Alg. 21, 397 (2002) for cubic random regular graphs, leaving little room for imp

225 Cubic-restricted splines and multivariable log-Poisson r

226 mics studies suggest that the melting of the cubic rock-salt phases is initiated at the vacancies, wh

227 In addition, packing of cubic salt crystals arise in various problems involving

228 nt optimized results for two-material simple cubic (SC), body centered cubic (BCC), and face centered

229 Smaller debris, with a cubic shape (below 2 mm), seems to roll at sea.

230 lithiated silver hollandite and face-centred-cubic silver metal with substantial volume expansion.

231 elongation without softening in face-centred-cubic silver nanocrystals, where crystal slip serves as

232 lization of super-swelled lipid bicontinuous cubic single crystals: (i) organic solvent drying speed,

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

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

235 12 O24 )Nay (OH)6 x H2 O crystallizes in the cubic space group Pm3m with a=10.0476(1) A.

236 e that crystal structure and particle shape (cubic, spherical, or tetrapodal) and, thereby, emission

237 sociations were investigated with restricted cubic spline (RCS) regression.

238 The fitted restricted cubic spline adiposity-residential density dose-response

239 Restricted cubic spline analysis was used to examine full-range ris

240 ng multivariable Cox modeling and restricted cubic spline function.

241 he use of mixed-effects model with a natural cubic spline function.

242 regression models and non-linear restricted cubic spline models as appropriate.

243 Cubic spline models confirmed these findings.

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

245 he nonlinear meta-regression with restricted cubic spline showed an almost linear inverse association

246 ox proportional hazard model with restricted cubic spline were used to evaluate the potential non-lin

247 at were conducted with the use of restricted cubic splines and adjusted for established CHD risk fact

248 is but also evaluated dose response by using cubic splines and generalized least squares regression.

249 Here we investigate the use of cubic splines as an alternative fitting approach.

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

251 Mixed-effects models with restricted cubic splines for the mean change in anthropometric z sc

252 A Cox model with restricted cubic splines identified the lowest mortality risk when

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

254 s colonoscopy, using logistic regression and cubic splines to assess temporal variation.

255 based on a fit of the experimental data with cubic splines using a stringent thermodynamic criterion

256 ivariate logistic regression with restricted cubic splines was utilized to examine the association be

257 Multivariable models with restricted cubic splines were used to identify a hospital volume th

258 vigorous-intensity activity using restricted cubic splines, and 2) estimated the mortality benefits a

259 In a dose-response assessment using cubic splines, elevated risk of DM was observed in US st

260 Using natural cubic splines, we plotted the hazard ratio for all-cause

261 s relationship was examined using restricted cubic splines.

262 egorically and continuously using restricted cubic splines.

263 nse analysis was modeled by using restricted cubic splines.

264 and examined the shape of associations using cubic splines.

265 s evaluated using Cox models with restricted cubic splines.

266 ase) or quantitative predictor by restricted cubic splines.

267 s in which we modeled smoking variables with cubic splines.

268 ivariable adjusted Cox models and restricted cubic splines.

269 atoms energetically prefers a face-centered-cubic stacking, to serve as a nucleus of stacking fault.

270 ilms of WO3 with an associated monoclinic-to-cubic structural reorganization.

271 , first-order transformation at 286 K to the cubic structure (Pm3m, no. 221).

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

273 The completely polymeric composition of the cubic structure renders it transparent to the Terahertz

274 alline silver nanoparticles of face-centered cubic structure with a mean size of 10 nm.

275 re packing as well as a common body-centered cubic structure.

276 o evidence of any deviation from the average cubic structure.

277 tion as it approached its final body-centred cubic structure.

278 nanowire axis, with a textured face-centered cubic structure.

279 Inverse bicontinuous cubic structures formed by lipids have been demonstrated

280 lloys exhibiting only face- or body-centered cubic structures.

281 -extended core dislocations in face-centered cubic structures.

282 l ZnO films might be manipulated on the same cubic substrate.

283 the formation of well-ordered body-centered cubic superlattices consisting of inorganic nanoparticle

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

285 Based on the cubic symmetry of the high-TC phase, it is argued that t

286 ed phenomena follow directly from the simple cubic symmetry of the photonic crystal, and can be achie

287 rnary complex, extended ternary complex, and cubic ternary complex models for 7TMR function.

288 the bite angle of five-membered chelates in cubic tetramers and resulting solvation numbers that wer

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

290 om temperature rolling induced face-centered cubic titanium (fcc-Ti) in polycrystalline hexagonal clo

291 e structure of the CsPbI3 QD transforms from cubic to orthorhombic, while usage of 1,4-benzoquinone p

292 ructure of bulk SrTiO3(STO) transitions from cubic to tetragonal at around 105 K.

293 The solution-phase periodicity of this cubic transition metal-cored supramolecular organic fram

294 can be parametrically amplified through the cubic tunneling nonlinearity in a cuprate superconductor

295 micro- and nanoparticles with a bicontinuous cubic two-phase structure, reported for the self-assembl

296 onequivalent), resulting in a 173.3-angstrom cubic unit cell enclosing 816 uranium nodes and 816 orga

297 from lamellar to hexagonal to body-centered cubic with increasing asymmetry in molecular volume frac

298 l phase transition is observed in archetypal cubic YbCu5 based heavy Fermion systems.

299 hat the crystal structure of the CdSe shell (cubic zinc-blende or hexagonal wurtzite) plays a key rol

300 -formylpyridine self-assembled to generate a cubic Zn(II)8(L(A))6 assembly.