ライフサイエンスコーパス: crystal growth

1 nt physiological inhibitor of hydroxyapatite crystal growth.

2 s is one of the most important challenges in crystal growth.

3 hile the magnetic field leads to anisotropic crystal growth.

4 they also increase the tolerance toward ice-crystal growth.

5 ted layer, created at the {010} faces during crystal growth.

6 on by X-ray crystallographic methods-that of crystal growth.

7 teins that promote or inhibit hydroxyapatite crystal growth.

8 e and act as modifiers during nucleation and crystal growth.

9 from G(T) using the Wilson-Frenkel model of crystal growth.

10 boundary, which is widely known to catalyze crystal growth.

11 ominated impedance, occurring as a result of crystal growth.

12 es a better fundamental understanding of the crystal growth.

13 enamel, taken to regulate crystal shape and crystal growth.

14 enges that are unprecedented in the field of crystal growth.

15 ization of the prism structure and deficient crystal growth.

16 y revealing routes for ex situ synthesis and crystal growth.

17 res form mesocrystals by oriented attachment crystal growth.

18 e used to teach the basics of nucleation and crystal growth.

19 y as potential additives for controlling MDM crystal growth.

20 crystallization may differ from traditional crystal growth.

21 f lateral contacts leading to nucleation and crystal growth.

22 ective surface modification, and anisotropic crystal growth.

23 ate phase (i.e., a solvent) that promotes Si crystal growth.

24 emplate for the subsequent quasiepitaxial 3D crystal growth.

25 materials were used as scaffolds for calcite crystal growth.

26 set of ice-binding proteins that control ice crystal growth.

27 nd play a marginal sterical hindrance of the crystal growth.

28 n oligomerize as a prelude to nucleation and crystal growth.

29 ic exchange, negative thermal expansion, and crystal growth.

30 "how to" guide for those interested in oxide crystal growth.

31 evelop biotechnological approaches to single-crystal growth.

32 , blocking surface sites for more productive crystal growth.

33 so relevant information on the inhibition of crystal growth.

34 ation, the kinetics of which depends only on crystal growth.

35 irus capsids for uses from bioconjugation to crystal growth.

36 e classical polynuclear theory developed for crystal growth.

37 e of the liquid structure on the kinetics of crystal growth.

38 and the physical constraints imposed during crystal growth.

39 atalysis, electrochemistry, lubrication, and crystal growth.

40 ned by kinetic effects associated with rapid crystal growth.

41 ly passivate surface defects and control the crystal growth.

42 ounded by the thermodynamics and kinetics of crystal growth.

43 l interactions that alter preferred modes of crystal growth.

44 owire growth in a manner akin to Czochralski crystal growth.

45 e of the fundamental puzzles in the field of crystal growth.

46 ntly affect nucleation but slightly retarded crystal growth.

47 lter results in phosphorus precipitation and crystal growth, (3) crystal retention takes place by fil

48 , inorganic materials via protein-influenced crystal growth--a process known as biomineralization.

49 ytically tipping the equilibrium in favor of crystal growth adding cholesterol from the membrane phas

50 ased dopants, which were used to control the crystal growth, adsorbed to the surfaces of the boron-ri

51 be valuable systems for detailed studies of crystal growth, allowing testing of theoretical concepts

52 r which there already exist industrial-scale crystal growth and advanced microfabrication techniques.

53 associated with a nonclassical mechanism of crystal growth and can trigger a self-purifying cascade

54 We term the phenomenon Plateau-Rayleigh crystal growth and demonstrate that it can be used to gr

55 ted to overcome the stochastic nature of the crystal growth and dissolution processes.

56 f important chemical transformations such as crystal growth and dissolution.

57 Such forces can be used to control crystal growth and enable surface-confinement of these m

58 critically depends on the fine tuning of the crystal growth and error correction rates within large D

59 te the thermal conductivity increases to the crystal growth and explain the thermal conductivity vari

60 n implicated in modulating calcium carbonate crystal growth and has been reported to possess an EF-ha

61 Understanding crystal growth and improving material quality is importa

62 ow that structural ordering strongly affects crystal growth and is controlled by nanorod thermal hist

63 on, these additives face-selectively inhibit crystal growth and lead to overall slower crystal appear

64 f high-temperature solutions for exploratory crystal growth and materials discovery of novel complex

65 We study the kinetics of crystal growth and melting of two types of colloidal cry

66 can then provide important information about crystal growth and particle size distributions.

67 s on ice growth, the AF(G)Ps can inhibit MDM crystal growth and recrystallization, and more significa

68 Here we describe how a different mechanism, crystal growth and scission, can accurately replicate ch

69 nd drug molecules to the inorganic surfaces, crystal growth and shape development, catalyst performan

70 can be incorporated into the cavities during crystal growth and stored inside for up to several hours

71 important implications in understanding the crystal growth and surface-related properties of MOFs.

72 e of a lack of fundamental insights into MOF crystal growth and the effect of various experimental pa

73 oteins (AFPs) have the ability to modify ice crystal growth and thus there is great interest in ident

74 regulatory effect of cryoprotectants on ice crystal growth and use this property to realize separate

75 eously as an electrode, a solvent/medium for crystal growth, and a coreactant for the synthesis of a

76 nduce recirculation in the ink for enhancing crystal growth, and engineered the curvature of the ink

77 gulating ACP-phase transformation and enamel crystal growth, and in maintaining ameloblast integrity

78 a decoupling between crystal nucleation and crystal growth, and it ensures that the grain boundaries

79 ly in the nucleation of new chemical phases, crystal growth, and other materials' transformations.

80 Here, we report synthesis, crystal growth, and structural characterization of the f

81 amine the relationships between unmixing and crystal growth, and the evolution of a nanoemulsion in a

82 This lateral confinement causes aligned crystal growth, and the smallest patterns of 0.5 mum wid

83 the interfacial characteristics, control the crystal growth, and understand the defect physics in met

84 In addition to limiting calcite crystal growth, AP7 is also observed to induce aggregate

85 Most of the established models for crystal growth are based on macroscopic thermodynamics,

86 Nucleation and crystal growth are important in material synthesis, clim

87 growth on biomineralization and spherulitic crystal growth are noted.

88 Although the effects of kinetics on crystal growth are well understood, the role of substrat

89 Additionally, the rate of crystal growth as a function of increased DNA linker len

90 metals and salts are calculated by treating crystal growth as an assignment problem through the use

91 nstrate the principal effect of As doping on crystal growth as reflected by considerably reduced aver

92 l six peptides dramatically affected calcite crystal growth (as observed by scanning electron microsc

93 rk open new avenues for the understanding of crystal growth, as well as other processes and systems i

94 behavior can be attributed to inhibition of crystal growth at microscopic length scale, as revealed

95 Studying nucleation and crystal growth at surfaces with submolecular-resolution

96 mpetent to self-assemble and control apatite crystal growth at the nanometer scale.

97 reactor, which draws from ideas of step-flow crystal growth augmented by detailed first-principles ca

98 tural-ordering processes, by which ultrafast crystal growth becomes possible.

99 probably because of the intrinsic isotropic crystal growth behavior of Pt.

100 So far, the factors preventing crystal growth beyond the favorable thickness of ca. 3 n

101 ding to kink sites, which is consistent with crystal growth by a classical mechanism.

102 ral and synthetic aragonite spherulites that crystal growth by attachment of ACC particles is more th

103 Although inhibition of crystal growth by L-cystine "imposters" at L-cystine cry

104 and form ordered mineral structures through crystal growth by particle attachment.

105 d form ordered aragonitic structures through crystal growth by particle attachment.

106 We review progress toward understanding crystal growth by particle-attachment processes and show

107 s of the copper diffusion barrier layer, the crystal growth can be controlled between a highly unifor

108 Crystal growth can be observed, quantified and controlle

109 e growth front is slow and the corresponding crystal growth can suitably be followed in time.

110 -mediated stress relaxation during epitaxial crystal growth comes from the study of inorganic heteros

111 ut screening to find suitable nucleation and crystal growth conditions.

112 Nanoscale crystal growth control is crucial for tailoring two-dime

113 thought to influence processes as diverse as crystal growth, corrosion, charge trapping, luminescence

114 his entropic component of lattice mismatched crystal growth could be used to develop unique methods f

115 es involves four critical steps: nucleation, crystal growth, crystal aggregation, and crystal adhesio

116 utilized extrinsic doping techniques or bulk crystal growth, detrimentally affecting uniformity, scal

117 that can spatially control frost formation, crystal growth, diffusion-controlled growth of biominera

118 magnetostriction of Galfenols by tuning the crystal growth direction (CGD) along the easy magnetizat

119 The method allows control of the pentacene crystal growth direction and domain-size distribution.

120 zeolite analcime and zeolite A implies that crystal growth does not always follow the classic theory

121 Now, a crystal-growth-dominated strategy is proposed to fabrica

122 ions that, in the formation of 2D COF single crystals, growth dominates over nucleation when monomers

123 ssible new model for biological control over crystal growth during amelogenesis, and hint at implicat

124 The crystal growth dynamics of the gold grains in each bicry

125 hnique is demonstrated for the Bridgman-type crystal growth enabling remote and direct measurements o

126 The OH molecules modulate the crystal growth, enhance the phase stability, passivate i

127 The slow heteroepitaxial crystal growth enlarged the perovskite crystals by 10-fo

128 ace-bound AFPs are sufficient to inhibit ice crystal growth even in solutions depleted of AFPs.

129 Through a combination of single crystal growth, experiments involving in situ deposition

130 Here, we show that the crystal growth faces of methyl alpha-D-mannopyranoside (

131 ) fix a bisignate tensor with respect to the crystal growth faces.

132 During crystal growth, faceted interfaces may be perturbed by d

133 solution and their influence upon perovskite crystal growth, film formation and device performance.

134 of capping agents in electroplating and bulk crystal growth, followed by discussion of how they affec

135 articles may dominate in the early stages of crystal growth, followed by surface crystallization, and

136 ) product, tunable bandgap and simple single crystal growth from low-cost solution processes.

137 to overcome the barrier for macroscopic ice-crystal growth from narrow cylindrical pores.

138 large mobility-lifetime product, and simple crystal growth from solution.

139 or stiffening of the melt can be induced by crystal growth from the melt or variation in oxygen fuga

140 position of the growing polymer chain on the crystal growth front as the chain is formed by the catal

141 Microporous zincophosphate sodalite crystal growth has been studied in situ by atomic force

142 ess natural and industrial processes such as crystal growth, heterogeneous catalysis, electrochemistr

143 The theory of dislocation-controlled crystal growth identifies a continuous spiral step with

144 eing capable of catalyzing ice formation and crystal growth in clouds at temperatures near 0 degrees

145 ystal hotel" microfluidic device that allows crystal growth in confined volumes to be studied in situ

146 rent crystal systems, attempts to understand crystal growth in detail have so far relied on developin

147 Antifreeze proteins prevent ice crystal growth in extracellular fluids, allowing fish to

148 A detailed study of carbamazepine crystal growth in four different bis(urea) gelators, inc

149 now recognized as an important mechanism of crystal growth in many materials, yet the alignment proc

150 Recent studies have found that crystal growth in organic glasses can be orders of magni

151 The kinetics of crystal growth in porous media controls a variety of nat

152 y be of value in probing parallel systems of crystal growth in solid inclusion compounds, crystal gro

153 e of research on the chemistry of doping and crystal growth in solution.

154 ril mineralization by selectively inhibiting crystal growth in the solution outside of the fibril.

155 own to form as inclusions during peritectoid crystal growth in the ternary CrZnSe solid-state compoun

156 Confinement of crystal growth in this manner provides a snapshot of the

157 that the presence of CCH can inhibit the ice crystals growth in NAM to reduce protein freeze-denatura

158 ypothesize that structural ordering enhances crystal growth, in contrast to assumptions from common g

159 perpetuating steps to enable one-dimensional crystal growth, in contrast to mechanisms that require m

160 ent explanations differ for surface-enhanced crystal growth, including released tension and enhanced

161 of synthetic compounds for the regulation of crystal growth, including the freezing of water and grow

162 film is structurally confined by directional crystal growth, inducing intense anisotropy in charge tr

163 nd the physical chemistry of the synergistic crystal growth inhibition by two inhibitors.

164 n" antifreeze activity as exemplified by ice crystal growth inhibition concomitant with melting tempe

165 with classical mechanisms of layer-by-layer crystal growth inhibition.

166 ations of the crystal habit and polymorph by crystal growth inhibitors may not affect crystal aggrega

167 ation, unique among antimalarials and common crystal growth inhibitors, that opens new avenues for ev

168 on of L-cystine stones by rational design of crystal growth inhibitors.

169 ing temperature, the ordered layer initiates crystal growth into the bulk, leading to an oriented, ho

170 range of applications, including catalysis, crystal growth, ion sensing, drug delivery, data storage

171 completes alignment and enables coalescence.Crystal growth is a fundamental process, important in a

172 Ice crystal growth is a major problem in cell/tissue cryopre

173 The Sb-assisted crystal growth is associated with the formation of a Sb-

174 gantic molecules formed by self-assembly and crystal growth is challenging as it combines two conting

175 A molecular-scale understanding of crystal growth is critical to the development of importa

176 , a novel collision-based approach to seeded crystal growth is described in which seed crystals are d

177 irst example of biomacromolecular core-shell crystal growth is described, by showing that these cryst

178 During the entire experiment, no crystal growth is detected, and rigid grain rotation is

179 When the crystal growth is dominated by the monomer attachment, t

180 Understanding and predicting crystal growth is fundamental to the control of function

181 d of lead chloride or iodide, the perovskite crystal growth is much faster, which allows us to obtain

182 ber of crystals increases with time, but the crystal growth is slowed down by the surrounding dense i

183 Our work paves the way to tune the crystal growth kinetics by simple chemistry.

184 in determining the temperature dependence of crystal growth kinetics.

185 ion processes, in particular, are plagued by crystal growth (known as scaling), which restricts the f

186 ice of the lead salt will aid in controlling crystal growth, leading to superior films and better per

187 ons such as dynamic photocontrol of a single-crystal growth, light-gated permeability in membrane-lik

188 low for control over individual Wulff-shaped crystal growth, location, and orientation.

189 e that electrostatic interactions in aqueous crystal growth may be systematically manipulated to synt

190 The process of surface crystal growth, meanwhile, is unperturbed by eliminating

191 nciled by invoking a three-step nonclassical crystal growth mechanism comprising (i) docking of clust

192 hollow crystals is attributed to a reversed crystal growth mechanism heretofore described only in th

193 predominantly in the solid state, an unusual crystal growth mechanism.

194 show that, at high temperature, the observed crystal growth mechanisms and crystallization speed are

195 ered, providing new insight into constricted crystal growth mechanisms underlying confined synthesis.

196 by a hydrophobic interface confined lateral crystal growth method.

197 With the optimization of single-crystal growth methods, large-size and high-quality boro

198 ion of this effect on a physically-motivated crystal growth model enables the quantitative prediction

199 Classical crystal growth models posit that crystallization outcome

200 matin inhibitors is not reflected in current crystal growth models.

201 Synergism between two crystal growth modifiers is expected, but the antagonist

202 crystal growth in solid inclusion compounds, crystal growth modifiers, emulsion stabilization, and re

203 terfacial phenomena such as charge transfer, crystal growth, nanoscale self-assembly and colloidal st

204 rge amount of new information, new rules for crystal growth need to be developed and tested.

205 With its facile crystal growth, novel structure type, and striking elect

206 nables simultaneous monitoring of individual crystal growth, nucleation rate, and macroscopic crystal

207 Lattice rotation in this new mode of crystal growth occurs upon crystallization through a wel

208 e demonstrate our approach by predicting the crystal growth of a diverse set of crystal types, includ

209 port where AF(G)Ps have been used to control crystal growth of carbohydrates and on AFGPs controlling

210 The synthesis and single crystal growth of clathrate-II Na(24)Si(136) is performe

211 t provides an overview of the method of flux crystal growth of complex oxides and can function as a "

212 oxidative decomposition of PB microcubes and crystal growth of iron oxide shells, we have demonstrate

213 istence of In(3+) and Cr(3+) induces a rapid crystal growth of large single crystals of heterometalli

214 nvestigation of some of the axioms governing crystal growth of nanoporous framework solids in general

215 We exploited this feature to separate the crystal growth of otherwise concomitant polymorphs from

216 e crucial in the manufacturing of chemicals, crystal growth of semiconductors, waste recovery of biol

217 a novel preparatory method for synthesis and crystal growth of solid state materials.

218 Here, we report new insights on the crystal growth of the perovskite materials, especially c

219 Single crystal growth of the rare earth hexaboride, SmB6, has b

220 oved understanding and better control of the crystal growth of these perovskites could further boost

221 e critical in the surface nucleation for the crystal growth of this material.

222 ould add new fundamentals to the insights of crystal growths of nanocrystals and would also help in o

223 Directed crystal growth on designer substrates has the potential

224 tor defects and thus can be harnessed during crystal growth or annealing to suppress defect populatio

225 because of limitations on the conditions of crystal growth or protein vitrification.

226 iate occurs with a switch from bidirectional crystal growth parallel to the calcite c axis to growth

227 rol the reaction rate and, consequently, the crystal growth pathway and morphology of final products.

228 ngle-unit-cell level reveals novel nanoscale crystal-growth phenomena associated with the lateral siz

229 Evidence of such a novel crystal growth phenomenon can be also found in many othe

230 nciple the approach could be adapted to many crystal growth problems.

231 he starting materials is the first step of a crystal growth procedure.

232 F and the micelles, making self-assembly and crystal growth proceed under the direction of the cooper

233 ty were systematically varied to control the crystal growth process and determine the optimal conditi

234 Biomineralization in sea urchin embryos is a crystal growth process that results in oriented single-c

235 Here we present a rapid crystal growth process to obtain MAPbX3 single crystals,

236 n be easily captured and released during the crystal growth process, resulting in the formation and o

237 roturbulent transport, must be active in the crystal growth process.

238 The current understanding of crystal growth processes in the presence of macromolecul

239 ements and observations of phase changes and crystal growth processes relevant to atmospheric science

240 n marine barites than expected for classical crystal growth processes remains unknown.

241 d on these observations, we suggest possible crystal growth processes underpinning synthetic control

242 itu scanning probe microscopy to monitor the crystal growth processes with all-atom molecular dynamic

243 ors grown by sophisticated, high-temperature crystal growth processes.

244 es than those that are possible by classical crystal growth processes.

245 e is widely applicable and is not limited to crystal growth processes.

246 Crystal growth propagates a sequence of bits while mecha

247 This rapid crystal growth rate (approximately 1 m/s) suggests that,

248 imated in the model included dissolution and crystal growth rate constants, as well as the dissolutio

249 ee of fivefold symmetry has little effect on crystal growth rate, suggesting that growth may be only

250 efect concentration could be correlated with crystal growth rate.

251 ng the net charge on a protein increases the crystal growth rate.

252 Ca isotopic compositions that suggest rapid crystal growth rates (>1 cm/y to 15 cm/y).

253 of large, uniformly sized crystals even when crystal growth rates change over time.

254 hat we can predict the activation energy for crystal growth rates, including activation energies sign

255 ite in southern California, USA, to quantify crystal growth rates.

256 apes and sizes as affected by nucleation and crystal growth rates.

257 generation of actinide chalcogenides in flux crystal growth reactions.

258 otope effects depend mainly on the rates for crystal growth relative to liquid phase Ca diffusivity (

259 Crystal growth required the assistance of an anti-A3 nan

260 ducing sugars formed due to inversion hinder crystal growth, resulting in relatively small crystals.

261 that PGEmix-8 is a nucleation enhancing and crystal growth retarding additive in palm oil crystalliz

262 The discovery of reversed crystal growth routes in zeolite analcime and zeolite A

263 In this paper we report the crystal growth, structure determination, and magnetic pr

264 Herein, approaches for crystal growth/synthesis of these unique nanostructures

265 New hydrothermal crystal growth technique enabled isolation of environmen

266 hemical vapor transport (CVT), an old single-crystal growth technique, has been extended from growing

267 The process utilizes templated liquid-phase crystal growth that results in user-tunable, patterned m

268 tructure is one of the primary objectives in crystal growth, the present lack of predictive understan

269 Subject to inevitable stresses during crystal growth, the relatively soft strut lengths and di

270 example, during phase separation) or faceted crystal growth, their surfaces tend to have minimum-area

271 inetics and those predicted from fundamental crystal growth theories confirms that the growth of thes

272 Kinetic crystal growth theory is used to show that crystals acce

273 indings not only expand the current scope of crystal growth theory, but may also lead to a broader sc

274 imental findings in the context of classical crystal growth theory, the former is suggested to create

275 ge is sufficient to inhibit further hemozoin crystal growth, thereby sabotaging heme detoxification.

276 During the crystal growth, these dopant-based surface complexions b

277 t for antifreeze proteins (AFPs) to stop ice crystal growth, they must irreversibly bind to the ice s

278 idation is only to sulfenic acid despite the crystal growth time period of 2 weeks.

279 ation (and eruption) events, as reflected in crystal growth times, can be as short as ~10(-3) y.

280 extends the possibility of mesoporous single-crystal growth to a range of functional ceramics and sem

281 that it is possible to harness non-classical crystal growth to fabricate organic molecular crystals w

282 om phase transitions, chemical reactions and crystal growth to grain boundary dynamics.

283 itive branching during one-step hydrothermal crystal growth to synthesize a new hierarchical zeolite

284 highly direction-specific interactions drive crystal growth via oriented attachment.

285 extraneous nucleation is avoided relative to crystal growth via spatially localized laser heating and

286 evidence of metal-organic frameworks (MOFs) crystal growth via the assembly of sublayer surfaces and

287 The intra-ER crystal growth was accompanied by cell enlargement and m

288 tural process of enamel formation, templated crystal growth was achieved by interaction of amelogenin

289 Crystal growth was also greatly reduced when using 0.7%

290 It was found that CaCO(3) crystal growth was inhibited mostly by soluble starch by

291 ystallinity, preferred orientation, and cage crystal growth was obtained by experimental and computat

292 centrations, the rate-limiting factor of the crystal growth was the adsorption of the precursor ions,

293 tion pressure as a result of rapid, oriented crystal growth, which leads to pore deformation and the

294 n appear to be determined by the kinetics of crystal growth with a statistical bias, but the diversit

295 wed increased inhibitory effects on palm oil crystal growth with increasing concentration of PGEmix-8

296 However, methods to control zeolite crystal growth with nanometer precision are still in the

297 odification can significantly facilitate the crystal growth with respect to the corresponding native

298 rovides a snapshot of the earliest stages of crystal growth, with insights into nucleation, size-depe

299 Confined crystal growth within these templates leads to size-tuna

300 sited, DPT's pendant phenyl groups frustrate crystal growth, yielding amorphous films.