ライフサイエンスコーパス: nanocrystal

1 materials (such as exfoliated nanosheets or nanocrystals).

2 ts reveal the high quality of the core/shell nanocrystal.

3 on to atoms for their incorporation into the nanocrystal.

4 aphene oxide (GO) sheet with alumina (Al2O3) nanocrystals.

5 oach to realize the collective properties of nanocrystals.

6 multifunctional lanthanide-doped core/shell nanocrystals.

7 e size, shape, composition, and structure of nanocrystals.

8 ear-infrared fluorescence for copper sulfide nanocrystals.

9 ly dissociate to methyl radicals and n-doped nanocrystals.

10 ting and sustaining the growth of octahedral nanocrystals.

11 the intracellular dissolution process of the nanocrystals.

12 aInS2 nanocrystals into Yb(3+)-doped PbIn2S4 nanocrystals.

13 rful tool for the synthesis of heterogeneous nanocrystals.

14 the process of ET from photoexcited CdSe/ZnS nanocrystals.

15 hydriding phase transformation of palladium nanocrystals.

16 the chemical and mechanical stability of MOF nanocrystals.

17 pproach for the synthesis of colloidal metal nanocrystals.

18 nge reaction using films of sintered CsPbBr3 nanocrystals.

19 ductor quantum dots, especially on Si and Ge nanocrystals.

20 of the art in nonthermal plasma synthesis of nanocrystals.

21 ol of electronic impurities in semiconductor nanocrystals.

22 nsisting of thin films of ligand-capped ZrO2 nanocrystals.

23 ss to minimize the lattice strain within the nanocrystals.

24 covering the large facets of disc-shaped TPP nanocrystals.

25 ed by visible-light photoexcitation of these nanocrystals.

26 involved in the synthesis of colloidal metal nanocrystals.

27 hells around different almost spherical core nanocrystals.

28 erparamagnetic Zn0.2Fe2.8O4 and plasmonic Au nanocrystals.

29 reactivity allows the extent of nucleation ([nanocrystal] = 4.6-56.7 muM) and the size following comp

30 i-n-octylphosphine oxide solution results in nanocrystal aggregation.

31 rsion, semiconducting, and thermoelectric 1D nanocrystals, among others, as well as combinations ther

32 Molecular complexes between CdSe nanocrystals and Clostridium acetobutylicum [FeFe] hydro

33 re of the excitonic process in Ag-doped CdSe nanocrystals and demonstrate that, in contrast to expect

34 to characterize structural changes in single nanocrystals and extract lattice level information throu

35 ail with nanometer spatial resolution within nanocrystals and grains in reactive environments.

36 our nanocellulose samples, such as cellulose nanocrystals and nanofibers with cellulose I and II stru

37 By tuning the ratio between the perovskite nanocrystals and polymers, pure white light is achieved

38 ategy for the selective growth of individual nanocrystals and provide crucial insights into understan

39 (3+) is both incorporated within the PbIn2S4 nanocrystals and sensitized by visible-light photoexcita

40 diverse systems, including atoms, molecules, nanocrystals and single bioparticles, under extreme cond

41 ns demonstrated in CdSe-CdS core-thick-shell nanocrystals and their modifications.

42 nching effects in colloidal lanthanide-doped nanocrystals, and that inert epitaxial shell growth can

43 rapid identification of phase, even in small nanocrystals ( approximately 2 nm), and may help predict

44 re found within macrophages as aggregates of nanocrystals ( approximately 2.5 nm diameter) in the fer

45 ive solution-processable materials.Colloidal nanocrystals are a promising material for easy-to-fabric

46 the exchanged, bound-ion-pair X-type ligated nanocrystals are characterized by a range of methods.

47 ed inorganic nanocrystals, even though these nanocrystals are connected only by soft organic ligands

48 for achieving size and shape control of ZIF nanocrystals are considered, which are important for opt

49 elated materials.The exposed facets of oxide nanocrystals are key to their properties.

50 ety of biological building blocks, cellulose nanocrystals are one of the most promising biosourced ma

51 ntal conditions for generating intermetallic nanocrystals are presented, followed by examples to high

52 idal liquid crystal suspensions of cellulose nanocrystals are reviewed and recent advances in structu

53 luminescence of copper-containing colloidal nanocrystals are reviewed in the context of the well-est

54 ction yields ambiguous phase signatures when nanocrystals are small or polytypic.

55 Our results show that colloidal nanocrystals are suitable for compact and efficient opto

56 Once the nanocrystals are supported onto oxide materials, thermal

57 tional semiconductors, molecular solids, and nanocrystal arrays by combining their most attractive fe

58 twork gel method is demonstrated, taking ZnO nanocrystals as an example.

59 to highlight the viable use of intermetallic nanocrystals as electrocatalysts or catalysts for variou

60 uthors synthesize rare earth down-converting nanocrystals as promising fluorescent probes for in vivo

61 graphene variants, luminescent carbon dots, nanocrystals as quantum dots, and photon up-converting p

62 Through the use of well-defined nanocrystals as seeds, including those with different ty

63 e polymer materials with the blue perovskite nanocrystals as the active layer.

64 easurement of this attraction between rutile nanocrystals, as a function of their mutual orientation

65 The orientations of the nanocrystals, as well as the crystallographic axes of th

66 y is used to organize polystyrene-grafted Au nanocrystals at a fluid interface to form ordered solids

67 al strategy for the synthesis of metal oxide nanocrystals, balancing the crystallinity and specific s

68 ical means to finely and reversibly tune the nanocrystal band gap over a wide range of energies (1.8-

69 arameters not only control the properties of nanocrystals but also determine their relevance to, and

70 d crystal structure for copper sulfide-based nanocrystals, but also provide a pathway to a previously

71 strate postsynthetic modification of CsPbBr3 nanocrystals by a thiocyanate salt treatment.

72 involve the displacement of Mn(2+) from CdSe nanocrystals by Cd(2+) or In(3+).

73 -doped visible-light-absorbing semiconductor nanocrystals by demonstrating selective cation exchange

74 0(22) cm(-3) to intrinsic) in copper sulfide nanocrystals by electrochemical methods.

75 odium rare-earth tetrafluoride (beta-NaLnF4) nanocrystals by exploiting the kinetics of the shell gro

76 lling the evolution of twin defects in metal nanocrystals by simply following thermodynamic principle

77 view demonstrates how the diversity of metal nanocrystals can be expanded with endless opportunities

78 cets for a range of applications.Metal oxide nanocrystals can be grown with different facets exposed

79 ge, imperfect crystals into microcrystals or nanocrystals can provide a simple path for high-resoluti

80 Nanocrystal cation exchange, which proceeds rapidly unde

81 Colloidal dispersions of amine bound nanocrystals (CdSe-NH2R') are indefinitely stable at ami

82 In this limited class of nanocrystals, CdSe/CdS core/arm tetrapods exhibit the un

83 ge, 2.2 nm diameter, thiolate protected gold nanocrystal characterized by single crystal X-ray crysta

84 Au/CdSe nanocrystal clusters (NCs) are successfully fabricated t

85 oated with thin films of bacterial cellulose nanocrystals (CN) to provide a more sensitive and adapte

86 Pure cellulose nanocrystal (CNC) aerogels with controlled 3D structures

87 Herein, we show that rod-like cellulose nanocrystal (CNC)-based NP-surfactants, termed CNC-surfa

88 ith cellulose I and II structures (cellulose nanocrystals (CNC) I, CNC II, cellulose nanofibers (CNF)

89 Polydopamine (PDA)-coated SnO2 nanocrystals, composed of hundreds of PDA-coated "corn-l

90 a unique series of 42 different quantum dot nanocrystals, composed of two chemical domains (CdS:CdSe

91 this all-perovskite, all-inorganic imbedded nanocrystal composite relative to pure CsPbBr3 indicates

92 rmation contain Fe-silicate and Fe-carbonate nanocrystal concentrations in cell interiors.

93 In this study, we utilized the hybrid nanocrystal concept and studied the kinetic process of d

94 The shapes of the nanocrystals continue to evolve in terms of the intimate

95 ligand coverage on nanocrystal surfaces and nanocrystal core size are responsible for the crystalliz

96 al with cerium doping (Er/Ce co-doped NaYbF4 nanocrystal core with an inert NaYF4 shell).

97 s, drug-loaded block-copolymer micelles, and nanocrystal-core reconstituted high-density lipoproteins

98 tween 0 and 20 conduction-band electrons per nanocrystal, corresponding to carrier densities between

99 concentration nc for films of heavily doped nanocrystals devoid of ligands at their surface and in d

100 irect polymerization of ethylene in water to nanocrystal dispersions of disentangled, ultrahigh-molec

101 The results indicate that nanocrystal dispersions solely stabilized by neutral don

102 The extent to which the drug nanocrystal dissolved was estimated according to the flu

103 m and the "rigid-soft" system crosslinked by nanocrystal domains like silk protein dopes, were secret

104 tropic and rod-like shells around beta-NaYF4 nanocrystals doped with Yb(3+)/Er(3+) and Yb(3+)/Tm(3+).

105 sites (that is, tin-doped indium oxide (ITO) nanocrystals embedded in NbOx glass) via acid-catalysed

106 ore-shell nanoplatelets, which are efficient nanocrystal emitters with the electronic structure of qu

107 d nanomaterials, to improve the precision of nanocrystal engineering and improve our understanding of

108 h as 100 mol% in NaY(Er)F4/NaLuF4 core/shell nanocrystals enhance the emission intensity of both upco

109 self-assembly of ligand-stabilized inorganic nanocrystals, even though these nanocrystals are connect

110 esonance (NMR) strategy to distinguish oxide nanocrystals exposing different facets.

111 The availability of some nanocrystal facets can be tuned by selectively covering

112 ns of the chemistry and physics of different nanocrystal facets.

113 tegies exist for synthesizing copper sulfide nanocrystals, few methods result in nanocrystals with bo

114 The resulting near-complete nanocrystal film coverage, coupled with the natural conf

115 When TPE is entrapped in a nanocrystal, fluorescence is emitted when the nanocrysta

116 cursor adsorbs onto the surface of a growing nanocrystal, followed by chemical reduction to atoms for

117 ies attached to the (111) and (110) of small nanocrystals form interparticle bridges, aligning the QD

118 mately 2 nm), and may help predict polytypic nanocrystals from differential phase contributions.

119 cal, electronic and structural properties of nanocrystals fundamentally derive from crystal phase.

120 Ligand exchange drives Au nanocrystal fusion and forms a porous network, imparting

121 lectively on the overall surface of the host nanocrystals, generating Cu2Se@PbSe core@shell nanoheter

122 zation and self-assembly of amphiphilic gold nanocrystals grafted covalently with polymer brushes.

123 In situ microscopy of colloidal nanocrystal growth offers a unique opportunity to acquir

124 F-279 nanocrystal has a core-shell structure containing a trun

125 e that the crystal structure of the starting nanocrystals has a strong influence on the exchange path

126 ed (001) and (101) facets of anatase titania nanocrystals have distinct (17)O NMR shifts, which are s

127 Colloidal semiconductor nanocrystals have emerged as promising active materials

128 lopments in the synthesis of polymer-grafted nanocrystals have greatly expanded the library of access

129 Solution-grown films of CsPbBr3 nanocrystals imbedded in Cs4 PbBr6 are incorporated as t

130 scale assemble into various architectures of nanocrystals in a binary solution system.

131 t is possible to quantify the dissolution of nanocrystals in a biological environment.

132 in films contain a homogeneous dispersion of nanocrystals in an amorphous matrix.

133 egrees C to form carboxylate-terminated PbSe nanocrystals in quantitative yields.

134 we tracked the self-assembly of lead sulfide nanocrystals in real time.

135 ation results showed the presence of the MOF nanocrystals in the active layer of the membranes.

136 weak bonding between individual molecules or nanocrystals in the active materials, which prevents sus

137 ct photo-oxidation of lithium iron phosphate nanocrystals in the presence of a dye as a hybrid photo-

138 erimental and computational results for gold nanocrystals in the shapes of spheres, cubes, octahedra

139 mic films of niobium oxide glass (NbOx) and 'nanocrystal-in-glass' composites (that is, tin-doped ind

140 uced emission (AIE), hybrid paclitaxel (PTX) nanocrystals integrated with tetraphenylethene (TPE) ena

141 are likely to be applicable to semiconductor nanocrystals interfaced with molecular chromophores, ena

142 we fully exploit this property by doping PbS nanocrystals into a newly formulated photorefractive com

143 ation of organic-inorganic hybrid perovskite nanocrystals into highly luminescent nanoplates with a s

144 n process that can transform solid palladium nanocrystals into hollow palladium nanocrystals through

145 urface energy, triggering the comminution of nanocrystals into nanoslices along such crystal plane.

146 ion in an effort to control the evolution of nanocrystals into predictable shapes.

147 Crystallization of colloidal nanocrystals into superlattices represents a practical b

148 nge to convert precursor Yb(3+)-doped NaInS2 nanocrystals into Yb(3+)-doped PbIn2S4 nanocrystals.

149 ate anisotropic elemental distributions in a nanocrystal is a great challenge in reaching higher tier

150 anocrystal, fluorescence is emitted when the nanocrystal is optically excited.

151 The self-assembly of cellulose nanocrystals is a powerful method for the fabrication of

152 lanthanide ions into colloidal semiconductor nanocrystals is a promising strategy for combining their

153 Understanding of the in vivo fate of drug nanocrystals is however very limited.

154 f framework reorganization in individual MOF nanocrystals is largely unknown.

155 ol over the doping density in copper sulfide nanocrystals is of great importance and determines its u

156 to success in producing monometallic hollow nanocrystals is the effective extraction of phosphorus t

157 universal role in the synthesis of colloidal nanocrystals, it is still poorly understood and controll

158 liquid medium due to the dissolution of the nanocrystal, its fluorescence is quenched.

159 vert tags by the transfer of an upconversion nanocrystal-laden LSMA.

160 powers, and realizing an efficient low-power nanocrystal laser has remained a difficult challenge.

161 In particular, the development of nanocrystal lasers is currently experiencing rapid progr

162 Nanocrystal ligand chemistry was studied through a combi

163 and studying reaction mechanisms of biphasic nanocrystal ligand-exchange reactions.

164 the important opportunities that micro- and nanocrystals may offer in these and similar time-resolve

165 ween plasmonic and fluorescent semiconductor nanocrystals might lead to their successful implementati

166 Nanocrystal modified EmuPAD showed wide linear range 0.0

167 e challenges, we developed an albumin-coated nanocrystal (NC) formulation of paclitaxel (PTX) with 90

168 difficulty in comprehensively characterizing nanocrystal (NC) surfaces, clear guidance for ligand des

169 xamine energy transfer between semiconductor nanocrystals (NCs) and pi-conjugated molecules, focusing

170 past couple of decades, colloidal inorganic nanocrystals (NCs) and, more specifically, semiconductor

171 use well-defined ligand-protected perovskite nanocrystals (NCs) as model systems to elucidate the rol

172 Nanocrystals (NCs) can self-assemble into ordered superl

173 molecules, but assembly of chiral inorganic nanocrystals (NCs) has been lacking.

174 Inorganic metal halide perovskite nanocrystals (NCs) have been employed universally in lig

175 loidal CsPbX3 (X = Br, Cl, and I) perovskite nanocrystals (NCs) have emerged as promising phosphors a

176 scence in copper (Cu(+))-doped semiconductor nanocrystals (NCs) involves recombination of delocalized

177 Doping of nanocrystals (NCs) is a key, yet underexplored, approach

178 redox potentials of colloidal semiconductor nanocrystals (NCs) is described.

179 f the size-dependent Stokes shift in CsPbBr3 nanocrystals (NCs) is explained for the first time.

180 Ternary metal chalcogenide nanocrystals (NCs) offer exciting opportunities as novel

181 Cesium lead halide (CsPbX3) perovskite nanocrystals (NCs) possess the unique capability of post

182 5 nm inverse spinel-type oxide Ga2FeO4 (GFO) nanocrystals (NCs) with control over the gallium and iro

183 nanoparticle assemblies for Ag/Au, CdSe/PbS nanocrystals (NCs).

184 ns (DBMPs) in 2.8-nm diameter CdSe colloidal nanocrystals (NCs).

185 tron microscopy, we show how gold and silver nanocrystals nucleate from supersaturated aqueous soluti

186 Here, we show that nanocrystals of digenite Cu2-x S transform to zincblende

187 h for incorporating manganese (Mn) ions into nanocrystals of lead-halide perovskites (CsPbX3, where X

188 rd diffusion of phosphorus from the compound nanocrystals of palladium phosphide and consequently the

189 Arrays of individual single nanocrystals of Sb2Te3 have been formed using selective

190 g a poorly water-soluble drug substance into nanocrystals offers many advantages.

191 xylate surface ligands from cadmium selenide nanocrystals, oleic acid impurities are first removed us

192 tically to govern the plastic deformation of nanocrystals over a material-dependent sample diameter r

193 the role of polymer structural conformation, nanocrystal packing, and superlattice dimensions.

194 to obtain uniform palladium-based bimetallic nanocrystals (PdM, M = V, Mn, Fe, Co, Ni, Zn, Sn, and po

195 Through the use of nanocrystal pinning, highly luminescent methylammonium l

196 ynthesized (PLQY approximately 90%) and aged nanocrystals (PLQY approximately 70%) to within measurem

197 sing methyl-ammonium lead bromide perovskite nanocrystals (PNC) to illustrate the working principle,

198 CH3 NH3 PbBr3 perovskite nanocrystals (PNCs) of different sizes (ca. 2.5-100 nm)

199 ntials of free-standing colloidal n-type ZnO nanocrystals possessing between 0 and 20 conduction-band

200 is tunable through synthesizing Fe-doped ZIF nanocrystal precursors in a wide range from 20 to 1000 n

201 g density and fluorescence of copper sulfide nanocrystals presented in this work and the ability to s

202 times to gradually inflate the hollow metal nanocrystals, producing nanoshells of increased diameter

203 Additionally, the MOF nanocrystals provided biocidal activity that lasted for

204 ecies on different facets of anatase titania nanocrystals, providing compelling evidence for the valu

205 diative energy transfer (NRET) from adjacent nanocrystal quantum dot (NQD) films.

206 Here we show that colloidal nanocrystal quantum dots (QDs) can serve as efficient an

207 ics and chemistry of colloidal semiconductor nanocrystal quantum dots (QDs) have been central to the

208 The use of semiconductor nanocrystal quantum dots (QDs) in optoelectronic devices

209 veral important nanoscale systems, including nanocrystal quantum dots, carbon nanotubes and graphene.

210 engineering and improve our understanding of nanocrystal reactions.

211 tion inversion and optical gain in colloidal nanocrystals realized with direct-current electrical pum

212 egion contained smaller and less-oriented HA nanocrystals relative to ones that constitute the diaphy

213 Facet engineering of oxide nanocrystals represents a powerful method for generating

214 large-scale ordered superlattices induced by nanocrystal sedimentation and eventual solvent evaporati

215 Here we use a nanocrystal-seeded growth method triggered by a single r

216 length of superlattices strongly depends on nanocrystal shape.

217 whole potential range on {310} surface of Au nanocrystal shaped as truncated ditetragonal prism (TDP)

218 ytic bone metastasis led to a decrease in HA nanocrystal size and perfection in remnant metaphyseal t

219 s in simultaneous lattice expansion and fine nanocrystal size control due to the superlattice templat

220 small-molecule organic semiconductor micro-/nanocrystals (SMOSNs) at desired locations is a prerequi

221 Slow solvent evaporation or cooling of nanocrystal solutions (over hours or days) is the key el

222 f lead sulfide (PbS) colloidal semiconductor nanocrystals, specifically quantum dots (QDs), can be tu

223 range between the lower and upper limits for nanocrystal stability by surface diffusional creep and d

224 operties of these giant QDs, with only cubic nanocrystals sufficiently bright and stable to be observ

225 omputational study demonstrates the power of nanocrystal superlattice engineering and further narrows

226 rystals and report a quasicrystalline binary nanocrystal superlattice that exhibits correlations in t

227 essure-driven processing of heterostructural nanocrystal superlattices (HNC-SLs) self-assembled from

228 Nanocrystal superlattices are typically prepared by care

229 The mechanical properties of colloidal nanocrystal superlattices can be tailored through exposu

230 sized, face-centred-cubic, three-dimensional nanocrystal superlattices during colloidal synthesis at

231 rystals, various single- and multi-component nanocrystal superlattices have been produced, the lattic

232 e the mechanical behavior of polymer-grafted nanocrystal superlattices while exploring the role of po

233 ctronic, and catalytic properties of ordered nanocrystal superlattices, and the coming advances requi

234 provide an overview of structural defects in nanocrystal superlattices.

235 With Ag nanocrystals supported on amorphous SiO2 as a typical ex

236 needs to access a limited number of CsPbBr3 nanocrystal surface sites, likely representing under-coo

237 latter ligation has X(-) anions bound to the nanocrystal surfaces and closely associated LH(+) counte

238 eractions dictated by the ligand coverage on nanocrystal surfaces and nanocrystal core size are respo

239 lead to a broader scientific application of nanocrystal synthesis.

240 viding the reader with the basic concepts of nanocrystal synthesis.

241 (>400 mus) emission lifetimes in a colloidal nanocrystal system opens promising new opportunities for

242 o this notoriously environmentally sensitive nanocrystal system.

243 The rational assembly of various nanocrystal systems into novel materials is thus facilit

244 transition to intrinsic low-chalcocite Cu2S nanocrystals that display air stable fluorescence, cente

245 rts the fabrication of protein-capped ZnS:Mn nanocrystals that exhibit the combined emission signatur

246 , we demonstrate a nanolaser using colloidal nanocrystals that exhibits a threshold input power of le

247 arious postsynthesis treatments of colloidal nanocrystals that have been developed to date, transform

248 rality in colloidal cinnabar mercury sulfide nanocrystals that originates from chirality interplay be

249 pants inside the size-confined semiconductor nanocrystals, the controlled dopant-host lattice couplin

250 On the other hand, in hexagonal Cu2Se nanocrystals, the entrance of Pb(2+) ions generated PbSe

251 scopy for visualizing the facet structure of nanocrystals, the volumes sampled by such techniques are

252 ead of direct sintering for the conventional nanocrystals, this study experimentally observes for the

253 palladium nanocrystals into hollow palladium nanocrystals through insertion and extraction of phospho

254 It is also the smallest gold nanocrystal to exhibit metallic behavior, with a surface

255 ive triplet-triplet energy transfer from the nanocrystals to 1-pyrenecarboxylic acid, producing a mol

256 c acid self-assembled on the surface of drug nanocrystals to form polymers with network-like structur

257 The exposure of cubic Cu2Se nanocrystals to Pb(2+) cations led to the initial format

258 here report the use of colloidal bimetallic nanocrystals to produce catalysts where the active and p

259 Exciton transfer from the blue nanocrystals to the orange polymers via Forster or Dexte

260 The growth of colloidal metal nanocrystals typically involves an autocatalytic process

261 re the mechanical behavior of individual MOF nanocrystals under compression within a transmission ele

262 breathing behavior of individual MIL-53(Cr) nanocrystals upon reversible water adsorption and temper

263 tures of cubic and hexagonal phases in II-VI nanocrystals using absorption spectroscopy and first-pri

264 he size, shape and composition of individual nanocrystals, various single- and multi-component nanocr

265 exchange, in both cases, was rock-salt PbSe nanocrystals, we show here that the crystal structure of

266 ing step not possible in, for example, II-VI nanocrystals, we use gentle chemical means to finely and

267 l of localized breast cancer, metaphyseal HA nanocrystals were also smaller and less perfect than in

268 Cellular uptake studies of hybrid nanocrystals were conducted with KB and HT-29 cell lines

269 MOF nanocrystals were immobilized in the active layer of the

270 Stoichiometric Cu2Se nanocrystals were synthesized in either cubic or hexagon

271 The results suggest that drug nanocrystals were taken up directly by the cells, and su

272 thout softening in face-centred-cubic silver nanocrystals, where crystal slip serves as a stimulus to

273 ttice under ambient conditions unlike larger nanocrystals, where Cu(+) ions and vacancies form an ord

274 earch endeavor centered around intermetallic nanocrystals, which are unique in terms of long-range at

275 Scaling the bulk form to nanocrystals, while successful in stabilizing the tetrag

276 the photophysical processes in heavily doped nanocrystals will give rise to enhanced properties not p

277 of a down-conversion luminescent rare-earth nanocrystal with cerium doping (Er/Ce co-doped NaYbF4 na

278 t is challenging to synthesize intermetallic nanocrystals with a tight control over their size and sh

279 ctly mixing synthesized bromide and chloride nanocrystals with a weight ratio of 2:1.

280 sulfide nanocrystals, few methods result in nanocrystals with both controlled morphological shapes a

281 t progress in the synthesis of intermetallic nanocrystals with controllable sizes and well-defined sh

282 -expanding toolbox used for generating metal nanocrystals with desired properties.

283 n generating high-quality conjugated-polymer nanocrystals with extended conjugation and exceptionally

284 Other typical metal oxide nanocrystals with good crystallinity and high specific s

285 ractical, efficient synthesis of metal oxide nanocrystals with good crystallinity and high specific s

286 nostructure consisting of, near the surface, nanocrystals with high density of nanotwins.

287 We validate that Ag nanocrystals with icosahedral, decahedral, and single-cr

288 Levitated diamond nanocrystals with nitrogen-vacancy (NV) centres in high

289 In contrast to alloy nanocrystals with no elemental ordering, it is challengi

290 l is largely composed of hydroxyapatite (HA) nanocrystals with physicochemical properties that vary s

291 Herein, we report that self-doping of SnO2-x nanocrystals with Sn(2+) red-shifts their absorption to

292 and thickness of up to several microns from nanocrystals with tens of nanometres in diameter.

293 pounds (e.g., nanoparticles, nanostructures, nanocrystals) with both top-down and bottom-up design pr

294 hesis of crystalline nanoparticles, that is, nanocrystals, with size- and shape-dependent physical pr

295 p for diamagnetic particles, such as diamond nanocrystals, with stable levitation from atmospheric pr

296 ses non-radiative Auger processes in charged nanocrystals, with successful non-blinking implementatio

297 his phase has only been prepared at 208 K as nanocrystals within ice.

298 confinement of metal-organic framework (MOF) nanocrystals within mesoporous materials, thereby render

299 , we observe continuous growth of individual nanocrystals within the lattices, which results in simul

300 using zeolites nanoflakes and graphene-oxide nanocrystals (Zeo-GO).