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1 l characterization and the properties of the nanocrystals.
2 ndgaps similar to Cu(3)VS(4) and Cu(3)VSe(4) nanocrystals.
3 ntrollable plastic reversibility in metallic nanocrystals.
4 further exploration into metal chalcohalide nanocrystals.
5 oles in guiding the shape evolution of metal nanocrystals.
6 reduction of metal ions and the formation of nanocrystals.
7 we substitute micrometer-size particles with nanocrystals.
8 nd kinetics involved in a synthesis of metal nanocrystals.
9 synthesis of random alloy and intermetallic nanocrystals.
10 lifetime with respect to the aspect ratio of nanocrystals.
11 rison to reported performance of Cu(3)VSe(4) nanocrystals.
12 sitionally and architecturally sophisticated nanocrystals.
13 surface, and impacts on the growth of metal nanocrystals.
14 X-ray pump/X-ray probe experiment on protein nanocrystals.
15 the structures of resulting Au-Ag core-shell nanocrystals.
16 eviously reported values among all colloidal nanocrystals.
17 of liposomal sample containing ciprofloxacin nanocrystals.
18 reported orthorhombic cube shaped CsPbBr(3) nanocrystals.
19 rature on the nucleation and growth of metal nanocrystals.
20 in determining the final shape of the metal nanocrystals.
21 echanism involved in the growth of inorganic nanocrystals.
22 ic ligands that densely cover the surface of nanocrystals.
23 characteristics as compared to single-domain nanocrystals.
24 f light amplification in II-VI semiconductor nanocrystals.
25 ent translational and orientational order of nanocrystals.
26 dict synthetic pathways for shape-controlled nanocrystals.
27 different planar defects formed in CsPbBr(3) nanocrystals.
28 n and subsequent attachment and alignment of nanocrystals.
29 and short-ranged orientational alignment of nanocrystals.
30 lid alternative to well established Cd-based nanocrystals.
31 for the improvement of synthesis pathways of nanocrystals.
32 uence-specific morphologies in various metal nanocrystals.
33 d also help in obtaining films of connecting nanocrystals.
34 s of surfactant-stabilized lead chalcohalide nanocrystals.
35 interaction between the ligands of adjacent nanocrystals.
36 twinning nucleation mechanism in HCP rhenium nanocrystals.
37 ow loadings (8-16 ppm) of Pt on shaped ceria nanocrystals.
38 d is further reduced to tetravalent UO(2) as nanocrystals (~1-2 nm) with random orientations inside n
39 te layout accommodates volume changes of the nanocrystals (~25%), which together leads to complete ch
40 cale character of nanocomposites is crucial: nanocrystals (5-50 nm) offer enhanced chemical reactivit
43 l in vitro data demonstrated that these gold nanocrystals act via a novel energy metabolism pathway i
47 extracted cellulose nanoparticles (cellulose nanocrystals and cellulose nanofibrils (CNF)) and natura
48 ions were not seen in chalcogenide and oxide nanocrystals and exclusively observed in perovskite nano
49 Li(x)NiO nanoclusters and polycrystalline Ni nanocrystals and its exceptional activities toward the h
53 arts from light absorption by the individual nanocrystals and subsequent excitation of out-of-equilib
54 cleation model suggests that the size of the nanocrystals and the host-guest interfaces are critical
55 coated with thin layers of calcium carbonate nanocrystals and the surface was modified to exhibit oil
56 ities for the structural characterization of nanocrystals and their assemblies using transmission ele
58 transferrin binding to cadmium chalcogenide nanocrystals and their subsequent delivery into cancer c
59 entals to the insights of crystal growths of nanocrystals and would also help in obtaining films of c
60 tment did not alter the thermal stability of nanocrystals, and BCNCs had high thermal stability like
61 late (BTC(3-) ) ligand reagents, to form MOF nanocrystals, and collect and characterise them on a TEM
62 lected to investigate the formation of rutin nanocrystals, and its incorporation in barley starch pyr
63 tives for studies on drug-induced nephritis, nanocrystals, and local lipid or carbohydrates alteratio
65 e.g., semiconductor quantum dots, perovskite nanocrystals, and rare earth doped phosphors), it is sur
66 distinguish intrinsic defects from extrinsic nanocrystals, and the findings pave the way for new desi
70 perty-structure probe reveals that CsPbBr(3) nanocrystals are contributing to the green emission of C
71 work demonstrates that bimetallic core-shell nanocrystals are excellent probes for the local physicoc
74 es and related properties of colloidal metal nanocrystals are key to the realization of their vast ap
75 s previously assumed: the c-axes of adjacent nanocrystals are most frequently mis-oriented by 1 degre
77 ning to orthorhombic CsPbBr(3), the obtained nanocrystals are stabilized by 12 facets ({200}, {020},
78 lecules into electronically coupled CsPbI(3) nanocrystal arrays is confirmed via infrared and photoel
79 y of the electronic properties of perovskite nanocrystal arrays is detailed using physically adsorbed
82 or the use of quantum confined semiconductor nanocrystals as photoinitiators, coining the term Quantu
88 As a proof-of-concept, we have synthesized a nanocrystal-based, dynamically tunable metasurface (an a
90 s as a feasible approach to enhance specific nanocrystal-biomolecule associations for improving cellu
92 hat primary ammonium ions led to six faceted nanocrystals, but tertiary ammonium ions obtained in thi
93 structures of individual colloidal platinum nanocrystals by developing atomic-resolution 3D liquid-c
94 ntal optical properties of halide perovskite nanocrystals by focusing on their linear optical propert
95 r-level understanding of the formation of Al nanocrystals by titanium(IV) isopropoxide-catalyzed deco
96 , which synthesize membrane-bounded magnetic nanocrystals called magnetosomes via a biologically cont
97 n(III), incorporated into ZnAl(2)O(4) spinel nanocrystals can achieve PLQYs of 50% for down-shifting
98 ow that the polar surface structure of oxide nanocrystals can be investigated by applying (17)O and (
99 demonstrated that small truncated-octahedral nanocrystals can self-assemble into a range of superstru
100 k, we utilize a combination of uniform Pd/Pt nanocrystal catalysts and theory to reveal the catalytic
102 ious research has focused on factors such as nanocrystal charging, the ratio of ligand length to core
103 leic acid (OA, 1, 2, and 3%, w/w), cellulose nanocrystal (CNC, 0.1, 0.3, and 0.5%, w/w), and 2% chito
104 ns of cellulose nanofibrils (CNF), cellulose nanocrystals (CNC), and kaolin-microfibrillated cellulos
105 ing interactions between rice bran cellulose nanocrystals (CNCs) and lauric arginate (LAE), which is
107 ed, namely, aqueous dispersions of cellulose nanocrystals (CNCs) that form superstructured, adherent
108 sustainable nanomaterials such as cellulose nanocrystals (CNCs) to be utilized in industrial applica
109 dispersible 'nanocage' composed of cellulose nanocrystals (CNCs), which are magnetically powered by i
111 Magnetosomes are intracellular magnetic nanocrystals composed of magnetite (Fe(3)O(4)) or greigi
112 We illustrate our approach with a multigrain nanocrystal comprising a Co(3)O(4) nanocube core that ca
114 materials to date have made exclusive use of nanocrystals containing toxic elements, precluding their
115 NCs crystallinity increased, and the size of nanocrystals decreased with increasing 10 degrees C hydr
116 preparation of clean-surfaced, faceted gold nanocrystals demonstrated robust remyelinating activity
118 solution-phase synthesis of ~4 nm defective nanocrystals (DNCs) composed of copper, aluminum, zinc,
119 ridges are initially inserted between a CdSe nanocrystal donor and anthracene acceptor, the rate of T
121 -dimensional strain evolution of single gold nanocrystals during a catalytic CO oxidation reaction un
122 rs, and light-emitting diodes) and colloidal nanocrystals (e.g., in liquid crystal displays and futur
123 st of in-situ formed high-quality perovskite nanocrystals embedded in the electron-transport molecula
124 of the heteroepitaxy of colloidal polyhedral nanocrystals enables ordered grain growth and can thereb
125 last five years, such that for heterogeneous nanocrystal ensembles, a single, atomically precise repr
126 nality, the nominally one-dimensional MoS(2) nanocrystals exhibit photoluminescence 50 meV higher in
127 multimetallic random alloy and intermetallic nanocrystals exhibit unique and intriguing physicochemic
129 onal heterostructures based on van der Waals nanocrystal films produced through the mechanical abrasi
130 to the general strategies for designing such nanocrystals, followed by four typical examples, includi
131 However, to amplify properties and prepare nanocrystals for specific applications, full atomic prec
134 r, mechanistic insight into the DNA-mediated nanocrystal formation remains elusive due to the lack of
136 we report the fabrication of precious metal nanocrystals from nuclei and the identification of the d
140 lecules in the solution direct the amplified nanocrystal handedness through a discontinuous transitio
141 stal phase of random alloy and intermetallic nanocrystals has been intensively explored in technologi
142 The self-assembly of two sizes of spherical nanocrystals has revealed a surprisingly diverse library
143 f-cell configuration in which 15-nm antimony nanocrystals have a consistently higher Coulombic effici
144 As such, random alloy and intermetallic nanocrystals have attracted extensive attention and inte
150 hastically ordered distribution of plasmonic nanocrystals in a fractal scaffold of high-index semicon
151 plications of random alloy and intermetallic nanocrystals in electrocatalysis, heterogeneous catalysi
152 s has been observed for CsPbBr(3) perovskite nanocrystals in film where nanocrystals were swollen to
153 swollen to get wider and fused with adjacent nanocrystals in self-assembly on film during solvent eva
154 c heterogeneity of ligand-protected platinum nanocrystals in solution, including structural degenerac
157 rm for the appendage/immobilization of small nanocrystals inside rendering high-performance catalysts
159 on further development of these bifunctional nanocrystals into a viable platform for investigating ot
161 omic structure presented on the surface of a nanocrystal is ultimately determined by its geometric sh
162 atomic structure determination of individual nanocrystals is a prerequisite for understanding and pre
164 Controlling which facets are exposed in nanocrystals is crucial to understanding different activ
165 mation from alpha to beta phases of tin (Sn) nanocrystals is investigated in nanocrystals with diamet
167 r long-range triplet energy transfer between nanocrystal light absorbers and molecular acceptors sugg
170 performed on perovskite cesium lead bromide nanocrystals, maps the lattice response to controlled ex
172 of intrinsically chiral lanthanide phosphate nanocrystals, measured via circularly polarized luminesc
173 , and optical images reveal that the bismuth nanocrystal melts during trapping, facilitating tip-to-t
174 of thermally activated photophysics at CdSe nanocrystal-molecule interfaces enables a new paradigm w
178 extent and rate of sintering as functions of nanocrystal (NC) size, temperature, and atmosphere.
179 prepare the near-infrared emission CsPbI(3) nanocrystal (NC)-polymer composite thin-film luminescent
180 Copper-based ternary (I-III-VI) chalcogenide nanocrystals (NCs) are compositionally-flexible semicond
182 s in the synthesis of lead halide perovskite nanocrystals (NCs) for use in solar cells, light emittin
186 colloidal synthesis of intrinsically chiral nanocrystals (NCs) of several chiral inorganic compounds
187 been devoted to understanding why colloidal nanocrystals (NCs) self-assemble into such a diverse arr
189 ic techniques that yield high quality BaTiO3 nanocrystals (NCs) with well-defined morphologies (e.g.,
194 uilibrium between complexes, monolayers, and nanocrystals of lead bromide, with substantial impact on
198 ials exposing nonpolar facets, polar-faceted nanocrystals often exhibit unexpected and interesting pr
199 triplet energy transfer across the inorganic nanocrystal/organic molecule interface remain poorly und
200 ulations to study the self-assembly of these nanocrystals over a broad range of ligand lengths and so
201 colloidal and photophysical stability to the nanocrystals over a broad range of solvent conditions an
202 ysical and structural characteristics of the nanocrystals over a period extending to 1.5 years under
203 nontoxic and stable bismuth-based perovskite nanocrystals (PeNCs) with applications for photocatalyti
204 nk is introduced, "photopatternable emissive nanocrystals" (PENs), which satisfies these requirements
205 Herein, we introduce the research area of nanocrystal photocatalysts, review their studies as Quan
206 entation of LSPR in all-inorganic perovskite nanocrystals (PNCs) is particularly important considerin
208 ovskite quantum dots (PQDs) or more broadly, nanocrystals possess advantageous features for solution-
211 We learn that having only one of the two nanocrystal precursors dissolving and diffusing toward t
213 properties, yet the question remains whether nanocrystal properties can be analyzed, understood, and
217 w the tunable preparation of cuprous sulfide nanocrystals ranging in internal structures from single-
218 hape-controlled synthesis of monodisperse Al nanocrystals remains an open challenge, limiting their u
220 inical studies, clean-surfaced, faceted gold nanocrystals represent a novel remyelinating therapeutic
224 ormation from CO(2) and that electrochemical nanocrystal scrambling is an avenue toward creating such
225 beta-Sn tetragonal structure, while smaller nanocrystals show stability with the alpha-Sn diamond cu
227 a detailed analysis of the role of effective nanocrystal size ratio, as well as softness expressed as
231 py, we show that sufficiently small antimony nanocrystals spontaneously form uniform voids on the rem
233 hanced and phase became stable, but ultimate nanocrystals still retained the hexahedron cube or plate
235 c nanocrystals and other types of structural nanocrystals such as core-shell and heterostructured nan
237 g strategy is reported to grow 2D Janus gold nanocrystal superlattice sheets with nanocube morphology
238 s guidance for the design and fabrication of nanocrystal superlattices with enhanced structural contr
243 orm, has been selected to develop injectable nanocrystal suspensions designed to be transferred to th
247 uted to the morphological evolution of Au-Ag nanocrystals synthesized with different DNA sequences.
248 sion can be extended to other multicomponent nanocrystal systems (metal alloy, mixed oxide, and chalc
249 t (CQD) microcrystals on organized cellulose nanocrystals templates at the liquid-air interface.
250 ultrasmall and monodisperse colloidal PtP(2) nanocrystals that achieve H(2)O(2) production at near ze
251 ironments(12) has resulted in platinum-based nanocrystals that enable very high ORR activities in aci
252 the composites with Pd (average size: 2 nm) nanocrystals, the material shows outstanding catalytic a
253 Unlike single-electron devices comprising nanocrystals, these cluster-based devices can be fabrica
255 stals and exclusively observed in perovskite nanocrystals, this would add new fundamentals to the ins
258 unable, highly luminescent halide perovskite nanocrystals to illustrate the role of carrier diffusion
259 direct photochemical electron delivery from nanocrystals to MoFe protein is able to support the mult
260 trate the capabilities of these bifunctional nanocrystals to monitor chemical reactions for the eluci
261 ctroscopy shows direct triplet transfer from nanocrystals to naphthalene; nonetheless, this "direct"
262 sheet T7-Pt{100} specificity drives cubic Pt nanocrystals to self-assemble into large-area, long-rang
263 atomistic spin model of elongated magnetite nanocrystals to specifically address the role of facetin
267 s with the ex situ oxidative etching of gold nanocrystals using FeCl(3) provides further insight into
269 le size and particle loading using colloidal nanocrystals, we reveal the opposite process as a novel
270 tals such as core-shell and heterostructured nanocrystals, well-defined multimetallic random alloy an
272 e transport layers, where a large density of nanocrystals were embedded, limiting the efficiency of s
273 bBr(3) perovskite nanocrystals in film where nanocrystals were swollen to get wider and fused with ad
274 achieved by chemical conversion reactions on nanocrystals, which are first self-assembled in nanocomp
275 eformable layer of ligands that envelops the nanocrystals, which contributes significantly to the ove
277 f providing structural support for plasmonic nanocrystals, which serve as nanoheaters, and reducing t
278 synthesis scheme to Pb(4)S(3)I(2) colloidal nanocrystals, whose structure matches the one that has b
279 le method for the synthesis of Ru octahedral nanocrystals with an fcc structure and an edge length of
280 an effective method for the synthesis of Ru nanocrystals with an fcc structure and well-defined {111
281 we were able to isolate methane hydrate (MH) nanocrystals with an sI structure encapsulated inside MO
282 ess in leveraging capping agents to generate nanocrystals with complex structures and/or enhance thei
283 The successful synthesis of noble-metal nanocrystals with controlled shapes offers many opportun
284 t progress in the development of noble-metal nanocrystals with controlled shapes, in addition to thei
285 More importantly, the final products are nanocrystals with controlled size and shape that can be
287 of tin (Sn) nanocrystals is investigated in nanocrystals with diameters ranging from 6.1 to 1.6 nm.
288 ll-controlled colloidal system consisting of nanocrystals with different aspect ratios, halide compos
289 used to control the evolution of seeds into nanocrystals with diverse but well-controlled shapes.
291 an be engineered to produce anisotropic gold nanocrystals with high chiroptical activity through the
293 roadly confined to only nanocubes, these new nanocrystals with intense emission would certainly provi
295 chemically functionalizing non-toxic silicon nanocrystals with triplet-accepting anthracene ligands.
297 el systems comprising lead halide perovskite nanocrystals with very low surface trap densities as the
298 mine as a halide precursor, different shaped nanocrystals without compromising the photoluminescence
299 nduced by electrical biasing of mixed-halide nanocrystals without the injection of charge carriers.
300 fraction and electron tomography of a single nanocrystal, X-ray powder diffraction, and density funct