ライフサイエンスコーパス: superlattice

1 he size and pitch of the quantum dots in the superlattice.

2 hs determined by the number of layers in the superlattice.

3 t the dynamic transformation from colloid to superlattice.

4 D planes within an Sb2Te3-GeTe van der Waals superlattice.

5 nced by the formation of a thorium phosphide superlattice.

6 s occupy defect sites that define a periodic superlattice.

7 particles self-assemble into a close-packed superlattice.

8 mposition-dependent, self-ordered octahedral superlattice.

9 netic impurities substituted into a graphene superlattice.

10 understandable toward achievement of desired superlattice.

11 decoration of graphene with an alkali adatom superlattice.

12 oroform self-assemble into only a single bcc superlattice.

13 icle size, defects, and inhomogeneity in the superlattice.

14 egree of magnetic moment compensation in the superlattice.

15 rsion medium, obtaining a high index faceted superlattice.

16 ces the magnetic ordering temperature in the superlattice.

17 and nanoparticles arranged into crystalline superlattices.

18 verview of structural defects in nanocrystal superlattices.

19 These Brownian objects readily order into superlattices.

20 rrangement of nanoparticles into crystalline superlattices.

21 otodetectors based on InAs/GaSb/AlSb type-II superlattices.

22 een energy and geometry in the emergent spin superlattices.

23 ovel structure for this kind of chalcogenide superlattices.

24 LuFeO3 matrix, that is, (LuFeO3)m/(LuFe2O4)1 superlattices.

25 e picture has not yet emerged for disordered superlattices.

26 which addresses resonant transmission in DLC superlattices.

27 he optical response in DNA-gold nanoparticle superlattices.

28 oys and producing TMD stacking structures or superlattices.

29 replace another to form doped self-assembled superlattices.

30 n of lamellar-type binary liquid crystalline superlattices.

31 f-organize into hexagonal close-packed (hcp) superlattices.

32 as a powerful tool for the fabrication of 3D superlattices.

33 light confinement in plasmonic metamaterial superlattices.

34 nds in the self-assembly of nanocrystal (NC) superlattices.

35 wo components comprising binary nanoparticle superlattices.

36 ferromagnetism in (LaMnO3+delta)N/(SrTiO3)N superlattices.

37 well thickness and SmTiO3 layer thickness in superlattices.

38 d carrier distribution in La delta-doped STO superlattices.

39 tween them causes the coexistence of the two superlattices.

40 ving forces responsible for the two distinct superlattices.

41 that BICs could be observed in semiconductor superlattices.

42 ic absorber molecules to form nanostructured superlattices.

43 o study the effective interactions in DNA-NP superlattices.

44 iferroic materials through modifying natural superlattices.

45 on causes simultaneous nucleation of the two superlattices.

46 d and can be fully harnessed for crystalline superlattices, a complete picture has not yet emerged fo

47 stem of multidomain ferroelectric-dielectric superlattices across a wide range of temperatures, in bo

48 imulations, we observe that in PbTiO3/SrTiO3 superlattices all of these effects can be found.

49 from the special geometry, the ZnO-graphene superlattice allows the generation of a tunable nanolase

50 ditions are investigated by growing the same superlattice alternatively on SrTiO3 substrates and 20 n

51 Here, we propose a waveguide superlattice and demonstrate advanced superlattice desig

52 These devices utilize a p-type Sb2Te3/Bi2Te3 superlattice and n-type delta-doped Bi2Te3-xSex, both of

53 ion ordering lifts inversion symmetry in the superlattice and produces a polar compound.

54 agnetization is freely adjustable within the superlattice and tends to minimize the binding energy.

55 nanocrystals occupy random positions in the superlattice and their density is readily and widely con

56 (-)/Ti, independent of GTO thickness in both superlattice and thin film geometries, in contrast to LA

57 ndamental understanding of heat transport in superlattices and the prospects of rationally designing

58 ntially annealed nitride metal/semiconductor superlattices, and show that this type of diffusion can

59 catalytic properties of ordered nanocrystal superlattices, and the coming advances required to make

60 This 1D superlattice approach is generalizable to a wide range o

61 powerful tools for controlling nanoparticle superlattices architecture, and establish the importance

62 e greatly expanded the library of accessible superlattice architectures, which allows superlattice me

63 and hardness of the ligand-free 3.7 nm ZrO2 superlattice are found to be similar to bulk yttria-stab

64 by a pump laser, the Stokes' photons of the superlattice are greatly amplified by the surface plasmo

65 he side discharges associated with honeycomb superlattice are verified by utilizing a high speed came

66 Quasi-quaternary nanocrystal superlattices are assembled by using exclusively core-sh

67 In addition to demonstrating that calcined superlattices are effective catalysts for alcohol oxidat

68 These superlattices are embedded in silica and calcined at 350

69 ng the formation of high-quality large-scale superlattices are explored in detail.

70 Moreover, three-dimensional binary superlattices are formed when DNA shells accommodate the

71 2D system, indicating that delta-doped oxide superlattices are good candidates for advanced thermoele

72 o show that the electronic properties of the superlattices are highly tunable and strongly affected b

73 triangle-shaped NaCl-type binary nanocrystal superlattices are produced driven by the entropic force,

74 to 7 nm, stable AlB2-type binary nanocrystal superlattices are produced, which remain independent of

75 Nanocrystal superlattices are typically prepared by carefully contro

76 dress these issues by realizing an epitaxial superlattice as an HMM.

77 h dependence of magnetic moments in BFO/LSMO superlattices as a function of the BFO layer thickness i

78 sion in disordered diamond-like carbon (DLC) superlattices as conventional models are not equipped to

79 es yields highly ordered binary nanoparticle superlattices as free-standing crystals, with up to a fe

80 cise orientational order, realization of dry superlattices as well as for the field of programmed sel

81 By moving beyond nanoparticle superlattices assembled only with DNA, a new degree of f

82 alytically active, porous structures through superlattice assembly and calcination.

83 treatment also transforms the bcc to an fcc superlattice at 175 degrees C.

84 xplain the ease of formation of different NC superlattices at slightly different synthesis conditions

85 We report on the observation of complex superlattices at the surface of the topological insulato

86 y discovered polar vortices in PbTiO3/SrTiO3 superlattices based on a combination of machine-learning

87 ange of magnetic properties in well-designed superlattice-based devices.

88 Microjunction InAs/InAs1-xSbx type-II superlattice-based long-wavelength infrared photodetecto

89 formation of 10 different binary nanocrystal superlattices (BNSLs) with both two- and three-dimension

90 e packing of particles in binary nanocrystal superlattices (BNSLs).

91 vents, we synthesized three types of PbSe NC superlattices--body-centered cubic (bcc), body-centered

92 l description of thermal phonon transport in superlattices by solving the Boltzmann transport equatio

93 We show that thermal transport in superlattices can be divided in two different heat trans

94 We show that the stripe-superlattices can be reproducibly and reversibly manipul

95 chanical properties of colloidal nanocrystal superlattices can be tailored through exposure to low-pr

96 l found in atomically thin delta-doped oxide superlattices can open a door to novel oxide-based high-

97 Such waveguide superlattices can potentially lead to significant reduct

98 Moreover, we show that symmetry-broken superlattices can sustain switchable nanolasing between

99 The superlattices can transition from exhibiting the propert

100 of nanocrystal synthesis, self-assembly, and superlattice characterization.

101 cture of the material and moves nanoparticle superlattices closer to naturally occurring biomaterials

102 his goal, we have synthesized a prototypical superlattice composed of a correlated metal LaNiO3 and a

103 charge transfer, we developed extremely thin superlattices composed of high Tc superconductor YBa2Cu3

104 High-quality superlattices comprising ferromagnetic La2/3Sr1/3MnO3 (L

105 By identifying four critical rules for the superlattice configuration we lay the foundation for a g

106 ormation of well-ordered body-centered cubic superlattices consisting of inorganic nanoparticles surr

107 ectrometry, which revealed that the calcined superlattice contained approximately 10% Au by weight.

108 Superlattices containing 3-20 vol % Au are found to have

109 nnihilation/reconstruction of the octahedral superlattice correlated with the delithiation/lithiation

110 ond, upon stabilization, all of these binary superlattices could be transformed into distinct "nanoal

111 As a result of the moire pattern superlattice created by this stacking, the electronic ba

112 the superlattice symmetry, but improves the superlattice crystallinity.

113 ow that two- and three-dimensional mesoscale superlattice crystals with precisely engineered optical

114 isplacive transformation in colloidal binary superlattice crystals, whereby a body-centered cubic to

115 study the switching process in chalcogenide superlattice (CSL) phase-change memory materials by desc

116 GeSbTe-based chalcogenide superlattice (CSLs) phase-change memories consist of GeS

117 e mechanism(s) driving the formation of such superlattices demands an understanding of their underlyi

118 l ordering occurs on a faster timescale than superlattice densification.

119 eguide superlattice and demonstrate advanced superlattice design concepts such as interlacing-recombi

120 ed on new InAs/InAs1-xSbx/AlAs1-xSbx type-II superlattice design.

121 for engineering novel transport behaviors in superlattice devices.

122 ctural ordering demonstrated in a variety of superlattice diffraction patterns.

123 tural conformation, nanocrystal packing, and superlattice dimensions.

124 editated growth, the concentration-dependent superlattice does not change lattice symmetry over the c

125 centred-cubic, three-dimensional nanocrystal superlattices during colloidal synthesis at high tempera

126 rmined to be critical parameters that govern superlattice elastic and plastic deformation.

127 ly inactive, highly crystalline nanoparticle superlattices embedded in silica into catalytically acti

128 xial attachment of quantum dots into ordered superlattices enables the synthesis of quasi-two-dimensi

129 study demonstrates the power of nanocrystal superlattice engineering and further narrows the gap bet

130 d by the identity of the atoms, nanoparticle superlattice engineering, where nanoparticle "atoms" are

131 deliberately designed transition metal oxide superlattice exhibits a resonant tunnelling behaviour wi

132 se changes in contrast with the GeTe-Sb2 Te3 superlattice film adopted in interfacial phase-change me

133 heterostructure films and devices, including superlattice films with vertical compositions designed l

134 re we report the formation of highly ordered superlattice films, with single crystalline domains of u

135 Here, we describe how plasmonic superlattices-finite-arrays of nanoparticles (patches) g

136 tion of the crystalline structure of the bcc superlattice following calcination and catalysis.

137 res lead to optimal quantum-transport in the superlattice for bidirectional operation compared to the

138 he effects of ligand-solvent interactions on superlattice formation from nonspherical nanoparticles.

139 g, quantum size effects, lattice mismatch or superlattice formation, the spectral variation is often

140 Exploration of Moire superlattices formed by the quintuple layers of topologi

141 onstrate the formation of binary and ternary superlattices from colloidal two-dimensional LaF3 nanodi

142 heterostructures, multiheterostructures, and superlattices from two-dimensional (2D) atomic crystals.

143 The superlattice geometry in LAO/STO offers qualitatively th

144 Here, using unit cell by unit cell superlattice growth technique, we determine the role of

145 superlattices, in order to reach anisotropic superlattice growths, yielding freestanding binary nanoc

146 ious single- and multi-component nanocrystal superlattices have been produced, the lattice structures

147 We find that rapidly self-assembled superlattices have the highest elastic modulus, despite

148 ably strong, such as 3d and 5d complex oxide superlattices, have revealed properties that only slight

149 etallic 1T-WS2 nanoribbons with zigzag chain superlattices, highly stabilized by ammonia-ion intercal

150 n processing of heterostructural nanocrystal superlattices (HNC-SLs) self-assembled from quantum-dot-

151 ther drives the formation of a PbSe nanowire superlattice in a two-dimensional (2D) perovskite matrix

152 opposed to DNA, is explored by synthesizing superlattices in which nanoparticles are bonded by DNA/D

153 solubility mediated nucleation and growth of superlattice, in which an evaporation-induced local grad

154 wth to lattice-mismatched binary nanocrystal superlattices, in order to reach anisotropic superlattic

155 Within type-II superlattices, InAs/InAs1-xSbx T2SLs have been shown to

156 o be generic to other forms of moire-forming superlattices, including van der Waals heterostructures.

157 isordered suspensions to large-scale ordered superlattices induced by nanocrystal sedimentation and e

158 at contains a large volume fraction of Cu5Zr superlattice intermetallic compound; this contributes to

159 ty single-crystal source, the orthogonal QPM superlattice is shown to suppress the spatial and tempor

160 A ZnO-graphene superlattice is synthesised via a spatially confined rea

161 First, a body-centered cubic (bcc) superlattice is synthesized through the assembly of two

162 ergence of a large variety of self-assembled superlattices is a dramatic recent trend in the fields o

163 Self-assembly of nanocrystals (NCs) into superlattices is an intriguing multiscale phenomenon tha

164 ation of void and gas bubbles in solids into superlattices is an intriguing nanoscale phenomenon.

165 scheme with shallow-well GaAs/Al0.10Ga0.90As superlattices is developed to achieve high-temperature o

166 and microstrain in DNA-mediated nanoparticle superlattices is dictated by annealing temperature and t

167 The macroscopic orientation of the superlattices is further tuned by changing the liquid su

168 engineer the bubble size and spacing of the superlattice leading to important conclusions about the

169 The uniform nanocube arrays (superlattices) led to low spatial SERS signal variances

170 e bulk and 2D hole, which usually coexist in superlattice-like doping systems.

171 The AlN/GaN digital alloy (DA) is a superlattice-like nanostructure formed by stacking ultra

172 The calcined superlattice maintains its bcc ordering and has a surfac

173 into complex colloidal supracrystals through superlattice-matched epitaxial overgrowth along the exis

174 Self-assembled nanoparticle superlattices-materials made of inorganic cores capped b

175 he lattice dimensions of silver nanoparticle superlattices may be reversibly manipulated between 0-8

176 ble superlattice architectures, which allows superlattice mechanical behavior to be linked to specifi

177 lf, it is remarkable that the orthogonal QPM superlattice meets all of these challenges without the n

178 rated for the first time using an artificial superlattice method in synthesizing 1D stripes from 2D l

179 ace plasmon/exciton interactions within such superlattice microcavities will catalyze studies involvi

180 Three-dimensional plasmonic superlattice microcavities, made from programmable atom

181 at interband transitions associated with the superlattice mini-bands in concert with free electrons i

182 t is then compared to a conventional lateral superlattice model potential.

183 Recently, a charge superlattice model that positions a small electron-like

184 proposed as a replacement for the prevalent superlattice models that position the Fermi pocket in th

185 sis of mechanically robust and self-healable superlattice nanocomposites is achieved through self-ass

186 By modelling the superlattice nanolasers with a four-level gain system an

187 is comprehensively studied as a short-period superlattice nanostructure consisting of ultra-thin III-

188 rchical structure to form Si/Ge hierarchical superlattice nanowire (H-SNW).

189 scale size effect, silicon/germanium (Si/Ge) superlattice nanowire (SNW) can have very low thermal co

190 re processing of CsPbBr3 perovskite nanocube superlattices (NC-SLs) is reported for the first time.

191 For 7-monolayer-thick LaNiO3/LaMnO3 superlattices, negative and positive exchange bias, as w

192 of the liquid in templating the formation of superlattices not achievable through self-assembly in bu

193 ere we report discovery of a new, nano-sized superlattice (NSS) phase in ball-milled Fe alloys, which

194 Most of the 3D superlattices observed to date are featured in our phase

195 l intercalation method, fabricating a hybrid superlattice of alternating inorganic TiS2 monolayers an

196 precursor (Me4N)2[Cd(SePh)4]: the first is a superlattice of monodisperse [Cd54Se32(SePh)48(dmf)4](4-

197 lasmons at the vacuum-surface interface of a superlattice of N graphene layers interacting with condu

198 We report a strategy for creating a diamond superlattice of nano-objects via self-assembly and demon

199 s a demonstration, we realize the tetragonal superlattice of octagonal gold nanorods, breaking throug

200 vironmental adsorbates into a highly regular superlattice of stripes with period 4-6 nm.

201 anopattern, and demonstrate that a synthetic superlattice of these building blocks forms an optoelect

202 45 mW m(-1) K(-2) were obtained for a hybrid superlattice of TiS2/[(hexylammonium)x(H2O)y(DMSO)z], wi

203 r optimization in a hybrid inorganic-organic superlattice of TiS2[tetrabutylammonium] x [hexylammoniu

204 The two-dimensional hexagonal close-packed superlattices of Ag nanoparticles formed in these films

205 e, orbital and lattice degrees of freedom in superlattices of alternating lead titanate and strontium

206 anocrystals act as substitutional dopants in superlattices of cadmium selenide or lead selenide nanoc

207 Here, it is shown that binary superlattices of Co/Ag nanocrystals with the same size,

208 Periodic dislocation arrays produce 2D superlattices of coherent MoS2 1D channels in WSe2.

209 We do so by synthesizing superlattices of electrically insulating perovskite oxid

210 ffraction during the growth of BaTiO3/SrTiO3 superlattices on SrTiO3 substrates by off-axis radio fre

211 Moreover, a novel honeycomb superlattice pattern is observed in experiment, where th

212 By exploring superlattice period-, temperature- and field-dependent e

213 f skipping orbits extending over hundreds of superlattice periods, reversals of the cyclotron revolut

214 array is the low-energy state for a range of superlattice periods.

215 ility of truncate NC assemblies with various superlattice polymorphs and associated NC-ligand interac

216 growth as well as transformation of various superlattice polymorphs but also lay foundation for cont

217 e structural fluctuations intrinsic to these superlattices pose a new challenge for structure determi

218 epitaxial (SrFeO2.5)1/(CaFeO2.5)1 thin film superlattices possessing both anion-vacancy order and Sr

219 irectly extract the steepness of the imposed superlattice potential.

220 We outline the extensive catalog of superlattices prepared to date using hydrocarbon-capped

221 on the final crystalline structure of binary superlattices produced by self-assembly of two sets of n

222 The charge stripe superlattice propagation vector, q = (2/3, 0, 1), corres

223 ess by a single atomic layer and coupling in superlattices recover the Fermi liquid behaviour.

224 Multicomponent nanocrystal superlattices represent an interesting class of material

225 ystallization of colloidal nanocrystals into superlattices represents a practical bottom-up process w

226 ed-cubic (fcc) and body-centered-cubic (bcc) superlattice, respectively, at concentrations </=17.5 an

227 We also find that the superlattice's mechanical response to hydrostatic compre

228 In addition, we demonstrate a novel ternary superlattice self-assembled from two different sizes of

229 Randomizing the layer thickness of superlattices (SL) can lead to localization of coherent

230 quasi-two-dimensional transition metal oxide superlattices (SLs) composed of a Mott insulator LaCoO3

231 pair separation by synthesizing Fe2O3-Cr2O3 superlattices (SLs) with precise atomic control.

232 g through the only hexagonal symmetry of the superlattice so far.

233 reveal that the ultimate coherence length of superlattices strongly depends on nanocrystal shape.

234 istries and assembly environments to control superlattice structure and produce nonbulk assemblies.

235 A crystal superlattice structure featuring nonlinear layers with a

236 f the nodes, and also point to an underlying superlattice structure of low frequency and long wavelen

237 carrier concentration without disrupting the superlattice structure prevents further improvement of t

238 ne MOF, IRMOF-74-V-hex, these domains form a superlattice structure that is difficult to reconcile wi

239 Specifically, in an AlxGa(1-x)N/GaN superlattice structure, by modulation doping of Mg in th

240 r) as a new approach to dynamically modulate superlattice structure.

241 ation distributions to modulate nanoparticle superlattice structure.

242 ng point remain to support and stabilize the superlattice structure.

243 e measurements and illustrate that while DLC superlattice structures are unlike their classical count

244 Recently, superlattice structures have been demonstrated to dramat

245 different dendritic covering) yielded binary superlattice structures of unprecedented single inorgani

246 Moire patterns are periodic superlattice structures that appear when two crystals wi

247 The first superlattice structures using DNA-NPs as building blocks

248 ons can also be controlled to form different superlattice structures, such as hexagonal close-packed

249 itive changes in the electronic structure of superlattices such that charge carriers experience effec

250 ch as WS2-WSe2-MoS2 and WS2-MoSe2-WSe2), and superlattices (such as WS2-WSe2-WS2-WSe2-WS2) were readi

251 We show that graphene superlattices support a different type of quantum oscill

252 g the solvent evaporation does not amend the superlattice symmetry, but improves the superlattice cry

253 d in the assembly process and determines the superlattice symmetry, leading to the tetragonal superla

254 and susceptible to aggregation, nanoparticle superlattices synthesized using DNA interactions offer a

255 Type-II superlattices (T2SLs) are a class of artificial semicond

256 InAs/(InAs,Ga)Sb type II superlattices (T2SLs) with different in-plane geometries

257 and fine nanocrystal size control due to the superlattice templates.

258 rlattice symmetry, leading to the tetragonal superlattice that becomes energetically favorable over i

259 ontinuous transition to a columnar hexagonal superlattice that does not display a first-order phase t

260 report a quasicrystalline binary nanocrystal superlattice that exhibits correlations in the form of p

261 nt, oleylamine (OAM), the binary nanocrystal superlattices that are produced, such as NaCl, AlB2, NaZ

262 atenar ligands self-assemble into softer bcc superlattices that deviate from conventional harder clos

263 interactions and the formation of adsorbate superlattices that extend beyond an original MOF unit ce

264 xially strained ferroelectric thin films and superlattices, the ferroelectric transition temperature

265 e DNA shells of the nanoparticles within the superlattice, thereby shifting interparticle interaction

266 2) can be achieved in thin-film Bi2Te3-based superlattice thermoelectric modules.

267 strated in these structurally disordered DLC superlattices through distinct current modulation with n

268 ate the ability of supported Au nanoparticle superlattices to catalyze alcohol oxidation.

269 nucleation and growth as well as subsequent superlattice transformation of NC assembles and undernea

270 ve and isotropic lattice expansion for three superlattice types (bcc, fcc, and AlB2) due to the inter

271 st appearance of an ordered arrangement, the superlattice underwent uniaxial contraction and collecti

272 at simple fractions of the flux quantum per superlattice unit cell.

273 faces in BiFeO3 /La0.7 Sr0.3 MnO3 (BFO/LSMO) superlattices using polarized neutron reflectometry is o

274 In addition to shrinking the superlattice volume, thermal treatment also transforms t

275 atalytically active nanoparticles within the superlattice was determined by inductively coupled plasm

276 By designing the quantum dots in a 2D superlattice, we show that new energy bands form where t

277 cted frequency and mean free path spectra of superlattices, we also investigate the existence of wave

278 e geometrical design of heterostructures and superlattices, we demonstrate the use of antiferromagnet

279 First, a variety of binary nanoparticle superlattices were prepared at the liquid-air interface,

280 ass of materials--namely, R2NiMnO6/La2NiMnO6 superlattices where R is a rare-earth ion--that exhibit

281 eport measurements of high-mobility graphene superlattices where the complete unit cell of the Hofsta

282 ized ferrimagnet based on [Mn2.9Ga/Co2MnSi]n superlattices, which attains thermal stability above 400

283 nanorod growth takes place inside organized superlattices, which can be regarded as mesocrystals.

284 ation of reconfigurable and thermally stable superlattices, which could lead to tunable and functiona

285 ical behavior of polymer-grafted nanocrystal superlattices while exploring the role of polymer struct

286 Hybrid inorganic-organic superlattice with an electron-transmitting but phonon-bl

287 nitride (h-BN) heterostructures is a lateral superlattice with high electron mobility and an unusual

288 dation for controlled fabrication of desired superlattice with tailored property.

289 rystals (NCs) can self-assemble into ordered superlattices with collective properties, but the abilit

290 at promise, as confirmed by perovskite oxide superlattices with compositional substitution to artific

291 mise for creating two- and three-dimensional superlattices with extraordinary physical properties.

292 When these are assembled into crystalline superlattices with gold nanoparticles, we find that the

293 o increase strand flexibility, gives rise to superlattices with less strain in the crystallites compa

294 Hence, the formation of binary superlattices with lower packing densities may be favore

295 In superlattices with relatively thin STO layers, we predic

296 Here we fabricated superlattices with the quantum dots registered to within

297 , and an active layer: a doped semiconductor superlattice, with electrical contacts, inserted into th

298 rystal body-centered cubic gold nanoparticle superlattices, with dye molecules coupled to the DNA str

299 d to program the crystallization behavior of superlattices, yielding access to complex three-dimensio

300 , acquiring satellite sub-Dirac cones at the superlattice zone boundaries.