ライフサイエンスコーパス: superlattice

1 Ni(4+) and Fe(3+) are observed in the n = 5 superlattice.

2 nsitive to the interparticle distance in the superlattice.

3 change the electronic band structure of the superlattice.

4 e overall dimensions of the micrometer-sized superlattice.

5 tor built as an artificial SrIrO(3)/SrTiO(3) superlattice.

6 inert [Formula: see text] counterlayers in a superlattice.

7 riodic modulation of the stacking, the moire superlattice.

8 TLG) and hexagonal boron nitride (hBN) moire superlattice.

9 breaks the rotational symmetry of the moire superlattice.

10 understandable toward achievement of desired superlattice.

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

12 egree of magnetic moment compensation in the superlattice.

13 rsion medium, obtaining a high index faceted superlattice.

14 ces the magnetic ordering temperature in the superlattice.

15 ated Chern insulator in an ABC-TLG/hBN moire superlattice.

16 app electron-electron scattering in graphene superlattices.

17 which allows the fabrication of their hybrid superlattices.

18 ting the nucleation and growth of the binary superlattices.

19 s a metal-to-insulator transition in SCO/LNO superlattices.

20 a chemical approach for actuating colloidal superlattices.

21 rs via its interaction with the buried moire superlattices.

22 orbital splitting is negligible in C-SCO/LNO superlattices.

23 mesoporous graphene derived from nanocrystal superlattices.

24 nanostructures such as heterointerfaces and superlattices.

25 hrough strain gradients present within moire superlattices.

26 nt oxides, solid solutions and larger period superlattices.

27 spintronic applications based on artificial superlattices.

28 e layers can result in long-wavelength moire superlattices.

29 and subsequently assembled them into binary superlattices.

30 on causes simultaneous nucleation of the two superlattices.

31 wo components comprising binary nanoparticle superlattices.

32 tween them causes the coexistence of the two superlattices.

33 ving forces responsible for the two distinct superlattices.

34 that BICs could be observed in semiconductor superlattices.

35 ic absorber molecules to form nanostructured superlattices.

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

37 iferroic materials through modifying natural superlattices.

38 phases in semiconducting WSe(2)/WS(2) moire superlattices.

39 heterostructures, multiheterostructures and superlattices.

40 g to unprecedented covalently doped graphene superlattices.

41 eal vdW interfaces with widely tunable moire superlattices.

42 tungsten diselenide/tungsten disulfide moire superlattices.

43 monstrated in (LuFeO(3))(m)/(LuFe(2)O(4))(1) superlattices.

44 phases of matter in multi-flat-band twisted superlattices.

45 and twisting have been used to create moire superlattices(1), enabling new optical and electronic pr

46 n reported in twisted bilayer graphene moire superlattices(1-12).

47 nd ABC trilayer graphene/boron nitride moire superlattices(1-4).

48 al misalignment introduces an in-plane moire superlattice(3).

49 rystal structures, which is known as a moire superlattice(3).

50 ociated with a Hubbard model on a triangular superlattice(5,6) where the bandwidth can be tuned conti

51 gned WSe(2)/WS(2) bilayers, which form moire superlattices(6) because of the difference between the l

52 One such structure is the LaAlO(3)/LaNiO(3) superlattice(7-9), which has been recently proposed for

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

54 This catalog of superlattices allowed us to not only study the frequency

55 a device structure employing both a strained superlattice and a heterojunction emitter.

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

57 OF nanorods (PCN-222) were assembled into 2D superlattices and found to be catalytically active for t

58 rigin of high-temperature magnetism in these superlattices and the charge-ordering pattern in the m =

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

60 n the evolution of the vortex state in these superlattices (and the associated electrostatic and elas

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

62 rature like normal DNA or DNA-interconnected superlattices, and they can be moved from water to organ

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

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

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

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

67 cting the self-assembly of NCs into coherent superlattices are also discussed, which provides a deep

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

69 Semiconductor quantum-well structures and superlattices are key building blocks in modern optoelec

70 Nanocrystal superlattices are typically prepared by carefully contro

71 rmining size and structure of the gas bubble superlattice as a function of irradiation conditions.

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

73 ted crystallographic alignment of the entire superlattice, as opposed to just the individual particle

74 The rhombic superlattice assembled from SD/Ag78a through intercluste

75 Nanoparticle superlattice assembly has been proposed as an ideal mean

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

77 ics of In(0.53)Ga(0.47)As/Al(0.48)In(0.52)As superlattice avalanche photodiodes (InGaAs/AlInAs SL APD

78 At half-filling of the first hole moire superlattice band, we observe a Mott insulating state wi

79 emonstration of electrostatic control of the superlattice bands over a wide energy range has, so far,

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

81 metric twist of the layers, leading to moire superlattices between the atomic layers.

82 r studies highlight the value of using moire superlattices beyond graphene to explore correlated phys

83 for creating artificial heterostructures or superlattices beyond the reach of existing materials.

84 achieved in a single reduced-dimensional TI-superlattice, (Bi(2) /Bi(2) Se(3) )-(Bi(2) /Bi(2) Se(3)

85 onfirm the formation of single-component MOF superlattices, binary MOF-Au single crystals, and two-di

86 ate, at least 15 distinct binary nanocrystal superlattice (BNSL) structures have been identified.

87 le of 12.2 degrees is selected such that the superlattice Brillouin zone is sufficiently large to ena

88 e we show that, in graphene-on-boron-nitride superlattices, Brown-Zak fermions can exhibit mobilities

89 s study provides new opportunities to design superlattices by chemically modifying simple perovskite

90 angle-aligned WSe(2)/WS(2) and MoSe(2)/WS(2) superlattices by optical reflectance spectroscopy.

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

92 synthesis of (SrNiO(3) )(m) /(LaFeO(3) )(n) superlattices by tuning n and m.

93 tride structures(4), the presence of a moire superlattice can lead to the observation of electronic m

94 It is widely recognized that the moire superlattice can modulate the electronic band structure

95 As a result, the superlattices can be programmed either to reorganize the

96 Moire superlattices can be used to engineer strongly correlate

97 electronic properties of van der Waals moire superlattices can further be tuned by adjusting the inte

98 cally precise, low-dimensional ferroelectric superlattices can lead to exotic polar structures, such

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

100 The superlattice channels produced multiple states due to cu

101 ssing through an ultrathin NaYF(4) /NaGdF(4) superlattice cladding (thickness: 6.9 nm).

102 From rock salt to nanoparticle superlattices, complex structure can emerge from simple

103 eport the tuning of magnetic interactions in superlattices composed of single and bilayers of SrIrO(3

104 In superlattices comprised of alternating one-unit-cell of

105 Here, we report decoupled multi-quantum-well superlattices comprised of the colloidal quantum wells o

106 We developed a bulk superlattice consisting of the transition metal dichalco

107 ansistors were realized by applying a hybrid superlattice consisting of zinc oxide composite nanolaye

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

109 g m = 1, spectroscopy reveals that the n = 1 superlattice contains Ni(3+) and Fe(4+) , whereas Ni(4+)

110 made assembling nanocrystals into different superlattices, controlling the relative orientations of

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

112 the superlattice symmetry, but improves the superlattice crystallinity.

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

114 ls platform for complex and molecularly thin superlattices, devices and integrated circuits.

115 we find experimentally that the ABC-TLG/hBN superlattice displays Mott insulating states below 20 ke

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

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

118 resulting in a resonant enhancement of moire superlattice effects.

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

120 Moire superlattices enable the generation of new quantum pheno

121 nocrystal precursors as ordered close-packed superlattices enables microscopy studies that deepen the

122 Here we report the observation of moire superlattice exciton states in tungsten diselenide/tungs

123 In quantizing magnetic fields, graphene superlattices exhibit a complex fractal spectrum often r

124 The Bi(2) -terminated superlattice exhibits a single Dirac cone with a spin mo

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

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

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

128 e superlattice is formed by converting a DNA superlattice first into highly-structured 3D silica scaf

129 a promise route for engineering topological superlattices for high-performance TI-spintronic devices

130 ecent theoretical predictions for gas bubble superlattice formation and highlight that superlattice f

131 e discover spontaneous symmetry breaking and superlattice formation in DSA of BCP.

132 le superlattice formation and highlight that superlattice formation is strongly dependent on the diff

133 oups both play critical roles in driving the superlattice formation.

134 We assemble 3D DNA superlattices from octahedral DNA frames with incorporat

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

136 ilar to those observable when the gas bubble superlattice has formed with very large ordering paramet

137 to characterize the local structure of moire superlattices has thus far impeded progress in the field

138 er extractor based on type-II InAs/AlSb/GaSb superlattices have been demonstrated.

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

140 ced effects on single-particle states, moire superlattices have recently been predicted to host excit

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

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

143 erstand the formation of the void/gas bubble superlattices in crystals under irradiation, we establis

144 ation of nanometer-scale properties of moire superlattices in van der Waals heterostructure devices i

145 Moire superlattices in van der Waals heterostructures have giv

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

147 s to create the decoupled multi-quantum-well superlattices, in which individual 2D material layers ar

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

149 U(84) assembles into superlattices including cubic-closest packed, body-cente

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

151 simulations, we found that the symmetry of a superlattice is determined by the coupling of diffusion

152 The electronic behaviour in the ABC-TLG/hBN superlattice is expected to depend sensitively on the in

153 The superconductive superlattice is formed by converting a DNA superlattice

154 eases, indicating improved ordering, until a superlattice is formed.

155 In contrast, the Bi(2) Se(3) -terminated superlattice is identified as a dual TI protected by coe

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

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

158 moment orientation of bright excitons in the superlattices is predominantly in-plane and independent

159 of PbTiO(3) layers (moving from trilayer to superlattices), it is possible to manipulate the long-ra

160 POEGMA-PS self-assembles into a superlattice lamellar morphology, a previously unknown c

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

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

163 died spin dynamics of charge carriers in the superlattice-like Ruddlesden-Popper hybrid lead iodide p

164 nd show that phase domain walls tend to form superlattice-like structures along the c axis.

165 toelectronic properties characteristic of 2D superlattice materials with tunable quantum well thickne

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

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

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

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

170 d at a small twist angle, the resulting flat superlattice minibands are expected to strongly enhance

171 e leads to the emergence of ultra-flat moire superlattice minibands.

172 This study highlights the accessibility of superlattice morphologies by introducing charges in a co

173 ere we report the discovery of an intriguing superlattice morphology from compositionally symmetric c

174 Moire superlattices (MSLs) are modulated structures produced f

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

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

177 Additionally, its superlattice nature may make various heterostructures of

178 Therefore, the low saturation field and the superlattice nature of MnBi(4)Te(7) make it an ideal sys

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

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

181 We defined a superlattice of COFs by engineering channels with a pers

182 oxide heterostructures, the oxynitride has a superlattice of insulating and metallic blocks.

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

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

185 Using resonant X-ray reflectivity, a superlattice of SrFeO(3) and CaFeO(3) is shown to exhibi

186 ls material Bi(4)O(4)SeCl(2), which is a 1:1 superlattice of the structural units present in the van

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

188 metallicity in GNRs by inserting a symmetric superlattice of zero-energy modes into otherwise semicon

189 nd response under applied electric fields in superlattices of (PbTiO(3))(n)/(SrTiO(3))(n) suggests th

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

191 y employing infrared light for imaging moire superlattices of twisted bilayers graphene encapsulated

192 Therefore, moire superlattices of two-dimensional materials manifest them

193 Moire superlattices offer an unprecedented opportunity for tai

194 ns(5-7); however, the influence of the moire superlattice on optical properties has not been investig

195 st decade as building blocks in constructing superlattices or dynamic aggregates, under the effect of

196 nerally identified based on the existence of superlattice ordering peaks in powder X-ray diffraction

197 increasing temperature and a flux-dependent superlattice parameter that decreases with increasing fl

198 observed, including a temperature-dependent superlattice parameter that increases with increasing te

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

200 Provided the superlattice period extends over many unit cells, the co

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

202 re, as well as the stabilization of a unique superlattice phase that only exists when magnetic coupli

203 orce one another and stabilize the resulting superlattice phases.

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

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

206 By introducing a moire superlattice potential (via aligning bilayer graphene wi

207 imensional materials, a moire pattern with a superlattice potential can be formed by vertically stack

208 ed by both the atomic lattice and long-range superlattice potentials arising in interlayer moire patt

209 stals can be modified substantially by moire superlattice potentials from an interlayer twist between

210 Strong superlattice potentials generate moire minibands of exci

211 r band-structure engineering via twist moire superlattice potentials.

212 is a key material in this regard because the superlattice produced by the rotated graphene layers int

213 /hexagonal boron nitride (ABC-TLG/hBN) moire superlattice provides an attractive platform with which

214 nce of transition metal dichalcogenide moire superlattices provides a highly controllable platform in

215 The rate of decay of superlattice reflections of the (SnSe(2))(1+gamma)(TiSe(

216 The set of {h + 1/2, k + 1/2, l + 1/2} superlattice reflections was observed for the first time

217 We find that all moire superlattices, regardless of whether the constituent lay

218 The freestanding 2D superlattices reported to date are typically constructed

219 2D freestanding nanocrystal superlattices represent a new class of advanced metamate

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

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

222 lize the large variety of different reported superlattices self-assembled from seemingly similar part

223 s reported to grow 2D Janus gold nanocrystal superlattice sheets with nanocube morphology on one side

224 eveal a Mott insulator state at one hole per superlattice site and surprising insulating phases at 1/

225 bout a filling factor of half a particle per superlattice site.

226 nsion plays a pivotal role in determining NC superlattice (SL) structure and orientation.

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

228 either a single InGaN underlayer or an InGaN superlattice (SLS) structure (both with low InN content)

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

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

231 d represents a novel mechanism for directing superlattice structure and highlights the experimental i

232 ions represents a powerful strategy to alter superlattice structure and stability, which can impact d

233 A crystal superlattice structure featuring nonlinear layers with a

234 The superlattice structure is stabilized by the configuratio

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

236 ation distributions to modulate nanoparticle superlattice structure.

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

238 amework to predict the symmetry selection of superlattice structures associated with anisotropic diff

239 contraindicated, but through the creation of superlattice structures both expanded unit-cell volume a

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

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

242 semble into crystalline, pseudo-1D elongated superlattice structures.

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

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

245 d structure with a single parameter in moire superlattices, such as twisted bilayer graphene by tunin

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

247 mergent phenomena can controllably alter the superlattice symmetry by using the mesoscale particle ar

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

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

250 rystals offers a strategy for creating other superlattice systems and, in particular, for exploring i

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

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

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

254 The interlayer twist gives rise to a moire superlattice that affects the electronic motion and alte

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

256 stortion vortex on a 2D mechanical honeycomb superlattice that can be mapped to a magnetic flux vorte

257 sh a new solid-state platform based on moire superlattices that can be used to simulate problems in s

258 In ferroelectric thin films and superlattices, the polarization is intricately linked to

259 an increase "bond strength", as evidenced by superlattice thermal stability enhancements of >60 degre

260 lows the modulus of DNA-grafted nanoparticle superlattices to be easily tuned overly nearly 2 orders

261 principles) simulations in SrTiO(3)/PbTiO(3) superlattices to directly determine, with atomic resolut

262 ur study lays the groundwork for using moire superlattices to simulate a wealth of quantum many-body

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

264 ly-coherent columnar plasmonic nanostructure superlattice-type thin films with high porosity and stro

265 typically associated with the formation of a superlattice under a built-in field.

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

267 ) fractions of the magnetic flux quantum per superlattice unit cell.

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

269 nipulate the vortices in a PbTiO(3)/SrTiO(3) superlattice via atomically resolved in-situ scanning tr

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

271 Prior to the formation of a superlattice, we observe a persistent substructure chara

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

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

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

275 noscale building blocks in three-dimensional superlattices, where nanoparticles densely modified with

276 ferent types of graphene/boron nitride moire superlattices, whereas correlated insulating states and

277 cupation up to ~30% is achieved in P-SCO/LNO superlattices, whereas the Ni e(g) orbital splitting is

278 ulating phases at 1/3 and 2/3 filling of the superlattice, which we assign to generalized Wigner crys

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

280 particles is a powerful way for preparing 3D superlattices, which may be useful in many areas, includ

281 Moire superlattices-which are created by stacking van der Waal

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

283 lemental-modulated layers into an artificial superlattice with Pb and Sn in independent layers, creat

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

285 mes at their vertices, which result in cubic superlattices with a 48 nm unit cell.

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

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

288 ionalized with DNA can assemble into ordered superlattices with defined crystal habits through progra

289 or the design and fabrication of nanocrystal superlattices with enhanced structural control.

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

291 mers were used to fabricate arrays of hybrid superlattices with molybdenum disulfide that could be us

292 superstructures, including recently observed superlattices with partial and short-ranged orientationa

293 of small gold satellites, into close-packed superlattices with pronounced orientational alignment of

294 ambient method to visualize real-space moire superlattices with sub-5-nm spatial resolution in a vari

295 to the self-organization of nanobubbles into superlattices with symmetry similar to the metal host ma

296 grammed to crystallize into a diverse set of superlattices with well-defined crystal symmetries and c

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

298 formation and structure of helium gas bubble superlattices within a tungsten host matrix to uncover m

299 ment as compared with the symmetric nanocube superlattices without Janus structures.

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