ライフサイエンスコーパス: 2D

1 2D covalent organic frameworks (2D COFs) are a unique ma

2 2D covalent organic frameworks (COFs) could have well-de

3 2D hybrid halide perovskites with the formula (A')(2) (A

4 2D maps of NLS-GFP recovery times showed no pixel-by-pix

5 2D materials that are piezoelectric, i.e., that allow fo

6 2D materials, such as graphene, exhibit great potential

7 2D measurements consider heterogeneity within a single o

8 2D proton nuclear magnetic resonance and SAXS data provi

9 2D semiconductors have shown great potential for applica

10 2D-IR spectra of blood serum samples supplemented with v

11 venting the restacking by fabricating 2D-0D, 2D-1D, and 2D-2D layer-by-layer composite structures are

12 constructed van der Waals 1T-MoS(2)/C(60) 0D-2D heterostructures via a one-pot synthetic approach for

13 The one-step generated 0D-2D bio-composite sensing film demonstrates synergetic ef

14 0) ]) oxo-caps can be exploited to build 1D, 2D, and 3D inorganic frameworks.

15 Additionally, the potential of 1D/2D NMR-based untargeted analysis was successfully tested

16 ar features can be selected in any of the 1D/2D/3D windows as sets of residues and these selections a

17 The luminance overshoot ratio of 3D/2D hybrid PeLED is only 7.4% which is greatly lower than

18 The 3D/2D hybrid perovskite is obtained by adding a small amoun

19 A 2D array of bismuth-substituted iron-garnet nanopillars

20 A 2D DNA sheet could be modularized into connected parts (

21 ne learning with deep learning approaches, a 2D dense convolutional neural network (CNN) was implemen

22 cell model and cultured cell monolayers as a 2D cell model.

23 Borophene, a 2D allotrope of boron and the lightest elemental Dirac m

24 To fill this critical gap, we developed a 2D implementation of the Regional Ocean Modeling System

25 calibration, adequate data redundancy from a 2D array of 2048 elements and a paraxial approximation.

26 Herein, a 2D titanium carbide (Ti(3) C(2) ) MXene film with transp

27 he dynamical processes of interstitials in a 2D colloidal crystal.

28 the distribution of compounds embedded in a 2D map, based on the similarity of structural properties

29 electrons that are instead localized near a 2D van Hove singularity explains the anomalous transport

30 The protocol includes the application of a 2D (1)H-(31)P HSQC-TOCSY experiment to detect (31)P-labe

31 The structure of a 2D-COF consists of two dimensional sheets held together

32 In addition, 2D CCFs exhibit certain notable properties (e.g., excell

33 gel reaction and imine-linked 2D COF analog (2D-C=N-PPQV1, E(g) =2.3 eV), unambiguously proving the s

34 spectrometry (UHPLC-HRMS) supported by 1 and 2D NMR spectroscopy was used for unambiguous metabolic p

35 onstruction of dynamically responsive 1D and 2D assemblies that undergo a structurally programmed mor

36 n profiles can be obtained from noisy 1D and 2D NMR data with high temporal resolution, allowing furt

37 demonstrates the proof of concept for 1D and 2D NMR methods in the targeted and untargeted analysis o

38 lear magnetic resonance spectroscopy (1D and 2D NMR) and high-resolution tandem mass spectrometry (HR

39 by single-crystal X-ray diffraction, 1D and 2D solid-state (19)F NMR spectroscopy supported by ab in

40 restacking by fabricating 2D-0D, 2D-1D, and 2D-2D layer-by-layer composite structures are discussed.

41 lative to three-dimensional MWW (MCM-22) and 2D layers prepared from postsynthesis exfoliation (ITQ-2

42 Although structured water adlayers and 2D ice have been imaged, capturing the metastable or int

43 tricity, and enable combining dielectric and 2D electronic materials.

44 of the obtained 2D-PPQV1 (E(g) =2.2 eV) and 2D-PPQV2 (E(g) =2.2 eV) are compared with those of cyano

45 association between transgender identity and 2D:4D indicating the influence of prenatal androgen on t

46 ta set of one-dimensional (1D) (31)P NMR and 2D (1)H-(31)P HSQC-TOCSY spectra of 38 common phosphorus

47 ine one-dimensional (1D) nanowires (NWs) and 2D graphene flakes grown out-of-plane for highly control

48 and calcium signaling in both organoid- and 2D-derived cortical neurons.

49 (phenylenequinoxalinevinylene)s 2D-PPQV1 and 2D-PPQV2, via the Horner-Wadsworth-Emmons (HWE) reaction

50 tory comparative study of the 1D PROFILE and 2D methyl methods on several mAbs samples to determine t

51 from experiments with murine xenografts and 2D and 3D co-cultures of NHFs and PDAC cells revealed th

52 apable of generating a sequence of arbitrary 2D spatial/polarisation wavefronts at a bandwidth limite

53 Classical diffractive optics are 2D diffractive optical elements (DOEs) and computer-gene

54 ch was then subjected to DIA (referred to as 2D-DIA) quantitative analysis.

55 ution configuration was designed to automate 2D-LC-MS/MS.

56 HATN-BDAN (2D CCP-BD), the bithiophene-based 2D CCP-Th exhibits a wide light-harvesting range (up to

57 esponding biphenyl-bridged 2D CCP-HATN-BDAN (2D CCP-BD), the bithiophene-based 2D CCP-Th exhibits a w

58 with a discussion of the prospects of beyond 2D TMD crystals in optoelectronics, catalysis, and quant

59 get and other redox regulatory genes in both 2D- and 3D-culture systems, uncovering a vulnerability o

60 ared with the corresponding biphenyl-bridged 2D CCP-HATN-BDAN (2D CCP-BD), the bithiophene-based 2D C

61 imensional (1D) imino (1)H NMR as well as by 2D HyperW NMR spectra acquired upon simultaneous injecti

62 Their complex structures were determined by 2D NMR studies as well as crystalline-sponge-based X-ray

63 Magnetic crystals formed by 2D layers interacting by weak van der Waals forces are c

64 inity capture, targeted analyte isolation by 2D-LC, and targeted detection by multiple reaction monit

65 ng-range ordered (crystalline) sheets called 2D polymers have recently been synthesized by irradiatin

66 ased high-performance liquid chromatography (2D chip-HPLC) approach, which enables multiple transfers

67 tears by both networks was also comparable (2D CNN, sensitivity of 82% [14 of 17] and specificity of

68 ly of anisotropic nanoparticles into complex 2D and 3D assemblies is one of the most promising strate

69 Chromatographic fingerprinting on composite 2D chromatograms from samples belonging to the same clas

70 nd woven textiles or on optimally configured 2D/3D structures such as serpentines and helical coils o

71 he C=C bond formation reaction to constitute 2D sp(2) carbon-conjugated frameworks.

72 products, composites and devices containing 2D materials.

73 s as strong as that observed in conventional 2D piezoelectric materials.

74 ion of 2DPs that form electronically coupled 2D heterostructures remains an outstanding challenge.

75 mple and straightforward method for covalent 2D patterning of graphene remains challenging.

76 ion and opens up a simple avenue to creating 2D membranes through molecular self-assembly for highly

77 d formation for the synthesis of crystalline 2D CPs.

78 sts that all of the materials in the current 2D library could be rolled into their 1D counterparts an

79 The Ni-DBA-2D-COF catalytic system displays excellent recyclability

80 curve resolution approach (MCR), to denoise 2D solid-state NMR spectra, yielding a substantial S/N r

81 grating CRISPR Engineering and hiPSC-Derived 2D Disease Modeling Systems, by Kristina Rehbach, Michae

82 Herein, we apply recently developed 2D characterization techniques to nanoparticles using at

83 dulate the structure of a recently developed 2D perovskite (HA)(2) (GA)Pb(2) I(7) (HA=n-hexylammonium

84 de separation orthogonality for 16 different 2D LC-ESI MS systems has been evaluated.

85 ghest reported for lead-free low-dimensional 2D and 1D perovskites and metal halides.

86 ting the rapid acquisition of 2-dimensional (2D) (15)N-(1)H NMR correlations, and thereby combining a

87 The discovery of 2-dimensional (2D) materials, such as CrI(3), that retain magnetic orde

88 vable in the edge currents of 2-dimensional (2D) topological band insulators with broken time-reversa

89 nt (PROFILE) method and the two-dimensional (2D) (1)H-(13)C methyl correlation-based approach.

90 m protein cages to extended two-dimensional (2D) and three-dimensional (3D) crystalline arrays.

91 rol of cellular activity in two-dimensional (2D) and three-dimensional (3D) platforms.

92 cells are immobilized in a two-dimensional (2D) array, with osmotically induced changes in droplet v

93 investigation on graphene, two-dimensional (2D) carbon-rich conjugated frameworks (CCFs) have attrac

94 Here, we isolate a two-dimensional (2D) chalcogenide quasicrystal and approximant, and inves

95 nal (3D) and the other with two-dimensional (2D) convolutional kernels.

96 f their advantages over the two-dimensional (2D) counterparts in fields of plasmonics, photonic cryst

97 p a formalism that maps the two-dimensional (2D) elastic problem into that of nonlinear interaction o

98 The advent of the two-dimensional (2D) family of halide perovskites and their demonstration

99 EEM) spectrometer generates two-dimensional (2D) fluorescence matrices at a data acquisition rate of

100 cinating feature of certain two-dimensional (2D) gapless quantum spin liquid (QSL) is that their spin

101 sorbed into a comprehensive two-dimensional (2D) gas chromatography (GC x GC) system coupled with low

102 tion in a tissue in situ is two-dimensional (2D) histopathology.

103 plementation of an array of two-dimensional (2D) layered conductive metal-organic frameworks (MOFs) a

104 determined that the compact two-dimensional (2D) LiInP(2)Se(6) detectors resolved the full-energy pea

105 Two-dimensional (2D) materials are at the forefront of materials research

106 HSV-1 infection of two-dimensional (2D) neuronal cultures causes intracellular accumulation

107 One-dimensional (1D) and two-dimensional (2D) NMR studies revealed that in fused sapphyrins, the f

108 ing Raman spectroscopy with two-dimensional (2D) perturbation correlation moving window (2DPCMW) anal

109 sheet of light to bleach a two-dimensional (2D) plane and subsequently image the recovery of the sam

110 entous cells that grow in a two-dimensional (2D) plane through a series of asymmetric cell divisions.

111 scenes from information in two-dimensional (2D) retinal images.

112 rly 1990s, the synthesis of two-dimensional (2D) silica nanostructures remains challenging.

113 st tomosynthesis (DBT) with two-dimensional (2D) synthetic mammography (SM) or standard 2D digital ma

114 Two-dimensional (2D) ternary materials recently generated interest in opt

115 rough research conducted on two-dimensional (2D) TMD crystals, it is vital to seek new research oppor

116 chiral-chiral heart-cutting two-dimensional (2D)-LC method has been developed to determine both the y

117 (SPEED) microscopy and its two-dimensional (2D)-to-3D transformation algorithm to provide an effecti

118 Newly discovered 2D Janus transition metal dichalcogenides layers have ga

119 n fiber organizations is formed by expanding 2D nanofiber membranes composed of multiple regions coll

120 have motivated increasing efforts to explore 2D CCFs for electrochemical energy applications.

121 for preventing the restacking by fabricating 2D-0D, 2D-1D, and 2D-2D layer-by-layer composite structu

122 terials and demonstrate their adaptation for 2D materials using carbon nitride and graphene materials

123 dset with respect to suitable insulators for 2D technologies may be required.

124 ized 2D material / ferromagnet interface for 2D-MTJs.

125 )O as an internal normalization standard for 2D-IR spectra.

126 A new cobalt metal-organic framework (2D-Co-MOF) based on well-defined layered double cores th

127 2D covalent organic frameworks (2D COFs) are a unique materials platform that combines c

128 interfaces, production of native oxides from 2D semiconductors and more intensive studies on crystall

129 Particle picking from 2D micrographs remains a challenging early step in the C

130 Ranging from 2D assemblies to peptide amphiphile-based biomaterials,

131 ections enable the developmental switch from 2D to 3D, but insights into the underlying mechanisms co

132 ss these issues using a thiol-functionalized 2D conjugated metal-organic framework as an electron-ext

133 Furthermore, 2D proton-detected (1)H-(17)O heteronuclear correlation

134 e single-crystal hBN paves the way to future 2D electronics.

135 protein recovery for every pixel in a given 2D slice, thus moving FRAP measurements beyond these pre

136 azine-2,3-dicarboxylic acid) inhibits GluN2C/2D with 40-fold selectivity over GluN2A-containing recep

137 owever, challenging, since epitaxially grown 2D layers exhibit complex restructurings coexisting on t

138 o the well-characterized murine MHC allele H-2D(b) are known, by applying thresholds for geometric fl

139 ess this gap in knowledge, we developed an H-2D(b) LoxP-transgenic mouse system using otherwise MHC c

140 nse restricted by the MHC class I molecule H-2D(b) The identity and function of the APC(s) involved i

141 dominant TMEV peptide VP2(121-130) Loss of H-2D(b) on CD11c(+) APCs mitigates the CD8 T cell response

142 nificantly higher (i.e. feminized) left-hand 2D:4D in the male-to-female transgender (MtF) identity [

143 However, 2D COFs typically form insoluble aggregates, thus limiti

144 The presented HTA 2D-LC platform has had a significant impact on drug deve

145 lation by proximity effect at the hybridized 2D material / ferromagnet interface for 2D-MTJs.

146 standard for diagnosis involves 3D imaging, 2D imaging by fundus photography is usually used in scre

147 The Li-impregnated 2D and 3D COFs show a significant room-temperature ion c

148 delocalized excitonic processes available in 2D COFs, which motivate their continued design and imple

149 The atomic buckling in 2D "Xenes" (such as silicene) fosters a plethora of exot

150 llular delivery was achieved in all cells in 2D cultures of a human bladder epithelial progenitor cel

151 onse induced by oxidation-related defects in 2D black phosphorus (BP) is exploited to achieve visual

152 alide perovskites and their demonstration in 2D/three-dimensional (3D) hierarchical film structures b

153 results suggest a significant difference in 2D:4D among MtF individuals compared to male controls [g

154 ated control of light-matter interactions in 2D materials and related heterostructures.

155 h implies huge sp-d exchange interactions in 2D monolayer regimes, leading to diluted magnetic semico

156 whether the mechanisms used for migration in 2D unconfined environments are relevant in 1D confined e

157 ctures to large-scale device performances in 2D semiconductors, the study provides insights into the

158 a surge of both pure and applied research in 2D magnetism.

159 and performed genome-wide CRISPR screens in 2D monolayers and 3D lung-cancer spheroids.

160 peptide-decorated nanoparticles was shown in 2D culture and further demonstrated in spheroids.

161 .e., septum transversum mesenchyme (STM), in 2D cultures.

162 ith measurement of histological thickness in 2D, and the resultant laminar atlas provides an unpreced

163 ns of Abeta42 accumulation in HSV-1 infected 2D (neuronal monolayers) and 3D neuronal cultures (brain

164 Ultrafast two-dimensional infrared (2D-IR) spectra can now be obtained in a matter of second

165 lectronic quality, and clean-limit inorganic 2D superconductivity.

166 etween the HAp and collagen molecules inside 2D voids within the fibril.

167 pt complex 3D measures into an interpretable 2D view, and a novel way to assess the quality of flow e

168 novel route to activate inert In(OH)(3) into 2D black In(2) O(3-) (x) nanosheets via photoinduced def

169 ented well-organization of the emitters into 2D rectangular columnar-like supramolecular structure st

170 he synthesized alloys can be exfoliated into 2D structures, and some of them exhibit: i) outstanding

171 rategy to link molecules and 1D ribbons into 2D cystalline frameworks.

172 ecifically, discretizing desired shapes into 2D ribbon components allows for analytic solutions to th

173 used to process the colloidal solution into 2D and 3D COF shapes as well as to generate a COF ink th

174 However, the invalid 2D architecture of fabric limits the application in ther

175 iant nanosheets represent one of the largest 2D supramolecular materials ever made, with potential ap

176 Here, various monolayer or few-layer 2D materials are presented in the conventional vertical

177 ere is an association between right and left 2D:4D (biomarker of prenatal sex steroids exposure) and

178 by the Knoevenagel reaction and imine-linked 2D COF analog (2D-C=N-PPQV1, E(g) =2.3 eV), unambiguousl

179 lts suggest improved control of imine-linked 2D COF formation can be obtained through manipulation of

180 terature indicate that periodic imine-linked 2D structures form within 60 s, which then form more ord

181 superior conjugation of the vinylene-linked 2D CPs using the HWE reaction.

182 trate the first synthesis of vinylene-linked 2D CPs, namely, 2D poly(phenylenequinoxalinevinylene)s 2

183 compared with those of cyano-vinylene-linked 2D-CN-PPQV1 (E(g) =2.4 eV) produced by the Knoevenagel r

184 for facilitated charge transfer, which make 2D CCP-Th a promising candidate for PEC water reduction.

185 erature synthesis of 2D graphitic materials (2D-GMs) remains an elusive aim, especially with electroc

186 oxides, Xenes, Mxenes and other non-metallic 2D materials.

187 In narrowband modulation 2D MS, we were able to separate the fragment ion pattern

188 Black phosphorus (BP) is a monoelemental 2D material predicted to be piezoelectric because of its

189 field of modern electronics, their monolayer 2D analogues have shown great promise for next-generatio

190 appearance of piezoelectricity in multilayer 2D material generally arises from the opposite orientati

191 nfigurations, such as plasmonic, multilayer, 2D, or metamaterial applications.

192 synthesis of vinylene-linked 2D CPs, namely, 2D poly(phenylenequinoxalinevinylene)s 2D-PPQV1 and 2D-P

193 he optoelectronic properties of the obtained 2D-PPQV1 (E(g) =2.2 eV) and 2D-PPQV2 (E(g) =2.2 eV) are

194 ssary conditions for the safe application of 2D materials.

195 e essential in many emerging applications of 2D materials such as semipermeable membranes; hence, the

196 tic exploration of EMI shielding behavior of 2D Ti(3) C(2) T(x) MXene assembled films over a broad ra

197 n this work, the optical characterization of 2D materials is used as a case study, and a neural-netwo

198 anus crystals represent an exciting class of 2D materials with different atomic species on their uppe

199 with this fascinating and emerging class of 2D materials.

200 rials, followed by other emerging classes of 2D materials including transition metal dichalcogenides

201 o benzylamine and enables crystallization of 2D perovskite without destroying the 3D phase.

202 From measurements of the dependence of 2D (13)C-(13)C ssNMR spectra on the time between mixing

203 help pave the way for future developments of 2D polymers by those interested in joining the effort wi

204 in with a brief overview of the evolution of 2D TMD research, discussing both the synthetic methods t

205 ayer materials, thus enlarging the family of 2D-materials based on graphene.

206 rization and biological functionalization of 2D MoS(2) flakes, epitaxially grown on sapphire, to deve

207 the material and thickness identification of 2D materials with high prediction accuracy and real-time

208 ng technique that enables the integration of 2D COFs into thin-film device architectures.

209 es as an ideal platform for investigation of 2D transport anisotropy and chiral charge transport as a

210 ates the general film formation mechanism of 2D halide perovskites during one-step spin-coating.

211 ied using solely the library-based method of 2D ultraviolet fragmentation spectroscopy-mass spectrome

212 ate the efficacy of ICT12035, in a number of 2D and 3D proliferation and invasion in vitro assays and

213 ects in COFs and highlights the potential of 2D c-COFs to display high conductivities and mobilities

214 serve as folding hinges during a process of 2D to 3D conversion via a deterministic buckling process

215 c chemical, physical and optical property of 2D materials can influence the performance of bio/sensin

216 alyzing the precise structural regulation of 2D CCFs.

217 real-space imaging of the edge structures of 2D bilayer hexagonal ice grown on a Au(111) surface.

218 Room-temperature synthesis of 2D graphitic materials (2D-GMs) remains an elusive aim,

219 nt vendors (P = .07) and higher than that of 2D CNN (DSC, 0.54 +/- 0.26 vs 0.48 +/- 0.29; P = .02).

220 Deterministic transformations of 2D patterns of materials into well-controlled 3D mesostr

221 This study investigated the use of 2D ultrasound imaging to quantify transverse muscle osci

222 The utility of 2D MOFs in voltammetric sensing is measured by the detec

223 Since graphene, a variety of 2D materials have been fabricated in a quest for a tanta

224 d infrared imaging under scattering based on 2D materials has yet to be realized.

225 Here, we report on 2D DJ phase perovskites using a 3-(aminomethyl)piperidin

226 the offline approach, we developed an online 2D ultrahigh-pressure nano-LC system for high-pH and low

227 The optimized 2D-DIA method allowed for improved identification and qu

228 s can be realized with these highly oriented 2D films.

229 vel (LL) structure(1-3), distinct from other 2D electron systems.

230 ue Native-PAGE and Blue Native-PAGE/SDS-PAGE 2D analyses demonstrated co-existence of the alpha1 subu

231 In this paper, we perform 2D Fourier analysis of the full bunch longitudinal phase

232 esign new 3D graphene devices with preserved 2D electronic properties and novel functionalities.

233 ve been shown to be far superior to previous 2D monolayer models.

234 ed using a combination of solution-processed 2D-molybdenum disulfide and graphene-oxide (GO) that can

235 economical method to fabricate programmable 2D patterns of chiral PDA with tailored chirality distri

236 Dirac material, is the latest very promising 2D material owing to its unique structural and electroni

237 on and a polar solvent leads to high-quality 2D perovskite films with sandwich-type structures and ve

238 Quasi-2D Ruddlesden-Popper halide perovskites with a large exc

239 Here we show that the plasmons in real quasi-2D metals are qualitatively different, being virtually d

240 rtant to control the morphology of the quasi-2D films to achieve efficient energy transfer, which is

241 between second-to-fourth digit length ratio (2D:4D), a proxy for prenatal androgen load, and transgen

242 cellular recordings from mice exploring real 2D arenas demonstrate that grid cells within these three

243 axon morphologies drive previously reported 2D trends in axon diameter and g-ratio.

244 ting on graphene toward a spatially resolved 2D-patterned architecture.

245 The resultant 2D c-COF ZnPc-pz-I(2) maintains its structural integrity

246 mely, 2D poly(phenylenequinoxalinevinylene)s 2D-PPQV1 and 2D-PPQV2, via the Horner-Wadsworth-Emmons (

247 luding the two-dimensional tandem mass scan (2D MS/MS scan) in which all precursor ions and their sub

248 tional order of nanorods within side-to-side 2D assemblies and shows that both electrostatic (at the

249 deep learning to make predictions via simple 2D images without sophisticated 3D-imaging equipment and

250 -free conditions, the structures of solvated 2D COFs are largely unexplored.

251 is driving the preparation of sophisticated 2D, 3D, and 4D materials at the nano-, micro-, and macro

252 ragmentation spectroscopy-mass spectrometry (2D UV-MS) of cold ions.

253 uid chromatography-tandem mass spectrometry (2D-LC-MS/MS) method which combines commercially availabl

254 maged using 2D-optical imaging spectroscopy (2D-OIS).

255 (2D) synthetic mammography (SM) or standard 2D digital mammography (DM) results in detection of more

256 As such, 2D materials are promising for hybrid systems that coupl

257 The hydrogel is cytocompatible and supports 2D/3D cell growth.

258 mensional self-assembly, most supramolecular 2D materials are assembled by tedious methodologies, wit

259 ok about the future development of synthetic 2D CCFs for electrochemical applications, which concerns

260 col (6-mm slabs with 3-mm overlap, synthetic 2D mammogram) with a crossover design.

261 bs with 5-mm overlap, 1-mm slices, synthetic 2D mammogram) and an experimental protocol (6-mm slabs w

262 A targeted-2D-with-dilution configuration was designed to automate

263 Recently, we demonstrated that 2D-IR spectroscopy of the protein amide I band can be pe

264 The 2D CNN classified all reconstructed ACLs correctly.

265 The 2D heterointerface offers opportunities for new design o

266 The 2D layers of the materials with a composition close to T

267 The 2D-GMs are formed at low onset potential and can be in s

268 of physics and material sciences beyond the 2D photonic platform: equivalent mapping occurs for 3D t

269 ues were observed than that indicated by the 2D-MSI data, suggesting that quantitative analysis of mo

270 a study of 464 participants, we compared the 2D:4D of transgender individuals with age- and sex-match

271 sity and intrinsic redox character endow the 2D Cu-THQ MOF with promising electrochemical activity.

272 onducted on small samples) that examined the 2D:4D and the testosterone response to a challenging sit

273 ence of bifunctional oxygen vacancies in the 2D black In(2) O(3-) (x) nanosheets host, which enhances

274 intermediate edge structures involved in the 2D ice growth, which could reveal the underlying growth

275 We describe results in three models: the 2D Ising ferromagnetic model, the 3D Vicsek flocking mod

276 actor range can still enter the cages of the 2D halide perovskites by stretching them.

277 demonstrates long-term immunogenicity of the 2D HPV vaccine schedule.

278 wavefunction and the holon excitation of the 2D Hubbard model can be revealed in unprecedented detail

279 nsor devices when the active channels of the 2D material are suspended and nanoscaled.

280 a recrystallization and reorientation of the 2D perovskite slabs occurs to form an ideal structure wi

281 evidence in a discussion on the links of the 2D:4D and the testosterone change.

282 We also propose that the 2D to 3D growth transition in P. patens is underpinned b

283 e combination of these experiments using the 2D-LC-CRMS strategy enables the sensitive characterizati

284 Via the 2D-CNN framework, the transfer learning of Mobile Net sh

285 r accumulation of Abeta42 peptide, but these 2D models do not recapitulate the three-dimensional (3D)

286 The 3D self-assembly of these 2D sandwich structures further reinforces the interconne

287 We tested these 2D catalysts using a model reaction that assesses extern

288 ion of non-van der Waals (non-vdW) solids to 2D vdW transition-metal chalcogenide layers with identif

289 t common Non-Cartesian readout trajectories (2D/3D radials and spirals), demonstrating efficient anti

290 irst-principle calculations based on typical 2D N-doped carbon/RuMo nanoalloys heterostructures demon

291 Using 2D and 3D imaging and image segmentation, we characteriz

292 Using 2D seismic lines and bathymetric data, we map tectonic f

293 And, using 2D invasion assays, we show that the inhibition of ESRPs

294 ess to cortical vasculature and imaged using 2D-optical imaging spectroscopy (2D-OIS).

295 by scientists is predominantly performed via 2D static images, since the embedding of interactive 3D

296 gration of tumor cells in different in vitro 2D and 3D co-cultures.

297 ch as spin dependent density of states) when 2D materials are used as ultimately thin interfaces.

298 One key challenge with 2D semiconductors is to avoid the formation of charge sc

299 ring was overcome by trapping particles with 2D optical tweezers.

300 nd interaction of electromagnetic waves with 2D materials.