ライフサイエンスコーパス: dimensional

1 One-dimensional (1D) and two-dimensional (2D) NMR studies re

2 d be identified for several nucleotides by 1-dimensional (1D) imino (1)H NMR as well as by 2D HyperW

3 One-dimensional (1D) nanoobjects have strongly anisotropic p

4 ifferent lengths and charges, within the one-dimensional (1D) nanoscale pores of surfactant-templated

5 We combine one-dimensional (1D) nanowires (NWs) and 2D graphene flakes

6 such as the quantum spin Hall effect in one-dimensional (1D) topological edge states, where quasipar

7 oscopy, the cis/trans isomerization in a two-dimensional (2-D) array of surface-mounted azobenzene-ba

8 tectures, from protein cages to extended two-dimensional (2D) and three-dimensional (3D) crystalline

9 aining single cells are immobilized in a two-dimensional (2D) array, with osmotically induced changes

10 hree-dimensional (3D) and the other with two-dimensional (2D) convolutional kernels.

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

12 the first implementation of an array of two-dimensional (2D) layered conductive metal-organic framew

13 reaction and determined that the compact two-dimensional (2D) LiInP(2)Se(6) detectors resolved the fu

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

15 One-dimensional (1D) and two-dimensional (2D) NMR studies revealed that in fused sapp

16 By combining Raman spectroscopy with two-dimensional (2D) perturbation correlation moving window

17 structure of scenes from information in two-dimensional (2D) retinal images.

18 Two-dimensional (2D) ternary materials recently generated in

19 port is observable in the edge currents of 2-dimensional (2D) topological band insulators with broken

20 b-diffraction (SPEED) microscopy and its two-dimensional (2D)-to-3D transformation algorithm to provi

21 By utilizing three-dimensional (3-D) human airway tissues to examine viral

22 key aspects of the viral life cycle in three-dimensional (3-D) human airway tissues.

23 ities to chemistry parameters during a three-dimensional (3-D) simulation.

24 lved use of two types of CNN, one with three-dimensional (3D) and the other with two-dimensional (2D)

25 hese 2D models do not recapitulate the three-dimensional (3D) architecture of brain tissue.We employe

26 of such multicellular tractions within three-dimensional (3D) biomaterials could elucidate collective

27 important role in the nascent field of three-dimensional (3D) bioprinting.

28 Dispersing RGO on three-dimensional (3D) carbon paper electrodes is one strategy

29 e, we developed an inducible system of three-dimensional (3D) collective invasion to study the behavi

30 s to extended two-dimensional (2D) and three-dimensional (3D) crystalline arrays.

31 The results suggest that a three-dimensional (3D) crystallographic registry within cage-l

32 Three-dimensional (3D) culture systems have fueled hopes to br

33 oning human MSCs (hMSCs) for 96 h on a three-dimensional (3D) ECM-based microgel platform.

34 likely facilitated by the evolution of three-dimensional (3D) growth, enabled the generation of morph

35 ovskites and their demonstration in 2D/three-dimensional (3D) hierarchical film structures broke new

36 Three-dimensional (3D) hydrogel printing enables production of

37 This prospective study implemented 3-dimensional (3D) isotropic contrast-enhanced T2 fluid-at

38 elial cells (EEC) grown as monolayers or a 3-dimensional (3D) model.

39 orm a porous g-C(3)N(4) interconnected three dimensional (3D) network of g-C(3)N(4) and GNF.

40 ight-emitting diodes (PeLEDs) based on three-dimensional (3D) polycrystalline perovskites suffer from

41 Their three-dimensional (3D) position can be resolved by holographic

42 We investigated differences in the 3-dimensional (3D) pressure profile of the LES and hiatal

43 Three-dimensional (3D) printed prostate cancer models are an e

44 Three-dimensional (3D) representations of the environment are

45 Three-dimensional (3D) shape perception is one of the most imp

46 ows rapid, nontoxic measurement of the three-dimensional (3D) spatial distribution of viscoelastic pr

47 Atomic-level three-dimensional (3D) structure data for biological macromole

48 d the collar regions while maintaining the 3-dimensional (3D) structure in the murine PDL.

49 Visual systems estimate the three-dimensional (3D) structure of scenes from information in

50 have been recently made to obtain the three-dimensional (3D) structure of the genome with the goal o

51 ular dynamics simulations to determine three-dimensional (3D) structures of activated beta-arrestin2

52 building blocks to realize deployable three-dimensional (3D) structures of arbitrary shape.

53 scopy (cryo-EM), we resolved the first three-dimensional (3D) structures of K63 ubiquitinated ribosom

54 (DSCs) were compared with those from a three-dimensional (3D) U-Net and a coarse-to-fine deep learnin

55 A generic three-dimensional (3D) U-Net was trained on four different dat

56 We measured in situ two-dimensional affinity on individual live T cells from thy

57 ion damage) and subtomogram averaging (three-dimensional alignment of macromolecules in a complex sam

58 Zeolites are three-dimensional aluminosilicates having unique properties fr

59 A novel three-dimensional analysis algorithm is then applied to object

60 sis on algorithms' ability to capture hybrid dimensional and categorical models of ASD, and 4) system

61 hm, we observe that there is typically a low-dimensional and easily modeled representation of the rel

62 based on their spontaneous migration in two-dimensional and three-dimensional microenvironments, res

63 n in ASD suggests that there is a need for a dimensional approach.

64 ion performance comparable to existing three-dimensional approaches was achieved when labeling verteb

65 demonstrates a facile approach to employ two-dimensional aromatic compounds as modular building block

66 mplementary strands into micrometer-long one-dimensional arrays.

67 development and assessment using simple, low-dimensional artificial stimuli.

68 hallenging synthetic targets because a three-dimensional assembly is necessary for their formation.

69 ry topologies, (b) RAG Builder: builds three-dimensional atomic models from candidate graphs generate

70 he analysis of top-ranked predictors in high-dimensional bioinformatics datasets, in order to avoid t

71 techniques are widely used to interpret high-dimensional biological data.

72 E can perform complex analysis on real three-dimensional biological samples that would otherwise be i

73 tively before gestational week 12, and three-dimensional breast volume assessments were performed.

74 r structures, including a finite-sized three-dimensional cage.

75 ristics combining nanoscale diameters of one-dimensional carbon nanotube and lateral infinity of two-

76 mples using an additively manufactured three-dimensional cartridge and a smartphone-based reader.

77 The present study aimed to assess the three-dimensional changes following soft tissue augmentation u

78 are to report clinical and volumetric three-dimensional changes in mucosal thickness (MT) 1 year aft

79 oscopicity, which limits the risk of further dimensional changes of wood exposed to a variable air mo

80 Their porosity consists of a one-dimensional channel connected to three peripheral pocket

81 sired quadratic Weyl points by using a three-dimensional chiral metacrystal of sound waves.

82 practical feature selection method for high-dimensional class-imbalanced data, which is simple and c

83 ultitask approaches to regularizing the high-dimensional classification task with a larger regression

84 Using biplots to visualize the data in 2-dimensional clusters, glaucoma suspect patients demonstr

85 Using bottom-up or top-down strategies, bi-dimensional COFs can be obtained as single- or few-layer

86 rpose of this study was to examine the three-dimensional collagen architecture of wounded embryonic c

87 , we report that tumor cells embedded in a 3-dimensional collagen gel, however, are killed by cryopre

88 defined 2-dimensional confinement and in a 3-dimensional collagen matrix through recording their long

89 Two-dimensional colloidal crystals of submicrometer microsph

90 igin of seed experiments; (4) exploit a high-dimensional, complex parameter space, and (5) achieve th

91 blocks to generate richly substituted, three-dimensional compounds.

92 c aortic valves have been documented by four-dimensional computed tomography (CT).

93 The three-dimensional configuration of dissolved organic matter (D

94 endritic cell migration under well-defined 2-dimensional confinement and in a 3-dimensional collagen

95 The three-dimensional conformation of a genome can be profiled usi

96 ngshot spiders, theridiosomatids build three-dimensional conical webs with a tension line directly at

97 Three-dimensional convolutional neural networks were trained t

98 ical phases and host symmetry protected zero-dimensional corner states.

99 y (IMC)), have been developed from their low-dimensional counterparts, flow cytometry and immunohisto

100 Ds are consistently recapitulated in a three-dimensional culture AD model, virus-infected APP/PS1 mic

101 Engineered ureteric buds branched in three-dimensional culture and expressed Hoxb7, a transcription

102 Cortical organoids are self-organizing three-dimensional cultures that model features of the developi

103 ds with cerebral cortical organoids in three-dimensional cultures to form cortico-striatal assembloid

104 ement of finger groups and in an offline two-dimensional cursor-control task, the SBP performed equal

105 It is well suited for high-dimensional data with small sample sizes like RNA-seq da

106 ts in complicated modeling scenarios in high-dimensional data, such as GWAS, gene expression, eQTL an

107 Structure of the multi-dimensional dataset was explored using principal compone

108 erstanding and visualizing these large multi-dimensional datasets during acquisition and pre-processi

109 on, feature extraction, and analysis of high-dimensional datasets.

110 ine learning and dimension reduction of high-dimensional datasets.

111 rimates, in an online task involving the one-dimensional decoding of the movement of finger groups an

112 involve time-intensive experiments and multi-dimensional design spaces.

113 Previous efforts to form two-dimensional dilute magnetic semiconductors utilized extr

114 on-native interaction interface on the three-dimensional dimeric structure of the N-terminal domain o

115 To this end we combined categorical and dimensional disorder models with a fully data-driven int

116 ccessible method for calculating fully three-dimensional displacement and 3D surface tractions at hig

117 Mediation analysis with high-dimensional DNA methylation markers is important in iden

118 pplied in the assembly of highly ordered two-dimensional droplet networks.

119 n condensation phase transitions, into three-dimensional droplets or in two-dimensional lattices on m

120 out for WM-guided behaviour, whereas the low-dimensional dynamic component could provide additional t

121 otentials are applied via two parallel three-dimensional electrodes, which interface the nanodroplets

122 ographic reconstruction then yield the three-dimensional electron density distribution with a voxel s

123 A two-dimensional electron gas in a magnetic field is a model

124 However, unlike semiconductors and two-dimensional electron gases where the charge degree of fr

125 ing electrons in an exceptionally clean, two-dimensional electron system confined to a modulation-dop

126 Here, using ultrafast two-dimensional electronic spectroscopy (2DES), we reveal th

127 Here, we employ polarization-dependent two-dimensional electronic-vibrational spectroscopy to study

128 e human situation, compared to classical two-dimensional endothelial cell cultures.

129 When confined within three-dimensional environments, they use the topographical fea

130 ximity FRET effect occurring in confined two-dimensional environments.

131 The current study uses fMRI and Multi-Dimensional Experience Sampling (MDES) to chart how cogn

132 Analysis of these sparse, high-dimensional experimental results requires dimension redu

133 cterization of B cell responses through high-dimensional flow cytometry to reveal substantial heterog

134 cellular membranes and, more generally, two-dimensional fluids on curved substrates.

135 ty of interlayer and intralayer space of two-dimensional fluorinated MOFs for capturing acetylene fro

136 gorithm" was developed for comprehensive two-dimensional gas chromatography coupled with time-of-flig

137 ale data, we generated graphs encoding the 3-dimensional geometry of the left ventricle.

138 carbon nanotube and lateral infinity of two-dimensional graphene.

139 The one-dimensional helical structures presented in this study a

140 ntum phenomena in electronically coupled two-dimensional heterostructures are central to next-generat

141 ional random projections and "classical" low-dimensional hexagonal grid cell responses.

142 three embedded spirals for the case of a two-dimensional hexagonal lattice.

143 zation from coarse-grained output of a three-dimensional high-resolution idealized atmospheric model.

144 Here, we used three-dimensional high-resolution imaging to investigate the f

145 Here, we create a three-dimensional hot electron gas through two-photon photoemi

146 Two-dimensional hybrid organic-inorganic perovskites with st

147 Finally automated robotized screening of low-dimensional hybrid perovskite materials through the scre

148 eously, but also constructs additional three-dimensional hyperchannels for electrical and thermal con

149 e a concise feature map in the form of a two-dimensional image by minimizing the pairwise distance va

150 notes and independent graders reviewing two-dimensional images and anatomic landmarks.

151 try (also known as CyTOF) and analogous high-dimensional imaging approaches (including multiplexed io

152 OCT offering 3-dimensional imaging of the retina is widely used to guid

153 ll as different imaging modalities for three-dimensional imaging.

154 Ultrafast two-dimensional infrared (2D-IR) spectra can now be obtained

155 curve resolution analyses of the one and two-dimensional infrared spectroscopy data show that the int

156 s can be monitored with conventional and two-dimensional infrared spectroscopy, vibrational circular

157 Our model constructs representations of high-dimensional inputs through a combination of low-dimensio

158 y judgements can be captured by a fairly low-dimensional, interpretable embedding that generalizes to

159 perceptual-decision-making, we extracted low-dimensional latent factors that captured the population-

160 is first compressed and integrated in a low-dimensional latent space that encodes the given data in

161 Displacement of the protective 2-dimensional lattice formed by annexin V on trophoblast s

162 s, into three-dimensional droplets or in two-dimensional lattices on membrane surfaces, have emerged

163 Here, we incorporate rather thick two-dimensional layered semiconducting crystals for reliable

164 Fullerene-based low-dimensional (LD) heterostructures have emerged as excell

165 methodology that creates an in silico three-dimensional library of composite peptidic macrocycles.

166 S) is a unique class of materials with a one dimensional line node accompanied by a nearly dispersion

167 vity for oxo-site bonding, leading to higher dimensional linking.

168 In this study, an achiral-chiral two-dimensional liquid chromatographic method for the enanti

169 resent a 27-plex TMT method coupled with two-dimensional liquid chromatography (LC/LC) for extensive

170 veloped a generic reagent, ultratargeted two-dimensional liquid chromatography-tandem mass spectromet

171 when analyzing single-molecule images for 3-dimensional localization microscopy or single-molecule t

172 o determine the diagnostic accuracy of three-dimensional magnetic resonance elastography (3D-MRE), wi

173 Noncollinear spin textures in low-dimensional magnetic systems have been studied for decad

174 500 MHz magnetic field of the complex three-dimensional magnetization in a two-phase bulk magnet wit

175 In two-dimensional magnets these effects manifest themselves in

176 computations as dynamics over relatively low-dimensional manifolds formed by correlated patterns of n

177 ecialized analysis software to produce three-dimensional maps for the epithelium of intact mouse lens

178 Two-dimensional materials from layered van der Waals (vdW) c

179 nides (TMDs) are one of the most studied two-dimensional materials in the last 5-10 years due to thei

180 e potential to enable the preparation of low-dimensional materials with prescribed morphologies and t

181 n has been a key to provide high-quality two-dimensional materials, but despite improvements it is st

182 m quasi-atomic interstitial electrons in low-dimensional materials.

183 ory of glasses predicts that in the infinite dimensional mean field limit, there exist two distinct g

184 Graft dimensional measurements were taken at time of surgery,

185 One-dimensional measures of adherence may ignore clinically

186 developments of mediation analysis with high-dimensional mediators.

187 Two-dimensional metal halide perovskites of Ruddlesden-Poppe

188 To assess the ability of the three-dimensional method for quantification purposes, matrix e

189 neous migration in two-dimensional and three-dimensional microenvironments, respectively.

190 profiles can be readily detected from three-dimensional microvessels-on-a-chip and display a more dy

191 was achieved when labeling vertebrae on two-dimensional MIPs.

192 ploying a computational approach using a one-dimensional model of the human vascular network.

193 Surprisingly for a one-dimensional model, this phase and its response to Dzyalo

194 Using 3-dimensional molecular modeling and mutational analyses,

195 Using three-dimensional morphological data from 158 species represen

196 Three-dimensional morphological parameters in 409 patients wit

197 The detailed, three dimensional morphology of the granules in conjunction wi

198 Analysis of the two-dimensional motion of cells between two rectangles with

199 that identifies modular components of three-dimensional mouse body language called 'syllables'.

200 Using this approach, the conventional three dimensional MR scalar images are replaced with spatially

201 increase in the conversion relative to three-dimensional MWW (MCM-22) and 2D layers prepared from pos

202 function for aluminosilicate zeolite MFI two-dimensional nanosheets before and after superheated stea

203 plementary brushes to form well-defined, one-dimensional nanostructures.

204 ive matrix to electronically connect a three-dimensional network of Shewanella oneidensis MR-1 to a g

205 The nanofibres assembled into a three-dimensional network with a high specific surface area, w

206 HENOM (Psychosis Heterogeneity Evaluated via Dimensional Neuroimaging) consortium.

207 beta-strand organization using multiple two-dimensional NMR and (13)C-(13)C dipolar recoupling exper

208 uld take up to a month, as it includes multi-dimensional NMR experiments that require prolonged exper

209 d their structures elucidated by one and two-dimensional nuclear magnetic resonance spectroscopy (1D

210 This procedure reduces the two-dimensional numerical search for the maximum of the like

211 A high-resolution, three-dimensional, optical imaging technique for the murine br

212 t competing energy scales present in the low-dimensional orbital-selective Mott phase (OSMP) induce a

213 recombination, are orchestrated by the three-dimensional organization of chromosomes at multiple leve

214 The three-dimensional organization of the genome supports regulate

215 A three-dimensional organoid assay in colonic crypts isolated fr

216 or the integration of heterogeneous and high-dimensional (p>>n) data, such as OMICS.

217 T derivatives yielded a highly unusual three-dimensional packing of the conjugated backbone, which is

218 state of knowledge on the creation of three-dimensional pancreatic islet structures in both microsca

219 ce the challenge of exploring large and high-dimensional parameter spaces in search of new scientific

220 t formation are obtained as functions of non-dimensional parameters, which agree well with experiment

221 An ensemble of three-dimensional patch-based, multiresolution pathway CNNs wa

222 main III (ED3)-targeting aptamers into a two-dimensional pattern precisely matching the spatial arran

223 25 nm by the coexistence of multiple reduced-dimensional perovskite domains, and the spectral stabili

224 tion highlights the unique attributes of two-dimensional perovskites as an exciting class of optoelec

225 e used to conduct genetic studies using high-dimensional phenotypes that are often collected in human

226 tly, this concept has been translated to two-dimensional photonic scenarios in connection with host m

227 nonimaging segment counting method (SC) or 2-dimensional planar lung perfusion scintigraphy (PS).

228 theory to understand the evolution of multi-dimensional plasticity.

229 (subjective) gating of subpopulations on two-dimensional plots.

230 odically ordered yet extended two- and three-dimensional polymers to create topologically well-define

231 versus choice-correlated activity in the low-dimensional population code.

232 fraction of the stimulus information in high-dimensional population recordings.

233 We approximately solve high-dimensional problems by combining Lagrangian and Euleria

234 oportional hazards models, adjusted for high-dimensional propensity scores, to generate adjusted haza

235 depolarization allowed us to construct a two-dimensional proximity correlation map that defines the s

236 Dimensional psychopathology in the parents was also corr

237 ion, but is attained exclusively by infinite-dimensional quantum systems (such as infinite-level syst

238 ensional inputs through a combination of low-dimensional random projections and "classical" low-dimen

239 Here, we present three-dimensional reconstructions of Namapoikia that we use to

240 By using three-dimensional reconstructions of serial-section transmissi

241 take segmentation algorithm identified all 3-dimensional regions of interest (ROIs) with increased tr

242 We also find that in the high-dimensional representational spaces these methods genera

243 were analyzed using steady and unsteady two-dimensional Reynolds-Averaged Navier Stokes, leading to

244 upling and energy level matching between two-dimensional Ruddlesden-Popper perovskite and graphene, w

245 ion coefficient and the allele age, to a one-dimensional search over the selection coefficient only.

246 in artificial membranes and demonstrate two-dimensional self-assembled heterostructures of graphene

247 Despite recent developments in two-dimensional self-assembly, most supramolecular 2D materi

248 (ICF) as a test-bed problem, we model a one-dimensional semianalytic numerical simulator and demonst

249 As promising channel materials, two-dimensional semiconductors show excellent capabilities o

250 states have been predicted to occur in three-dimensional semimetals, a corresponding Hall response ha

251 Our fully three-dimensional simulations highlight the crucial role of ac

252 Recent high-dimensional single-cell technologies such as mass cytome

253 tware package designed to render large three-dimensional single-molecule localization microscopy data

254 bstructures, which we identify here by three-dimensional single-molecule superresolution imaging.

255 ng a sample elemental composition in a three-dimensional space from nano- to submilliscale with high

256 still limited to simplified problems in two dimensional space or straight motions.

257 propose that hand control occupies a higher dimensional space than previously considered.

258 e theory of these domains is unified in four-dimensional space.

259 te outcomes and their standard errors in a 2-dimensional space.

260 We also simulated a two-dimensional spatial version of this model across a circa

261 e spectroscopy as well as conventional and 2-dimensional speckle-tracking echocardiography.

262 The three-dimensional STAIR-UTE sequence effectively suppressed wa

263 Two-dimensional STED has been extensively used to elucidate

264 re natural settings, involving complex, high-dimensional stimuli.

265 velopment has little influence on global two-dimensional stomatal patterning.

266 the brain to cope with the continuous, high-dimensional stream of sensory information it receives.

267 at human BEX3 (hBEX3) has well-defined three-dimensional structure in the presence of small fragments

268 hot topic, including the shaping of its two-dimensional structure into nanoribbons or nanobelts.

269 The low-dimensional structure of a model is easier to interpret

270 With the unique three-dimensional structure of laser-induced graphene based el

271 episome is known to interact with the three-dimensional structure of the human genome in infected ce

272 e the t(11;14)(q13;32), which modifies the 3-dimensional structure of the involved regions.

273 single-particle cryo-EM to analyze the three-dimensional structure of the mature ASFV particle.

274 hat N325 deamidation altered the local three-dimensional structure, which might interfere with the bi

275 ning faithful to empirical data on their low-dimensional structure.

276 n is greatly enhanced by insights from its 3-dimensional structure.

277 ograms, documented haploinsufficiency, three-dimensional structure/function analyses, cell biology ex

278 necessary to determine the ensemble of three-dimensional structures associated to the experimental da

279 ushed far out of equilibrium by a simple low-dimensional suppressive drive might ameliorate inference

280 e accompanied by a nearly dispersionless two-dimensional surface state.

281 Cell crawling on two-dimensional surfaces is a relatively well-understood phe

282 them comparing the living and non-living two-dimensional systems self-organizing at the spherical sur

283 mity screening of many-body phenomena in two-dimensional systems.

284 thods This prospective study evaluated three-dimensional T1-weighted spinal cord MRI scans in seropos

285 eriments can be performed, including the two-dimensional tandem mass scan (2D MS/MS scan) in which al

286 offers a practical, all-optical, fully three-dimensional tomography of electronic structure even in m

287 logical pumps are able to reduce this higher-dimensional topological insulator phenomena to lower dim

288 ary states, which themselves represent lower-dimensional topological phases and host symmetry protect

289 gs open a path towards exploration of higher-dimensional topological physics with time as a synthetic

290 While p-n homojunctions in two-dimensional transition metal dichalcogenide materials ha

291 Here we obtain the phase diagram of the two-dimensional triangular-lattice Hubbard model by studying

292 ow, by direct numerical simulations of three-dimensional turbulent Rayleigh-Benard convection flows i

293 the clinical feasibility of pulmonary three-dimensional ultrashort echo time (UTE) MRI at breath hol

294 g-range intrinsic magnetic orders in the two-dimensional van der Waals materials provide a new platfo

295 he coronary artery calcification score and 2-dimensional vascular ultrasound.

296 This general synthesis of diverse two-dimensional vdWH arrays provides a versatile material pl

297 ion-robust reconstruction framework for four-dimensional visualization and quantification of blood fl

298 oil ganglia distribution analysis, and three-dimensional visualization of fluid occupancy maps in por

299 eps involved in tissue preparation for three-dimensional volumetric imaging and provide a brief overv

300 e the data are often over-dispersed and high-dimensional, we formulate a well-posed hypothesis from a