ライフサイエンスコーパス: 2D

1 2D immunoblots were made in parallel to elucidate IgE an

2 2D IR chemical exchange spectroscopy further shows these

3 2D materials possess many interesting properties, and ha

4 2D MRE can estimate hepatic stiffness in children with N

5 2D nanocarbon-based materials with controllable pore str

6 2D nanoscale cloth will provide access to a new generati

7 2D phase-field simulation verifies the effect of strain.

8 2D total correlation spectroscopy (TOCSY) provides uniqu

9 2D transition-metal carbides and nitrides, known as MXen

10 Having already the data acquired (1D/2D NMR and RDCs), the procedure begins with the determin

11 ; typical large needle-like arrays having 20 2D layers units correspond to a model consisting of smoo

12 The coronal 21%-22% 2D RL and the 26%-28% 3D RSA bone loss apical to the cem

13 owever, corresponding to a 75%, 50%, and 25% 2D BSH reserve, premolars retained 67-68%, 39-41%, and 1

14 The coronal 30%-31% 2D RL and the 41%-42% 3D RSA bone loss corresponded to a

15 passes through the minimum that marks the 3D-2D crossover in the system.

16 dule in terms of seroconversion rates and 3D/2D geometric mean titers for anti-HPV-16 and anti-HPV-18

17 al phonons whose fast escape leaves behind a 2D-projected mass density increase endowing the flexural

18 hich the adherence junctions of cells form a 2D manifold that is fluorescently labeled.

19 rvation of these topological edge modes in a 2D photonic lattice, where these propagating edge states

20 arch for nonregenerating sparse targets in a 2D space with steps drawn from a Levy distribution with

21 ect pyrene knots at regular intervals into a 2D lattice with pi conjugations extended along both x an

22 Graphene is a 2D material that has been extensively used in the develo

23 many claim that the photonic properties of a 2D layer provide evidence that the material is "high qua

24 stal-to-single-crystal (scsc) synthesis of a 2D polymer based on photochemically triggered [2 + 2]-cy

25 he third ever case for a scsc synthesis of a 2D polymer.

26 rmation can be represented as a pathway on a 2D phase plane.

27 We find that a 2D bridging network is energetically favored over a 3D n

28 re, we adapt this raster/vector concept to a 2D colloidal system and realize 'vector assembly' by man

29 In this work, a 2D MS method is developed to characterize complex mixtur

30 that we hope will inspire new users to adopt 2D-LC for their analytical problems.

31 port that MoS2 films with vertically-aligned 2D layers exhibit excellent visible light responsive pho

32 ovel idea with implications in designing all 2D device architecture as the structural phases in 2D ma

33 ented of how significant improvements in all-2D photodetectors can be achieved by exploiting the type

34 initially determined via analysis of 1D and 2D NMR spectroscopic data and the assignment was confirm

35 To facilitate characterization via 1D and 2D NMR, we synthesized (13)C-enriched FEC, ultimately al

36 for all investigated loci using both 3D and 2D approaches in multiple subjects.

37 We used 3D and 2D motion analysis to quantify the probing behavior of t

38 sional (2D) gradient-recalled echo (GRE) and 2D spin-echo (SE) echo-planar imaging (EPI) magnetic res

39 t can be studied simultaneously by FT-IR and 2D IR correlation spectroscopies.

40 strumentation (like UV-vis, FTIR, Raman, and 2D NMR benchtop spectrometers), is shown to provide a de

41 rdness tester (final SMH), and roughness and 2D profiles using atomic force microscopy were measured

42 Fs in the one-dimensional (1D) nano-wire and 2D system, and enrich the theoretical research on findin

43 on and growth dynamics of highly anisotropic 2D lateral heterojunctions between pseudo-1D ReS2 and is

44 This makes it possible to apply 2D NMR spectral fingerprinting approaches directly to dr

45 moved along linear, circular, and arbitrary 2D trajectories.

46 up new avenues for the design of artificial 2D materials.

47 restricted by the applied approaches such as 2D conventional soft lithography methods that have recta

48 r, many oxides are not easy to synthesize as 2D materials through conventional methods.

49 were designed and 3D printed in titanium as 2D serpentine, 3D spiral, and 3D serpentine columns, of

50 atients with 2,602 morphologic images (axial 2D T2-weighted imaging) of the prostate were obtained.

51 w compelling evidence that the silicon based 2D overlayer is responsible for the observed linear disp

52 present some of the basic principles behind 2D IR and show how they have, and can, impact the field

53 ac and Weyl fermions can be realized in both 2D and 3D materials.

54 o-target binding predictions inaccessible by 2D fingerprints and confirm three of them experimentally

55 vie provide insight into future solar cells, 2D materials and other semiconductor devices.

56 The characteristic 2D IR features of amyloid beta-sheet secondary structure

57 ultiple achiral x chiral and chiral x chiral 2D-LC examples (single and multiple heart-cutting, high-

58 nline two-dimensional liquid chromatography (2D-LC) method where the first dimension column is eluted

59 rrays at the atomic scale for the S-Mo-S(Co) 2D- layers that conform the spherically shaped catalyst

60 T growth speeds in ECs cultured on compliant 2D ECMs but promotes slow MT growth speeds in ECs cultur

61 Under identical such conditions, 2D-nanosheets of boehmite (gamma-AlOOH) exfoliated from

62 the integration of exceptionally continuous 2D channels and nacre-inspired brick-and-mortar architec

63 l-based reaction route can be used to create 2D materials that were previously inaccessible with pree

64 s on in vitro alphaB- and gammaD-crystallin, 2D IR spectroscopy can identify the highly ordered beta-

65 Current 2D bioelectronics research is focused on the design of s

66 Currently 2D COF syntheses are developed empirically, and most mat

67 plitting of Ln ions by the highly designable 2D material crystal field provides a new method to exten

68 imensional transition metal dichalcogenides (2D TMDs) have gained great interest due to their unique

69 parameters and one (1D) and two dimensional (2D) (1)H Nuclear Magnetic Resonance (NMR) relaxometry.

70 r lattices, we can generate two dimensional (2D) phases, which are characterized by the Berry phase o

71 form and colloidally stable two-dimensional (2D) assemblies by bottom-up methods represents a challen

72 res, and superlattices from two-dimensional (2D) atomic crystals.

73 Recently discovered two-dimensional (2D) boron polymorphs, collectively tagged borophene, are

74 ase are mainly based on the two-dimensional (2D) cell culture and are limited by the difficulty of si

75 inefficient packing of the two-dimensional (2D) chains of PIM-TMN-Trip generates a high concentratio

76 root surface area (RSA) and two-dimensional (2D) crown-to-root ratio (CRR) of extracted teeth to clas

77 We synthesized a two-dimensional (2D) crystalline covalent organic framework (sp(2)c-COF)

78 asic theoretical aspects of two-dimensional (2D) crystals.

79 tain exact solutions to the two-dimensional (2D) Dirac equation for the one-dimensional Poschl-Teller

80 ystals are next modified to two-dimensional (2D) elastic crystals, of the type 4-bromophenyl 4'-nitro

81 trometry which is solved by two-dimensional (2D) Fourier transform ion cyclotron resonance mass spect

82 Purpose To compare two-dimensional (2D) gradient-recalled echo (GRE) and 2D spin-echo (SE) e

83 Two-dimensional (2D) graphene and graphene oxide (GO) offer great potenti

84 Two-dimensional (2D) hybrid halide perovskites come as a family (B)2(A)n-

85 We accomplish this using two-dimensional (2D) layered hybrid trihalide perovskites that are deposi

86 Only a selected group of two-dimensional (2D) lead-halide perovskites shows a peculiar broad-band

87 ast tomosynthesis (DBT) and two-dimensional (2D) mammography varies with number of years of experienc

88 arable electronics based on two-dimensional (2D) material heterojunction structures also known as het

89 imple criterion to identify two-dimensional (2D) materials based on the comparison between experiment

90 tion of a growing number of two-dimensional (2D) materials has inspired worldwide efforts to integrat

91 Two-dimensional (2D) materials offer a promising platform for exploring c

92 rapid growth of interest in two-dimensional (2D) materials.

93 n ecosystems have relied on two-dimensional (2D) measures of greenspace structure to calculate connec

94 MXenes, two-dimensional (2D) metal carbides and nitrides, have attracted attentio

95 has held great promise as a two-dimensional (2D) metal with massless carriers and, thus, extremely hi

96 s by integrating conductive two-dimensional (2D) metal-organic frameworks (MOFs) into fabrics through

97 Electronic properties of two-dimensional (2D) MoS2 semiconductors can be modulated by introducing

98 s and multifunctionalities, two-dimensional (2D) nanomaterials have aroused increasing interest in th

99 Two-dimensional (2D) oxides have a wide variety of applications in electr

100 and use it to prepare novel two-dimensional (2D) pi-conjugated COFs, as crystalline powders and exfol

101 caveolin-1 projected onto a two-dimensional (2D) plane.

102 Two-dimensional (2D) Ruddlesden-Popper perovskites are solution-processed

103 r synthesizing high-quality two-dimensional (2D) semiconductors is essential for their practical appl

104 Two-dimensional (2D) separations are able to generate significantly highe

105 ich is capable of obtaining two-dimensional (2D) spectra from three spatial dimensions.

106 s of graphene stem from its two-dimensional (2D) structure, with a linear dispersion of the electroni

107 investigate the MTZFs in a two-dimensional (2D) system as compared to MFs in the one-dimensional (1D

108 ol is crucial for tailoring two-dimensional (2D) zeolites (crystallites with thickness less than two

109 e range of distribution on a two-dimensional(2D) plot upon structural root-mean-square deviations(RMS

110 used for integration of any fluid-dispersed 2D nano-objects on silicon-on-insulator photonics platfo

111 ired worldwide efforts to integrate distinct 2D materials into van der Waals (vdW) heterostructures.

112 heterochiral rather than homochiral domains (2D crystals or clusters) is not known.

113 The N-doped 2D GO is also impermeable to small molecules, and hence

114 stability, make PtSe2 a versatile electronic 2D layered material.

115 dimensional difference gel electrophoresis (2D-DIGE) and mass spectrometry (MS).

116 imensional-differential gel electrophoresis (2D-DIGE) to compare protein expression profiles of trans

117 th generated by the LC pumps (pulsed-elution 2D-LC).

118 dy suggests a high promise of these emerging 2D materials for water treatment, significantly broadeni

119 owth process allowed us to cool the existing 2D crystals to prevent undesired thermal degradation and

120 such as particles, 1D nanowires and fibres, 2D films and coated surfaces, and 3D patterned surfaces

121 nd of F-P sensor may open up new avenues for 2D materials in biomedical and environmental application

122 ductivity is the lowest observed to date for 2D materials, (0.55 +/- 0.07) W m(-1) K(-1) , resulting

123 ral chromatography as a second dimension for 2D chromatographic separations.

124 es will offer promise as design elements for 2D assemblies with face-selective functionalization.

125 single split-ring resonator (SRR) probe for 2D surface mapping and imaging of relative dielectric pe

126 two-dimensional covalent organic frameworks (2D COFs) are crystalline polymer networks with enhanced

127 es was not directly observed in freestanding 2D MoS2 before.

128 3D porous nanostructures built from 2D delta-MnO2 nanosheets are an environmentally friendly

129 es predict drug-to-target relationships from 2D small-molecule topology patterns.

130 pronounced differences in the 1D-IR (FTIR), 2D-IR, and vibrational circular dichroism spectra.

131 Integrating functionalized 2D materials into multilayer device architectures increa

132 ne), a partial agonist at GluN1/2B and GluN1/2D (10% and 27%, respectively), and a highly efficacious

133 HLA class II, and natural killer cell group 2D (NKG2D) ligand expression in the lesional keratinocyt

134 As a new member of the MXene group, 2D Mo2 C has attracted considerable interest due to its

135 in mice expressing the MHC class I allele H-2D(b).

136 analysis of a prototypical Vbeta8.1(+) TCR-H-2D(b)-GAP5040-48 ternary complex revealed that germline-

137 This study expands the scope of heterodyned 2D IR spectroscopy to tissues.

138 rue dissolution of a wide range of important 2D nanomaterials by forming layered material salts that

139 development, discuss the state of the art in 2D-LC performance as measured by peak capacity, and desc

140 One important type of defect in 2D layered materials is known as rotational stacking fau

141 Allergen detection in 2D-Western blots with PBS resulted in greater sensitivit

142 also highlight technological developments in 2D IR that continue to expand the scope of scientific pr

143 ary phases (CSPs) as the second dimension in 2D-LC, especially in the comprehensive mode.

144 Alloying/doping in 2D material is important due to wide range bandgap tunab

145 hey cause the Lindemann criterion to fail in 2D in the sense that the mean squared displacement of at

146 ar myocytes; a median separation of 20 nm in 2D electron microscopy and 3.3 nm in 3D electron tomogra

147 pair multiplication has not been observed in 2D TMD devices.

148 ice architecture as the structural phases in 2D materials such as transition metal dichalcogenides ar

149 The discovery of emergent phenomena in 2D materials has sparked substantial research efforts in

150 IIA filaments to leading edge protrusions in 2D, and this in turn blocks maturation of anterior focal

151 w nanoscale changes can induce reactivity in 2D materials, which can provide unique surface interacti

152 r cell motility and increased colony size in 2D cultures.

153 subsequent tasks are more rapidly solved in 2D.

154 plications for smooth electron waveguides in 2D Dirac-Weyl systems are discussed.

155 ndocrine-dependent cell line (MCF-7:WS8), in 2D and 3D cultures, using ERalpha in-cell westerns, ERE-

156 Here, two-dimensional infrared (2D IR) and IR polarization selective pump-probe (PSPP) s

157 Two-dimensional infrared (2D IR) and polarization selective IR pump-probe (PSPP) t

158 study, we collect two-dimensional infrared (2D IR) spectra on tissue slices of porcine eye lenses.

159 eflection enhanced two-dimensional infrared (2D IR) spectroscopy, on a carbonyl stretching mode of tr

160 We reveal the presence of intrinsic 2D Dirac plasmons in 3D nanoporous graphene disclosing s

161 ching the mosaic planes into a single, large 2D image and (iv) adjusting the contrast.

162 3)(CH3NH3)nPbnI3n+1 (n = 1, 2, 3) of layered 2D perovskites.

163 variety of inorganic compounds with layered (2D) structure is described.

164 ed LC2MS4 in a comprehensive LC1MS2 x LC1MS2 2D-LC separation.

165 nsors based on graphene and on graphene-like 2D materials for biomarkers detection.

166 thesis and characterization of graphene-like 2D materials, single and few-atom-thick layers of van de

167 Off-line 2D LC-MS/MS analysis (SCX-RPLC) of S. cerevisiae whole c

168 tion of a prototypical boronate-ester linked 2D COF known as COF-5 from its 2,3,6,7,10,11-hexahydroxy

169 py a narrow and unique space in the CCS-mass 2D spectrum, suggesting a tight structure-function relat

170 n of the spectral signatures of the measured 2D signals.

171 (CHD7(LOF)) and lysine (K) methyltransferase 2D (KMT2D(LOF)), respectively.

172 This antibody-mimetic 2D material holds great potential toward the blood-based

173 he feasibility for designing multifunctional 2D optoelectronic devices.

174 he 2D-Xene systems promising multifunctional 2D materials for nanotechnology.

175 Efforts have been devoted to exploring novel 2D and 3D auxetic structures through rational design, op

176 Until now 2D FTICR MS afforded only a moderate resolution for prec

177 rous areas, but the construction of objects, 2D and 3D crystalline lattices and devices is prominent

178 Quantitative analysis of 2D T1-T2 maps greatly facilitated the interpretation of

179 ethylsiloxane) substrates and a new class of 2D elastomeric substrates with controlled patterned rigi

180 ReS2 represents a different class of 2D materials, which is characterized by low symmetry hav

181 gh Young's modulus and surface conformity of 2D capping layers such as graphene and MoS2 substantiall

182 s, and opens the door to the construction of 2D hierarchical structures with broad utility.

183 or the control of liquid phase deposition of 2D materials.

184 ults will inform the rational development of 2D COF polymerizations by controlling the rate of nuclea

185 plications and technological developments of 2D vibrational surface spectroscopy.

186 g contributing to the synergistic effects of 2D morphology, amorphous structure, conductive substrate

187 Rational surface engineering of 2D nanoarchitectures-based electrode materials is crucia

188 demonstrate controlled strain engineering of 2D semiconductors during synthesis by utilizing the ther

189 dent semiconductor-to-semimetal evolution of 2D layered PtSe2 .

190 his work is a major advance for the field of 2D polymers synthesized at the air/water interface as it

191 ter splitting via in situ vertical growth of 2D amorphous FePO4 nanosheets on Ni foam (Am FePO4 /NF).

192 s leading to anisotropic epitaxial growth of 2D zeolites with rates as low as few nanometers per day.

193 new insight into the stability mechanism of 2D boron and open new ways for the control of the lattic

194 ous in-situ Raman spectroscopy monitoring of 2D dispersed flakes during the device operation.

195 ly influence the formation and morphology of 2D h-BN.

196 n 3D reconstruction from a limited number of 2D projections.

197 e 3D structure of an object from a number of 2D projections.

198 tween photonic and electronic performance of 2D semiconducting layers, and demonstrates that they are

199 omic defects present on the lattice plane of 2D MoS2 nanoassemblies are due to atomic vacancies and c

200 trate a method for probing the properties of 2D materials via nanometer-scale nuclear quadrupole reso

201 mapping studies showed that a wide range of 2D heterostructures (such as WS2-WSe2 and WS2-MoSe2), mu

202 generates chaotic fluid flow reminiscent of 2D turbulence.

203 the nearly instantaneous time-resolution of 2D IR spectroscopy, parallel and antiparallel helix asso

204 tructural variation among systematic sets of 2D NMR fingerprint spectra using the NISTmAb and illustr

205 sm of molecular adsorption on the surface of 2D materials, while introducing TPTEM as a novel and pow

206 ition of molecular adsorbates on surfaces of 2D materials is key to their development in applications

207 lybdenum disulfide (MoS2) and other types of 2D dichalcogenides.

208 Thus, use of 2D membrane based off surface matrix may present the new

209 The different variants of 2D vibrational spectroscopy are based on either the even

210 h number of years of experience or volume of 2D mammograms read.

211 1,25(OH)2D induced 324 differentially expressed genes, with 187

212 However, 1,25(OH)2D induced only 10 differentially spliced genes, with no

213 esign of more sophisticated devices based on 2D materials.Strain engineering is an essential tool for

214 3D photonic microstructure shaping based on 2D-fluid composites and CMOS photonics platform, while a

215 erformance is enabled by epitaxial growth on 2D boron nitride for chemical-free transfer to a soft, f

216 We here introduce an online 2D-LC-HCD-MS/MS platform for comprehensive glycated pept

217 This online 2D-LC-HCD-MS/MS platform has high enrichment efficiency

218 Here, we show that the optical 2D photon echo spectra of this complex at ambient temper

219 resonance mass spectrometry (2D FTICR MS or 2D MS) allows direct correlation between precursor and f

220 ars with alveolar bone loss based on 3D's or 2D's measurement is inconsistent.

221 of ReS2 are discussed relative to the other 2D materials.

222 hat Ti3 CN is metallic, in contrast to other 2D saturable absorber materials reported so far to be op

223 exfoliated from bulk crystals, a pentagonal 2D layered noble transition metal dichalcogenide with a

224 terostructures reveal about 0.1 electron per 2D unit cell transferred between the interfacial Mn and

225 y electrophoresis (CE) with muFFE to perform 2D CE x muFFE separations.

226 hway for the fabrication of high-performance 2D optoelectronic devices.

227 Peripapillary 2D RNFL thickness circle scans were also obtained.

228 gnostic capability compared to peripapillary 2D RNFL thickness measurements, although differences wer

229 ocarbon stacks is composed of well-preserved 2D sheets with highly accessible interlayer macropores,

230 Using the technique on a prototypical 2D system, a GaAs quantum well, we uncover signatures of

231 n electron microscopy, TEM) can only provide 2D simplifications of size and shape with a spatial reso

232 an be selectively crystallized into the pure 2D or 3D net using an anionic or neutral surfactant, res

233 and aqueous phases is confined under a quasi-2D geometry.

234 embly for the crafting of high aspect ratio, 2D sheets that are densely surface-decorated with DNA.

235 The resulting 2D fingerprints were interpreted by pattern recognition

236 Our data reveal 2D dynamics of the mitochondria, plasma membrane and fil

237 diology resident individually; each reviewed 2D and then 3D images, including color and spectral Dopp

238 ed to the more common Ruddlesden-Popper (RP) 2D perovskites, the ACI perovskites have a different sta

239 undefined components and difficult to scale 2D culture formats.

240 processing tasks above resulting in a single 2D image of the stained manifold across which contrast i

241 rmation at the microscopic scale in a single 2D light-field image.

242 stained manifold in each stack into a single 2D projection plane, (ii) correcting uneven illumination

243 m ion cyclotron resonance mass spectrometry (2D FTICR MS or 2D MS) allows direct correlation between

244 nt gene expression when compared to standard 2D cell cultures.

245 y by adding silicene, germanene and stanene (2D allotropes of Si, Ge, and Sn), lends itself as a plat

246 to generate a "brick-wall" motif with strong 2D interlayer electronic interactions.

247 aminations performed with DBT plus synthetic 2D imaging (38.5 screens per hour) than with FFDM (60 sc

248 Conclusion DBT plus synthetic 2D imaging increases CDRs with recall rates comparable t

249 assessment was higher for DBT plus synthetic 2D imaging than for FFDM (RR, 1.93; 95% CI: 1.31, 2.03).

250 in patients screened with DBT plus synthetic 2D imaging than in those screened with FFDM among women

251 l was almost doubled with DBT plus synthetic 2D imaging: 23.3% versus 12.9% of recalled patients who

252 15 through March 2016 for DBT plus synthetic 2D screening in the Verona screening program.

253 in these directions, which demonstrate that 2D microfluidics is uniquely set to study complex out-of

254 rimental and computational studies find that 2D CTGU-5 which has coordinates water and more open acce

255 It has been thought that 2D materials are the only seed layers for van der Waals

256 The 2D structure and relative configuration of 1 were initia

257 that globally adjusts contrasts amongst the 2D tiles so as to produce a seamless, high-contrast imag

258 dria, plasma membrane and filopodia, and the 2D and 3D dynamics of the endoplasmic reticulum, in livi

259 First, the 2D projection step employs a specially developed algorit

260 observed enhanced photoluminescence from the 2D photonic crystal and the 1D nanocavities.

261 served in the 3D RSA measurement than in the 2D RL measurement at the evaluated CRRs.

262 ation chemistry or the substrate, making the 2D-Xene systems promising multifunctional 2D materials f

263 everity of periodontitis on the basis of the 2D RL and 3D RSA measurements.

264 deposition of the metal nanoparticles on the 2D carbon nanomaterial planar sheets.

265 By modulating the number of vacancies on the 2D MoS2 nanoassemblies, the physical and chemical proper

266 ntrol of electron delocalization through the 2D COF sheets.

267 emical bonds, are of a great interest to the 2D materials research.

268 We perform dot-product operations with the 2D and 3D memristive crossbars to demonstrate the applic

269 l with the theoretical predictions for these 2D systems.

270 The device potential of these 2D ferroelectric materials is further demonstrated using

271 This 2D lattice structure also develops substantially more sl

272 At approximately 1,100 F cm(-3), this 2D material exhibits a 65% higher volumetric capacitance

273 We have named this 2D colony a 'SEAM' (self-formed ectodermal autonomous mu

274 n binding properties by (1)H NMR titrations, 2D NOESY experiments and computational studies.

275 d eta, for quadrupolar nuclei, I > (1)/2) to 2D correlations, to analysis of chemical shift anisotrop

276 increased resistance to the drug compared to 2D culture where MDA-MB-231 attained a drug-resistant tu

277 f extensive characterizations, extensions to 2D and 3D trajectories, and applications to common scena

278 nctional connectivity using both traditional 2D greenspace models and waveform lidar-generated vegeta

279 issues are beginning to supplant traditional 2D cell cultures and preclinical animal studies that hav

280 performance limitations set by traditional, 2D designs.

281 undred thirteen consecutive renal transplant 2D and 3D ultrasound examinations were performed and ret

282 We report the use of an Ultrafast 2D NMR approach applied on a benchtop NMR system (43MHz)

283 plasmonic responses in SNL, these ultrathin 2D films display rapid and reversible red-blue color cha

284 3D hepatic microtissues, unlike 2D cell cultures, retain many of the in-vivo-like functi

285 Here we use 2D and 3D X-ray imagery on Noril'sk nickel sulfide, comb

286 Using 2D Brownian dynamics simulations, we study a dense, conf

287 Using 2D NMR spectroscopy, we established for the first time t

288 ) addressing each droplet individually using 2D arrays of electrodes and ultrahigh throughput droplet

289 We have tested our method using 2D and 3D DNA brick and DNA origami structures.

290 reover, the novel analytical method of using 2D plasmonic nanoparticle as a sensor to understand the

291 esponding plasma fraction were studied using 2D gel electrophoresis techniques.

292 ization of separation selectivity in various 2D combinations and for other applications.

293 faster than all the directly grown vertical 2D heterostructures.

294 Via 2D X-ray diffraction, highly ordered and textured crysta

295 he nature of the shape dimensionality (1D vs 2D vs 3D) of cell-scaffold interactions relevant to tiss

296 ting intersection of these materials wherein 2D graphenes are hybridized with 3D hydrogels to develop

297 in full-text article.)=97.5%) compared with 2D ((Equation is included in full-text article.)=54.5%)

298 ns, making borophene the first material with 2D plasmons at such high frequencies, notably with no ne

299 les, the amount of information obtained with 2D MS was comparable with what obtained with multiple 1D

300 s; twice as many as previously reported with 2D-UPLC/IM/MS(E) method.