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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
11 ; typical large needle-like arrays having 20 2D layers units correspond to a model consisting of smoo
13 owever, corresponding to a 75%, 50%, and 25% 2D BSH reserve, premolars retained 67-68%, 39-41%, and 1
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
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
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
28 re, we adapt this raster/vector concept to a 2D colloidal system and realize 'vector assembly' by man
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
38 sional (2D) gradient-recalled echo (GRE) and 2D spin-echo (SE) echo-planar imaging (EPI) magnetic res
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
47 restricted by the applied approaches such as 2D conventional soft lithography methods that have recta
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
54 o-target binding predictions inaccessible by 2D fingerprints and confirm three of them experimentally
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
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-
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
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
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
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
93 n ecosystems have relied on two-dimensional (2D) measures of greenspace structure to calculate connec
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
100 and use it to prepare novel two-dimensional (2D) pi-conjugated COFs, as crystalline powders and exfol
103 r synthesizing high-quality two-dimensional (2D) semiconductors is essential for their practical appl
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.
116 imensional-differential gel electrophoresis (2D-DIGE) to compare protein expression profiles of trans
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
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
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
136 analysis of a prototypical Vbeta8.1(+) TCR-H-2D(b)-GAP5040-48 ternary complex revealed that germline-
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
142 also highlight technological developments in 2D IR that continue to expand the scope of scientific pr
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
148 ice architecture as the structural phases in 2D materials such as transition metal dichalcogenides ar
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
155 ndocrine-dependent cell line (MCF-7:WS8), in 2D and 3D cultures, using ERalpha in-cell westerns, ERE-
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
166 thesis and characterization of graphene-like 2D materials, single and few-atom-thick layers of van de
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
175 Efforts have been devoted to exploring novel 2D and 3D auxetic structures through rational design, op
177 rous areas, but the construction of objects, 2D and 3D crystalline lattices and devices is prominent
179 ethylsiloxane) substrates and a new class of 2D elastomeric substrates with controlled patterned rigi
181 gh Young's modulus and surface conformity of 2D capping layers such as graphene and MoS2 substantiall
184 ults will inform the rational development of 2D COF polymerizations by controlling the rate of nuclea
186 g contributing to the synergistic effects of 2D morphology, amorphous structure, conductive substrate
188 demonstrate controlled strain engineering of 2D semiconductors during synthesis by utilizing the ther
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
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
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
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
219 resonance mass spectrometry (2D FTICR MS or 2D MS) allows direct correlation between precursor and f
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
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,
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
234 embly for the crafting of high aspect ratio, 2D sheets that are densely surface-decorated with DNA.
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
240 processing tasks above resulting in a single 2D image of the stained manifold across which contrast i
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
245 y by adding silicene, germanene and stanene (2D allotropes of Si, Ge, and Sn), lends itself as a plat
247 aminations performed with DBT plus synthetic 2D imaging (38.5 screens per hour) than with FFDM (60 sc
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
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
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
262 ation chemistry or the substrate, making the 2D-Xene systems promising multifunctional 2D materials f
265 By modulating the number of vacancies on the 2D MoS2 nanoassemblies, the physical and chemical proper
268 We perform dot-product operations with the 2D and 3D memristive crossbars to demonstrate the applic
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
281 undred thirteen consecutive renal transplant 2D and 3D ultrasound examinations were performed and ret
283 plasmonic responses in SNL, these ultrathin 2D films display rapid and reversible red-blue color cha
288 ) addressing each droplet individually using 2D arrays of electrodes and ultrahigh throughput droplet
290 reover, the novel analytical method of using 2D plasmonic nanoparticle as a sensor to understand the
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
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