ライフサイエンスコーパス: atomic

1 products by high resolution continuum source atomic absorption spectrometer (HR-CS AAS) after leachin

2 method was developed and combined with flame atomic absorption spectrometry (FAAS) for pre-concentrat

3 ts between 0.13 and 0.35ngmL(-1) using flame atomic absorption spectrometry (FAAS).

4 ed beans, corn, and fungi) by Electrothermal Atomic Absorption Spectrometry (Perkin Elmer, SIMAA 6000

5 owed by Se determination with electrothermal atomic absorption spectrometry.

6 zinc followed by its determination by flame atomic absorption spectrometry.

7 h those results obtained by graphite furnace atomic absorption spectrometry.

8 spectroscopic techniques, namely cold vapour atomic absorption spectroscopy (CV-AAS) and a direct mer

9 validation was performed by using cold vapor atomic absorption spectroscopy.

10 rk and in four of six CDRs in one design and atomic accuracy in the entire Fv in another.

11 more, crystallographic analysis demonstrated atomic accuracy throughout the framework and in four of

12 ese structures we are now firmly within the "atomic age" of electron cryomicroscopy, as these studies

13 tural transformations are correlated at both atomic and mesoscale levels with the band-gap evolution

14 te with negligible motion of domain walls on atomic and mesoscopic scales occurs in the RSG.

15 ere will enable thermal transport studies in atomic and molecular chains, which will be key to invest

16 underwent structural transformation at both atomic- and mesoscales during the pressure processing.

17 diverse fields ranging from the study of 3D atomic arrangements in matter to the study of human heal

18 lecular processes to be described at the sub-atomic, atomic, supra-atomic, or supra-molecular level.

19 wo CVA6 particles have essentially identical atomic capsid structures resembling the uncoating interm

20 The [010] atomic chains and the resulting anisotropic behavior are

21 Small variations on geometry and atomic charge were detected on the carbonate ions, imply

22 great importance in the fields of chip-scale atomic clock and quantum information.

23 anipulating single nuclear spins, exploiting atomic clock transitions for robust qubits and, most rec

24 ies on precision timing signals furnished by atomic clocks.

25 nt of precision sensors and state-of-the-art atomic clocks.

26 ntly dominated by the attachment kinetics of atomic clusters in the liquid phase, melting is instead

27 The aptamer self-assemble onto the gold atomic clusters makes Apt/AuAC/Au an excellent platform

28 iquids, involving a change in the packing of atomic clusters over medium-range length scales as large

29 By varying the extent to which the atomic coefficients of heavy metal d orbitals contribute

30 2.1 A, allowing the resolution of individual atomic columns of Zn and organic linkers in the framewor

31 t complexity of Ub signaling due to the high atomic complexity of Ub conjugates, where Ub is attached

32 superatomic analogue of traditional layered atomic compounds.

33 with Sb/In substitution arise from different atomic configurations for these atoms.

34 opy (cryo-EM) has been used to determine the atomic coordinates (models) from density maps of biologi

35 alculations, there is a pressing need to use atomic coordinates of real systems beyond average crysta

36 nces between subsets of amino acids based on atomic coordinates).

37 to the generation of protein CD spectra from atomic coordinates.

38 searchers to produce CD spectra from protein atomic coordinates.

39 The outer radius is the atomic (covalent) radius, and the inner is that of the u

40 We describe the atomic crystal structures of the catalytic flavin adenin

41 and superlattices from two-dimensional (2D) atomic crystals.

42 le single photon emitters were reported from atomic defects in layered hexagonal boron nitride (hBN),

43 This review of atomic defects in two-dimensional materials will offer a

44 The atomic defects present on the lattice plane of 2D MoS2 n

45 photon eigenmodes (a supermode), coupled to atomic density waves of a quantum gas.

46 new insight on the microscopic mechanisms of atomic desorption from organic coatings.

47 n and atomic force microscopy to deliver, in atomic detail, structural models of three key PANS: the

48 hly abundant class of proteins is scarce, so atomic details of how S-layers are arranged on the surfa

49 The improved structure also reveals atomic details of membrane-lytic protein VI and genome-c

50 cryomicroscopy, as these studies can reveal atomic details of protein and nucleic acid topology and

51 Knowledge of the atomic details of these structures helps our understandi

52 collectively formed, leading to significant atomic disorder that causes the additional reduction of

53 eparation and charge trapping induced by the atomic disorder.

54 often depends on the spatial distribution of atomic displacements within collision cascades.

55 ive atomic motion in the form of string-like atomic displacements, potential energy fluctuations and

56 tron microscopy reveals an interesting local atomic distribution in ReS2x Se2(1-x) alloy, where S and

57 ray diffraction allows the direct imaging of atomic dynamics simultaneously on its natural time and l

58 knowledge-based multibody potential and two atomic energy terms.

59 lly accessible memory cells in a macroscopic atomic ensemble.

60 photon in a crystal that contains many large atomic ensembles with distinct resonance frequencies.

61 Using the homogeneous atomic Fe model catalysts, we elucidated the active site

62 The high-performance atomic Fe PGM-free catalyst holds great promise as a rep

63 istry enables the creation of well-dispersed atomic Fe sites embedded into porous carbon without the

64 er MoTe2 is controlled by simply changing Te atomic flux controlled by the temperature of the reactio

65 y the in-plane crystalline axes of the V2O3; atomic force and scanning electron microscopy reveal ori

66 We applied atomic force microscope (AFM) to demonstrate directly th

67 An atomic force microscope (AFM) was employed to further ex

68 the beta-peptide with the nonpolar tip of an atomic force microscope (AFM).

69 1 nN) to the N-cadherin-coated beads via an atomic force microscope induced a localized mechanical r

70 amined by measuring the forces arising as an Atomic Force Microscope tip (diameter 20 nm) - simulatin

71 cell is formed by bringing a Pt/TiO2-coated atomic force microscope tip into contact with a flat sub

72 l-field enhancement around the region of the atomic force microscope tip.

73 Using a custom-built atomic force microscope, myofibrils were first placed in

74 thogens, via external pressure applied by an atomic force microscope, or via cell migration across un

75 By integrating conducting-probe atomic force microscopy (12,13) with custom-fabricated p

76 To measure islet stiffness, we used atomic force microscopy (AFM) and developed a novel "bed

77 rier transform infrared spectroscopy (FTIR), atomic force microscopy (AFM) and high-resolution scanni

78 Contact and non-contact based atomic force microscopy (AFM) approaches have been exten

79 Atomic force microscopy (AFM) on wild-type BM in vivo re

80 ble because the nanometer-scale radius of an atomic force microscopy (AFM) tip yields a very low sign

81 We then utilize atomic force microscopy (AFM) to demonstrate that the re

82 f scanning probe tips that combine SECM with atomic force microscopy (AFM) to perform measurements at

83 y combining electrical probing measurements, atomic force microscopy (AFM), and scanning transmission

84 ng Cu/In ratio, using Helium Ion Microscopy, Atomic Force Microscopy (AFM), and Time of Flight-Second

85 EM), energy dispersive X-ray analysis (EDX), atomic force microscopy (AFM), scanning electron microsc

86 Atomic force microscopy (AFM), surface plasmon resonance

87 g unmasking were explored in live cells with atomic force microscopy (AFM).

88 HBc particle morphology was confirmed by Atomic Force Microscopy (AFM).

89 tion charges using a conventional conductive atomic force microscopy (CAFM) without a top electrode i

90 Here we present high-speed atomic force microscopy (HS-AFM) observations of membran

91 orce-induced unfolding using single molecule atomic force microscopy (smAFM) and steered molecular dy

92 Height measurements and images obtained by atomic force microscopy also demonstrated the dissociati

93 Atomic force microscopy analysis of PRP and growth facto

94 assembly and dynamics combining electron and atomic force microscopy and biochemical analyses.

95 orin pore assembly, we carried out real-time atomic force microscopy and electron microscopy studies.

96 Here, we use atomic force microscopy and environmental scanning elect

97 ular tunnel formation using a combination of atomic force microscopy and fluorescence microscopy of l

98 ties of these fibers are characterized using atomic force microscopy and Raman spectroscopy.

99 ock copolymers in solution were conducted by atomic force microscopy and transmission electron micros

100 en individual MV3 cells was quantified using atomic force microscopy and validated by multicellular a

101 By using a complementary approach of atomic force microscopy and vertical scanning interferom

102 rmed by X-ray photoelectron spectroscopy and atomic force microscopy experiments.

103 Here we undertake a direct high-speed atomic force microscopy imaging analysis to visualize th

104 ections of M x giganteus stems and leaves by atomic force microscopy indicates that phloem sieve elem

105 Through conductive atomic force microscopy measurements on an ultra-thin (0

106 tetrapods via in situ scanning electron and atomic force microscopy measurements.

107 By performing atomic force microscopy mechanical mapping combined with

108 Images of the template obtained by atomic force microscopy show that TFAM creates loops in

109 Atomic Force Microscopy showed significant alterations t

110 Direct force measurements using atomic force microscopy showed that SdrF mediates bacter

111 y, we show a specific interaction between an atomic force microscopy tip decorated with recombinant a

112 ination of molecular dynamics simulation and atomic force microscopy to deliver, in atomic detail, st

113 Here, we used high-speed atomic force microscopy to directly visualize the membra

114 are formed by solution deposition and we use atomic force microscopy to obtain images of the BP surfa

115 Herein we present a technique that uses atomic force microscopy to probe directly for the phase

116 Atomic force microscopy was used to determine the height

117 al SMH), and roughness and 2D profiles using atomic force microscopy were measured after five cycles.

118 Herein, we show the first application of atomic force microscopy with infrared spectroscopy (AFM-

119 High-speed atomic force microscopy with single-molecule resolution

120 Combining genetics, atomic force microscopy, and immunolabeling, we demonstr

121 Analysis of H and O-NDs by Atomic Force Microscopy, contact angle measurements and

122 complementary biophysical methods, including atomic force microscopy, cryo-electron microscopy, and n

123 ; specifically, we discuss interpretation of atomic force microscopy, Forster resonance energy transf

124 te dielectric and CuPc films are analyzed by atomic force microscopy, grazing incident X-ray diffract

125 Atomic force microscopy, high-resolution flow cytometry,

126 iffness, organization and ultrastructure via atomic force microscopy, second harmonic generation imag

127 Using conducting tip atomic force microscopy, the energies of {Co9(P2W15)3} f

128 By using atomic force microscopy, we found that during reverse tr

129 With single-molecule atomic force microscopy, we show a specific interaction

130 Using atomic force microscopy, we studied the elasticity of mo

131 and dynamics at equilibrium were analyzed by atomic force microscopy.

132 ord at 1.5 and three weeks post-injury using atomic force microscopy.

133 to bind to dental enamel was evaluated using atomic force microscopy.

134 s in adsorption were further interrogated by atomic force microscopy.

135 d by measuring cellular elastic moduli using atomic force microscopy.

136 scence, light scattering, SDS stability, and atomic force microscopy.

137 terisation, as well as scanning electron and atomic force microscopy.

138 e UPSS are validated using in situ real-time atomic-force microscopy, representing the first instance

139 The atomic forces required for the phonon scheme are highly

140 three energy terms [Formula: see text](intra-atomic), [Formula: see text] (electrostatic) and [Formul

141 nd yttrium oxide with an yttrium-to-tantalum atomic fraction of 14% was prepared by magnetron sputter

142 ormation is almost fully transferred between atomic ground states.

143 The superhydride phases consist of an atomic hydrogen sublattice with H-H distances of about 1

144 The atomic interaction of cholesterol with M2, as with most

145 Atomic interactions between the inhibitor and IRAP that

146 pic quality factor of 4 x 10(17) Previously, atomic interactions have forced a compromise between clo

147 ation-mediated gating differed between small atomic ions (current) and fluorescent dye permeants, ind

148 Laser cooling and trapping of atoms and atomic ions has led to advances including the observatio

149 Thermal transport in individual atomic junctions and chains is of great fundamental inte

150 icker medium due to the profoundly different atomic kinetics.

151 oxide (AZO) was deposited by low-temperature atomic layer deposition (ALD) as the transparent conduct

152 template to polydimethylsiloxane (PDMS) via atomic layer deposition (ALD) assisted sacrificial etchi

153 Notably, atomic layer deposition (ALD) in MOFs has recently emerg

154 dimeric methylalumina surface species during atomic layer deposition (ALD) on a silver surface.

155 Here we introduce a new, robust atomic layer deposition (ALD) procedure for the preparat

156 ted with an aluminum oxide film deposited by atomic layer deposition (ALD) with optically pumped NMR

157 thin films of Zinc Oxide (ZnO) deposited by atomic layer deposition (ALD).

158 of two stacking faults separated by a single atomic layer, and proceeded with the emission of a parti

159 High-quality two-dimensional atomic layered p-n heterostructures are essential for hi

160 .e., virtual vacancy layers) in the stack of atomic layers and the concurrent reconfiguration of In a

161 be tuned by changing the number of inorganic atomic layers in between the organic cation layers.

162 f guest atoms, ions or molecules between the atomic layers of a host structure, can produce novel ele

163 arriers converge as the step height is three atomic layers or thicker.

164 ge ferromagnetic order in pristine Cr2Ge2Te6 atomic layers, as revealed by scanning magneto-optic Ker

165 that probes local motions of a system at the atomic level by allowing extraction of dynamical paramet

166 of unequivocal structural information at the atomic level for complex systems is uniquely important f

167 methods, no direct observation of DPD at the atomic level has been reported.

168 d has been actively investigated approaching atomic level patterning.

169 Our study elucidates at atomic level that the hydrophobicity and substitution ge

170 relationship of RNA both in real time and at atomic level will have a profound impact in advancing ou

171 (1)H photo-CIDNP for characterizing, at the atomic level, transient species involved in electron-tra

172 ntal understanding of their properties on an atomic level, we investigate single crystals of CH3NH3Pb

173 ls of initiation-to-elongation transition on atomic level.

174 Our findings provide an atomic-level characterization of the genome release mech

175 molecular dynamics simulations, providing an atomic-level description of alternating access transport

176 echniques have been correlated to illuminate atomic-level details of bond breaking and formation duri

177 osystem II allows us to identify the precise atomic-level differences between organisms in the vicini

178 pret experimental results and understand the atomic-level dynamics of chemical reactions; (2) illustr

179 ncies present in the samples, thus providing atomic-level insights into the structures of colloidal T

180 of prototypical RRNPP members have provided atomic-level insights into their mechanism and regulatio

181 The structure and the atomic-level interactions were determined by saturation

182 ursuit, yet little has been achieved for the atomic-level manipulation of metallic nanomaterials.

183 Here, we elucidate the atomic-level nature of Cs and Rb incorporation into the

184 Determining a complete atomic-level picture of how minerals grow from aqueous s

185 olloidal nanoclusters as a function of their atomic-level structural characteristics.

186 to derive direct correspondence between the atomic-level structural correlations and reported proper

187 Murray et al. report an atomic-level structural model for FUS LCD fibrils that a

188 rates, we conclude that there is no fractal atomic-level structure associated with the packing of al

189 Scanning tunnelling microscopy and atomic manipulation can be used to assemble a two-dimens

190 mass number less than 140) and one of heavy (atomic mass number greater than 140) r-process elements.

191 of ejecta, one composed primarily of light (atomic mass number less than 140) and one of heavy (atom

192 ducts were observed from scan range 200-1000 atomic mass units (amu) in the aqueous phase after irrad

193 re consistent with light r-process elements (atomic masses of 90-140).

194 A, which are close to predictions for solid atomic metallic hydrogen at these pressures.

195 e dayside atmosphere of KELT-9b are probably atomic metals.

196 rotated and translated to provide an initial atomic model for the new structure.

197 We present an atomic model of a substrate-bound inner mitochondrial me

198 Here we report the complete atomic model of the headful DNA-packaging bacteriophage

199 Accurate atomic modeling of macromolecular structures into cryo-e

200 e of yeast U1 snRNP at 3.6 A resolution with atomic models for ten core proteins, nearly all essentia

201 ess, molecular dynamics simulations based on atomic models of the KcsA channel were performed.

202 For a set of 50 RNA structures, we obtain atomic models with reasonable geometries and interaction

203 urfaces were performed using the large-scale Atomic/Molecular Massively Parallel Simulator (LAMMPS) w

204 Atomic motion at grain boundaries is essential to micros

205 lass-forming (GF) liquids such as collective atomic motion in the form of string-like atomic displace

206 cs simulations, PGC1alpha induced correlated atomic motion throughout the entire LRH-1 activation fun

207 c performances, but the understanding of the atomic motions remains inadequate even though they take

208 Using suitable representations of atomic neighborhoods and Kernel Ridge Regression, we sho

209 is performed using descriptors comprised of atomic NMR chemical shifts ((13)C and (15)N NMR) and cor

210 he ferrofluid "multiverse" is populated with atomic or molecular species, and these species are excit

211 e described at the sub-atomic, atomic, supra-atomic, or supra-molecular level.

212 ated to evaluate the effect of the extent of atomic orbital overlap on their reactivity.

213 y functional theory with the gauge invariant atomic orbitals (DFT-GIAO).

214 Our atomic overlap distance complements computed partial cha

215 Through high-energy x-ray diffraction and atomic pair density function analysis we find that Zr-ba

216 ilicon oxycarbide (SiOC) alloys by using the atomic pair-distribution function (PDF) obtained from el

217 n protocols accessible with state-of-the-art atomic physics experiments.

218 les and their structural characterization to atomic precision are important challenges in nanoscience

219 his assay can be correlated to amino-acid or atomic propensities weighted by the surface areas obtain

220 nit cell with perfect matching between their atomic radius and space size of each X site.

221 o Pd-Ni-P nanoparticles and tuning the Ni/Pd atomic ratio to 1:1.

222 (236)U/(238)U atomic ratios in Danish seawater are more than 4 times h

223 The levels of (236)U/(238)U atomic ratios obtained are comparable to those reported

224 the cryo-EM structure of mature JEV at near-atomic resolution and identify structural elements that

225 uctural basis for this stabilization with an atomic resolution crystal structure.

226 ectron microscopy (cryo-EM), we establish an atomic resolution model of the RSV CA tubular assembly u

227 We construct atomic resolution models of thousands of candidate subst

228 structure for the apo form of AgmNAT with an atomic resolution of 2.3 A, which points towards specifi

229 cryo-electron microscopy structures at near-atomic resolution of Hsp104 in different translocation s

230 Here, we describe the near-atomic resolution structure of the phi6 double-shelled p

231 systems, new methods are required to obtain atomic resolution structures from biological material un

232 ral major capsid protein, elucidated at near-atomic resolution using cryo-electron microscopy, is str

233 f mature Japanese encephalitis virus at near-atomic resolution, which reveals an unusual "hole" on th

234 eikastus rhodopsin 2 (KR2), was resolved at atomic resolution.

235 n only if the protein structure is solved to atomic resolution.

236 peptide-activated GLP-1R-Gs complex at near atomic resolution.

237 ecular interface remain poorly understood at atomic resolution.

238 ependency of the intensities associated with atomic-resolution annular dark field imaging line scans

239 se molecular dynamics simulations to provide atomic-resolution insight into the influence of choleste

240 ent strategy to inactivate TNFalpha, but the atomic-resolution mechanism of its inactivation remains

241 These atomic-resolution observations offer a basis for rationa

242 ly weak superstructure phenomena revealed by atomic-resolution scanning TEM (STEM) and single-crystal

243 Atomic-resolution scanning transmission electron microsc

244 approach uses multiple-sequence alignments, atomic-resolution structural information, and riboswitch

245 persion of the parameters from a database of atomic-resolution structures.

246 particle porosity and fractal arrays at the atomic scale for the S-Mo-S(Co) 2D- layers that conform

247 face structures under reaction conditions at atomic scale is critical for understanding reactivity.

248 the reduction of material dimensions to the atomic scale poses a challenge for traditional measureme

249 roperties of these films are designed at the atomic scale using layer-by-layer assembly of two-dimens

250 urthermore, by confining the filament to the atomic scale, current switching characteristics are obse

251 This sensitivity, approaching the atomic scale, holds the promise of extreme subwavelength

252 , phonon oscillations can be observed on the atomic scale.

253 are not fully understood, especially at the atomic scale.

254 oviding access to picosecond dynamics at the atomic scale.

255 The collective atomic-scale defect disorder improves the zT to 1.09 +/-

256 x Hfx NiSn1-y Sby alloys containing inherent atomic-scale defect disorders are produced in one hour b

257 d controlled phonon emission from individual atomic-scale defects in graphene.

258 Together, these results provided atomic-scale descriptions of the SrtC substrate selectiv

259 ding of core-shell formation is critical for atomic-scale design and control of the platinum shell, w

260 een possible, as the recovery process at the atomic-scale has been difficult to observe.

261 highly active, and we delineate the specific atomic-scale mechanisms associated with their nucleation

262 Using dynamic, atomic-scale resolution electron microscopy observations

263 The achieved atomic-scale spatial resolution in remote sensing of spi

264 independent reading and writing, we built an atomic-scale structure with two Ho bits, to which we wri

265 deformation of nanocrystalline C-S-H to its atomic-scale structure, which is changed by varying the

266 Here, by performing in situ atomic-scale transmission electron microscopy, we report

267 rface Au atomic sites "coalesce" into one Cd atomic site and, accordingly, a new bimetal nanocluster,

268 cluster, in which two neighboring surface Au atomic sites "coalesce" into one Cd atomic site and, acc

269 es consistent with experimentally determined atomic sites and fractional occupancies.

270 have been limited to one donor because their atomic size causes fabrication challenges.

271 e system, a change that occurs indirectly in atomic solid-solid phase transitions via changes in temp

272 bute, and at separations comparable to inter-atomic spacing the transition to heat conduction should

273 appear on the spectral continuum, indicating atomic species produced by nucleosynthesis that occurs i

274 calculations of material properties such as atomic spin and orbital magnetic moments and local magne

275 educes the influence of dissipations such as atomic spontaneous emissions and cavity decays.

276 h low coordination numbers, such as found at atomic steps and surface defects, is firmly established.

277 Here we report a HCMV atomic structure consisting of the herpesvirus-conserved

278 n fluorescence imaging and higher-resolution atomic structure determination, to cover the full scale

279 sing cryo-electron microscopy, we solved the atomic structure of an apex bnAb, PGT145, in complex wit

280 Here we present a de novo atomic structure of Drosophila NOMPC determined by singl

281 Here, we report the near-atomic structure of jasplakinolide (JAS)-stabilized PfAc

282 mputational modeling, we resolve the precise atomic structure of metal-oxo species deposited in the M

283 Although the atomic structure of T4 is largely known, the dynamics of

284 o other heterogeneous catalysts, the surface atomic structure of the nanoporous metal catalysts plays

285 The cellular S-layer atomic structure shows that the S-layer is porous, with

286 In this work, we report the atomic structure, electronic properties, and vibrational

287 Based on the atomic structure, we propose a local seeding model where

288 f electronic excitation, chemical state, and atomic structure.

289 These results elucidate how surface atomic structures determine the reaction pathways via bo

290 microelectron diffraction, we determined the atomic structures of 11-residue segments from both Abeta

291 that can be further used for two-dimensional atomic super-resolution optical testing and sub-waveleng

292 processes to be described at the sub-atomic, atomic, supra-atomic, or supra-molecular level.

293 A many-body atomic system coupled to quantized light is subject to w

294 honon analog of the vacuum Rabi splitting in atomic systems.

295 Because of its atomic thickness and unique properties, graphene opens u

296 o observe ballistic, diffusive, and arrested atomic transport.

297 microcosm occurs on a time scale set by the atomic unit of time-24 attoseconds.

298 e plane of 2D MoS2 nanoassemblies are due to atomic vacancies and can act as an active center for vac

299 introduce so-called intrinsic defects, e.g., atomic vacancies and/or interstitials.

300 the main phase, with chloride content of 3-5 atomic weight %.