ライフサイエンスコーパス: scatter

1 entral/paracentral, enlarged blind spot, and scatter).

2 al consistency (by mitigating the effects of scattering).

3 dynamics (e.g. formation of flocks, streams, scattering).

4 d VAMP-7 recapitulates light-cytometric side scatter.

5 but into near-field surface waves in reverse scattering.

6 rely by Raman mapping and confirmed by X-ray scattering.

7 stent with interference of bulk and boundary scattering.

8 r of relative strength of single to multiple scattering.

9 g sponge phase observed by small-angle x-ray scattering.

10 ay free electron laser using inelastic X-ray scattering.

11 d, which is expected to be gradual with weak scattering.

12 honon anomalies in LSNO by inelastic neutron scattering.

13 g single molecule FRET and small angle X-ray scattering.

14 correlated with phase breaking by polariton scattering.

15 n microscopy and in-situ small angle neutron scattering.

16 er vesicle size as measured by dynamic light scattering.

17 ing of a conjugated polymer system via X-ray scattering.

18 nline can be difficult: They're often widely scattered across the internet or hidden in their home in

19 -paired regions, covering much of the RNA in scattered acyl esters.

20 erosols, resulting in higher particle single-scattering albedo (SSA).

21 th more than one hundred discrete Spitz nevi scattered all over her skin.

22 n performed, and cases described to date are scattered among at least 14 publications.

23 the wealth of available experimental data is scattered among multiple resources and must be gathered,

24 xpressed and purified proteins, static light-scattering analysis, and disaggregation assays, we repor

25 Using few scattered and noisy measurements, we are able to infer t

26 Using neutron scattering and ab initio calculations, we report here a

27 tools and fluorescent probes, and decreased scattering and absorption in mammalian tissues.

28 electrochemical measurements, operando X-ray scattering and absorption spectroscopy, and density func

29 structurally identical) by small-angle X-ray scattering and analytical ultracentrifugation revealed t

30 ructure of the supramolecular polymer, light scattering and atomic force microscopy experiments show

31 are challenging, however, due to substantial scattering and autofluorescence in tissue at visible (35

32 with the help of small- and wide-angle x-ray scattering and complementary neutron diffraction experim

33 fect on corneal collagen architecture, x-ray scattering and electron microscopy data were collected f

34 acentrifugation, reinforced by dynamic light scattering and environmental scanning electron microscop

35 ric complex in solution by small-angle X-ray scattering and find that mutations that disrupt the comp

36 ows us to excite water with stimulated Raman scattering and hemoglobin with transient absorption.

37 peak position [Formula: see text] by neutron scattering and in simulations.

38 rustrated lattice by means of resonant X-ray scattering and Lorentz transmission electron microscopy

39 Here, neutron scattering and molecular-dynamics simulations reveal the

40 clusion chromatography with multiangle light scattering and native mass spectrometry (MS) for the bio

41 de at room temperature using inelastic X-ray scattering and neutron scattering techniques.

42 zed complexes were measured by dynamic light scattering and NMR respectively.

43 These dual scattering and spectroscopy methods are used to demonstr

44 ilized, featuring coherent anti-Stokes Raman scattering and stimulated Raman scattering modalities.

45 restimating the contribution from flask wall scattering and the corresponding dose distribution.

46 Simultaneous measurements of resonant X-ray scattering and transport reveal that this drastic respon

47 nductors is to avoid the formation of charge scattering and trap sites from adjacent dielectrics.

48 icles were characterized using dynamic light scattering and were found to have a diameter of 108+/-2.

49 How natural photonic systems manage light scattering and what can be learned from plants and anima

50 uation-corrected (AC) OSEM, and attenuation, scatter, and collimator response-corrected (ASCC) OSEM.

51 Combining oxygen sensing, X-ray scattering, and Atomic Force Microscopy, we show that ma

52 tallography, biochemistry, small angle X-ray scattering, and electron microscopy unveil an XPG homodi

53 ry (DSC), grazing-incidence wide-angle X-ray scattering, and microscopy can be related directly to de

54 tometry, thermodynamic measurements, neutron scattering, and Monte Carlo simulations, we establish Ho

55 s; and immunofluorescence, small-angle X-ray scattering, and MS-based analyses, we report that GAPDH

56 that govern magnon generation, propagation, scattering, and relaxation.

57 re for diffraction is evident by varying the scattering angle and observing sharp features in the sca

58 The EES and electron-lattice scattering are intertwined resulting in breaking of the

59 diffraction based on both Bragg and diffuse scattering are powerful techniques to achieve such goal.

60 Rayleigh scattering, arising from frozen-in density fluctuations

61 we introduce time-resolved two-magnon Raman scattering as a real time probe of magnetic correlations

62 stic waves is the presence of reflection and scattering at sharp edges, defects, and disorder.

63 Emission data were corrected for scatter, attenuation, and decay supplemented by resoluti

64 estricted to a few presynaptic terminals and scattered axonal growth cones.

65 dynamic information contained in the diffuse scattering background.

66 However, polarized infrared imaging under scattering based on 2D materials has yet to be realized.

67 vage of complement C3, and small-angle X-ray scattering-based modeling indicates that this occurs thr

68 reduces the kappa(latt) by effective phonon scattering because of the excess point defects and rich

69 olecular interactions results in distinctive scattering behavior, ranging from the universal Wigner l

70 rized by unorganized clusters of macrophages scattered between lymphocytes.

71 e use of expensive chiral phosphines is more scattered, but the most common ligands include BINAP, Me

72 es, grain boundary, and polar optical phonon scattering, but has negligible influence on lattice ther

73 ent beam into far-field radiation in forward scattering, but into near-field surface waves in reverse

74 untable attenuation limit set by the glass's scattering, but requires reduction of all the other loss

75 transverse acoustic phonons are almost fully scattered by the compound's intrinsic distorted rocksalt

76 racting waveforms, we detected seismic waves scattered by three-dimensional structures near the core-

77 ivity than inherently weak spontaneous Raman scattering by exciting localized surface plasmon resonan

78 ave enjoyed excellent agreement with quantum scattering calculations performed on state-of-the-art co

79 reporter mice and coherent anti-Stokes Raman scattering (CARS) imaging of the sciatic nerve, we decip

80 tion of Sb-doping leads to additional phonon scattering centers and optimizes the p-type carrier conc

81 A surface-enhanced Raman scattering-chiral anisotropy (SERS-ChA) effect is report

82 lementary tools such as X-ray and/or neutron scattering combined with electron diffraction and imagin

83 arried out to determine the spatial electron scattering contribution from the flask walls.

84 orrected PET (PET(NC)) into attenuation- and scatter-corrected PET (PET(ASC)).

85 the regions with attenuation correction- and scatter correction-based artifacts.

86 d IR imaging system and state-of-the-art Mie scattering corrections, we observe how the presence of m

87 Conversely, multiangle laser light scattering-coupled size exclusion chromatography and dyn

88 e measurement and analysis of absolute Raman scattering cross sections spanning the frequency range o

89 es simulations, to determine ratios of Raman scattering cross-sections of aqueous species under extre

90 listic trial arrangements of SCR domains for scattering curve fits.

91 ively consistent with that from experimental scattering data on high MW (>10 kDa) PEO and the P(R(ee)

92 Small-angle X-ray scattering data revealed that in the presence of tRFs, h

93 Neutron-scattering data reveals that most of the void space with

94 n structures in this library fit well to the scattering data, and these structures readily accommodat

95 simulations constrained by high energy x-ray scattering data.

96 onstructs, spanning N6-N3, small-angle X-ray scattering demonstrates that the tandem VWA array has a

97 By using in situ grazing-angle X-ray scattering/diffraction, X-ray absorption spectroscopy, a

98 ng angle and observing sharp features in the scattered distribution.

99 Using dynamic light scattering (DLS) and ultra high pressure liquid chromato

100 ere characterized by XRD, FTIR dynamic light scattering (DLS), FESEM, HRTEM, and EDX spectroscopy alo

101 ion electron microscopy (TEM), dynamic light scattering (DLS), Fourier-transform Infrared (FT-IR) and

102 Angle X-ray Scattering (SAXS), Dynamic Light Scattering (DLS), Transmission Electron Microscopy (TEM)

103 rroelectrics that contain high-density light-scattering domain walls.

104 l T(-1.5) dependence, indicating that phonon scattering dominates the charge carrier transport.

105 We map the pattern using the scattering dynamics of phonon polaritons launched in hex

106 ing substrate-based 2D biosensors produces a scattering effect, which leads to a irregular signals fr

107 Using a combination of calorimetric, scattering, electron microscopic, and in silico techniqu

108 re analyzed by Zeta potential, dynamic light scattering, electron microscopy, and other spectroscopic

109 n methods and characterised by dynamic light scattering, electron microscopy, encapsulation efficienc

110 cture determinations by the use of intrinsic scattering elements.

111 ines chiral discrimination and surface Raman scattering enhancement on chiral nanostructured Au films

112 (full visible range) lossless multiple light scattering events, enabled by a highly porous (>99.99%)

113 However, in the literature, one can find scattered evidence that other, more abundant saccharide

114 Small- and wide-angle X-ray scattering examines the packing of PE chains into semicr

115 Since scattering experiments and analytical calculations usual

116 al docking experiments, and multiangle light-scattering experiments disclosed novel oligomeric states

117 This enabled us to perform neutron scattering experiments where we observe close to quarter

118 n operando synchrotron X-ray diffraction and scattering experiments with geochemical modeling to cont

119 We combine optical spectroscopy and light-scattering experiments with theoretical modeling to show

120 ed resolution via coherent anti-Stokes Raman scattering (FASTER CARS) using tip-enhanced techniques m

121 ission electron microscopy, wide-angle x-ray scattering, Fourier transform infrared spectroscopy, and

122 orientation indices were recorded for small-scatter Fraunhofer diffraction patterns and also visuali

123 particles, have been proposed to demonstrate scatter-free chiral propagation, but their experimental

124 rriers and is affected by crystal structure, scattering from boundaries and defects, and strain.

125 The overall intensity of scattering from cancerous regions is a degree of magnitu

126 However, scattering from defects, grain boundaries, and interfaci

127 vel of Jupiter's atmosphere (assuming photon scattering from points beneath the clouds)(1-3,7,8,10-12

128 We show that the speckle contrast in scattering from water depends on the delay-time as expec

129 ic, fast-neutron backscatter and the Compton-scattered gamma radiations, simultaneously.

130 SLs with grazing-incidence small-angle X-ray scattering (GISAXS) while using nuclear magnetic resonan

131 hermal analysis, and grazing incidence X-ray scattering (GIWAXS) techniques.

132 Their hyper-Rayleigh scattering (HRS) responses in solution were accordingly

133 -OCT of the right eye revealed a highly back-scattering hyper-reflective vessel across the fovea with

134 ission electron microscopy and dynamic light scattering identified nonfibrillar ~20-nm oligomers, whi

135 Although a large scatter in the results (DeltaC/Zr = 0.07) from these dif

136 er graphene and of umklapp electron-electron scattering in graphene superlattices.

137 absence of any evidence of ionized impurity scattering in Te-doped Mg(3) Sb(2) single crystals prove

138 CD and dynamic light scattering indicate that a conformational transition in

139 te's duration in a standard laboratory light scattering instrument we reproduce the theoretically pre

140 face-modified nanoparticles displayed higher scattering intensities in a particle-size dependent mann

141 onally, as a background signal, the relative scattering intensities provide a quantitative measure of

142 The small angle neutron scattering intensity measured in-situ, over a Q-range of

143 fraction limitations by using changes in the scattering intensity of a continuous wave visible laser

144 e SAXS patterns, axial d-spacing and diffuse scattering intensity were observed to provide the greate

145 The measured scattering intensity, fitted by the maximum entropy mode

146 therefore used an emerging technique, X-ray scattering interferometry (XSI), to directly probe the c

147 ctrons from the large, "cold" Fermi surfaces scatter into one hot and one cold electron renders the o

148 Such enhanced scattering is a powerful tool for light manipulation, bu

149 Solvent scattering is a valuable internal reference for determin

150 Here, we used interferometric scattering (iSCAT) microscopy to monitor diffusion of si

151 We used interferometric scattering (iSCAT) microscopy to track dynein-dynactin-B

152 (88)Sr(+) ion with our stimulated Brillouin scattering laser and achieve a clock exhibiting short-te

153 medial frontoparietal lobes, in addition to scattered lateral frontal, parietal, and temporal areas.

154 se organisms, nanostructures that coherently scatter light create structural color, but how such stru

155 of NLOS imaging is that diffuse reflections scatter light in all directions, resulting in weak signa

156 length scales, their resonant modes begin to scatter light into many spatial channels.

157 By monitoring Raman-scattered light from a single-trapped liposome, the effe

158 We use a sensitive and fast measurement of scattered light from nanoliter droplets to demonstrate r

159 The linearly polarized, inelastically scattered light rotates by ~40 degrees , more than two o

160 e we demonstrate the tuning of inelastically scattered light through symmetry control in atomically t

161 Intra-acinar ductular cells and the scattered loss of myoepithelial cells are other abnormal

162 raphy (MM SEC) coupled with multiangle light scattering (MALS) to analyze different forms of bispecif

163 We present a finely sampled diffuse scattering map from triclinic lysozyme with unprecedente

164 The scattering matrix we obtain from the experimental data d

165 tes in solution exhibit correlation peaks in scattering measurements and simulations.

166 Grazing-incidence wide-angle X-ray scattering measurements are conducted to study the cryst

167 oring materials science problems using x-ray scattering measurements at a synchrotron beamline.

168 xperiments and independent small angle x-ray scattering measurements demonstrate that heme disassocia

169 e exclusion chromatography and dynamic light scattering measurements showed that the polydisperse pre

170 Finally, we show that the same scattering mechanism into hot electrons that are instead

171 s can elucidate the electronic structure and scattering mechanisms in materials and is particularly h

172 me for free charge carriers, indicating that scattering mechanisms limiting the mobility are mitigate

173 Conventional approaches for imaging through scattering media operate at microscopic scales or requir

174 maging, cryo-EM tomography and in-situ X-ray scattering methods.

175 comparable to the resolution of small-angle scattering methods.

176 g toolkit that makes use of stimulated Raman scattering microscopy and deep learning-based computatio

177 In this study, coherent Raman scattering microscopy was used to probe de novo intracel

178 Stokes Raman scattering and stimulated Raman scattering modalities.

179 tical ultracentrifugation, small-angle X-ray scattering, molecular dynamics simulations and a DNase I

180 cterized this complex protein by HPLC, light scattering, MS analysis, differential scanning fluorimet

181 Highly sensitive laser light scattering observations have revealed that loud speech c

182 We exploited the anomalous scattering of bromine and iodine to define the pose of t

183 Strong scattering of phonon quasiparticles by anharmonicity and

184 Scattering of seismic waves can reveal subsurface struct

185 the ligand association and small-angle x-ray scattering of the dual domain in the absence and presenc

186 rise the impact of fluctuations and impurity scattering on the thermodynamic properties.

187 ty ring down spectroscopy probed by Rayleigh scattering optical frequency domain reflectometry (OFDR)

188 labeling for NMR, or deuteration for neutron scattering or diffraction, can be realized by an efficie

189 techniques such as static and dynamic light scattering or sedimentation have proliferated to the poi

190 Findings in this research area are scattered over a variety of sources and subfields.

191 (1.4%) and cytomegalovirus (6%), were rare, scattering over 12 months across all SOT recipients.

192 representation of three-dimensional diffuse scattering, over a wide range of spin Hamiltonians.

193 mbined it with synchrotron-based X-ray total scattering, pair distribution function (PDF) analysis, a

194 vestigate the relationship between suspended scattering particles in motion (SSPiM) in optical cohere

195 ous sizing of a single droplet using its Mie scattering pattern.

196 rmore, it is possible to establish a carrier scattering phase diagram, which can be used to select re

197 esses responsible for refocusing diffusively scattered photons without violating the second law of th

198 ood flow, they remain far-removed from light scattering physics and difficult to interpret in layered

199 However, the presence of scattering places fundamental limits on our ability to i

200 differential log-hazard ratio, the survival scatter plot, the hazard ratio receiver operating charac

201 In the randomized study, the EI scatter plots were visibly separated for the low- and hi

202 the temporally-invariant distribution of the scattered pressure field arising from the presence of sc

203 y applicable to other materials and types of scattering problems.

204 e through a complex medium as if observing a scattering process in reverse, entering the medium as a

205 Specifically, a scattering process in which two electrons from the large

206 ed by discrete electron-spin and phonon-spin scattering processes induces the formation of spin fluct

207 leon densities, however, proton- and neutron-scattering processes may alter the effective width of th

208 lar dichroism and solution small-angle X-ray scattering profiles consistent with the design models an

209 fine structure (EXAFS); resonant soft X-ray scattering (R-SoXS); ultraviolet photoelectron spectrosc

210 a minimum bound(3,4), with an interparticle scattering rate saturating(1) at the Planckian time, the

211 We find that the 2ph scattering rates are as large as nearly half the value o

212 ur theoretical analysis agrees well with the scattering rates extracted from measurements of electron

213 e lifetimes, we compute and converge the 2ph scattering rates, and analyze their energy and temperatu

214 les the associated electron-two-phonon (2ph) scattering rates.

215 eedback inputs from higher visual areas have scattered receptive fields relative to their putative ta

216 -mm-thick detectors and intercrystal Compton scatter recovery), good energy and timing resolutions (u

217 o overcome this challenge by supporting back-scattering resistant wave transmission.

218 We observe wide scattering resonance features in both elastic and inelas

219 gner laws near 0 kelvin to the occurrence of scattering resonances at higher energies.

220 The driven spinwave undergoes four-magnon scattering resulting in an increase in the population of

221 X-ray scattering revealed no difference in average collagen in

222 tu neutron diffraction and inelastic neutron scattering revealed that confined nickel(II) sites enabl

223 Steady-state operando X-ray scattering reveals a doping-induced lamellar expansion o

224 Time-resolved operando X-ray scattering reveals asymmetric rates of lamellar structur

225 By combining in situ HP-small-angle neutron scattering (SANS) and HP-ultraviolet/visible absorption

226 in cooperation with the small angle neutron scattering (SANS) measurement.

227 Small angle neutron scattering (SANS) provides a method to obtain important

228 sing synchrotron radiation small-angle X-ray scattering (SAXS) and circular dichroism (CD).

229 Using synchrotron small angle x-ray scattering (SAXS) techniques, determining nanometer scal

230 We use small-angle X-ray scattering (SAXS) to characterize the structure of this

231 By small angle X-ray scattering (SAXS) we have demontrated how the self-assem

232 M structure, combined with small-angle X-ray scattering (SAXS), also allowed us to predict the genera

233 Small-Angle X-ray Scattering (SAXS), Dynamic Light Scattering (DLS), Trans

234 Using small angle X-ray scattering (SAXS), we elucidate the ensemble of Bvht RNA

235 pertussis, as measured by small angle X-ray scattering (SAXS).

236 chromatography coupled to small-angle X-ray scattering (SEC-SAXS) of this hybrid module bound to 1D1

237 s, plasmonic devices, Surface-Enhanced Raman Scattering (SERS) and biological applications.

238 emical specificity of surface-enhanced Raman scattering (SERS) for online detection of metabolites fr

239 been developed as the surface-enhanced Raman scattering (SERS) probes for sensing transduction; and a

240 Surface-enhanced Raman scattering (SERS) spectroscopy offers the unique possibi

241 l-free detection, via surface-enhanced Raman scattering (SERS), of picomolar concentrations of biomar

242 mical (EC) biosensor, surface enhanced Raman scattering (SERS)-based biosensor, field-effect transist

243 dy, we fabricated the surface-enhanced Raman scattering (SERS)-based molecular sensors for detection

244 X-ray crystallography and small-angle X-ray scattering showed that 5-benzyloxygramine stabilizes the

245 LNPs compared to spherical LNPs, while x-ray scattering shows little disparity in internal structure.

246 early perfect understanding of atom-molecule scattering shows that RET usually occurs by only a simpl

247 -range static ferromagnetic order, inelastic scattering shows that short-range correlated antiferroma

248 However, light absorption and scattering significantly prevents penetration to deep br

249 to dynamical arrest, combining dynamic light scattering, small-angle x-ray scattering, tracer-based m

250 Such waves are special "pre-scattered" spatiotemporal fields, which propagate throug

251 llimator penetration, hardware versus object scatter, spectral crosstalk, spatial resolution, spatial

252 u films (CNAFs) equipped in the normal Raman scattering Spectrometer.

253 n spectroscopy, followed by stimulated Raman scattering (SRS) microscopy and transcriptomics analysis

254 he utility of hyperspectral stimulated Raman scattering (SRS) microscopy associated with a Raman tag

255 ns via ultrafast multicolor stimulated Raman scattering (SRS) microscopy for cellular phenotyping.

256 tates, despite being resonantly coupled to a scattering state, become protected from decay whenever t

257 uasi-2DEGs dramatically reduces the Frohlich scattering strength.

258 ent structural colors, where isotropy in the scattering structure is present, only produce coloration

259 al and parity states of v = 10 for inelastic scattering studies.

260 ptive SDRC effect through combining particle scattering, sunlight-excited fluorescence, and mid-infra

261 D curvature can be utilized to tune the back-scattering-suppressed electrical transport of Dirac ferm

262 onance spectroscopy (PDS), small-angle x-ray scattering, targeted protein cross-linking, and cryo-ele

263 ible using a surface plasmon resonance (SPR) scattering technique.

264 es and lattice dynamics by combining neutron scattering techniques with first-principles simulations.

265 Light scattering techniques yield deep insights into the chang

266 rgy- and momentum-resolved neutron and X-ray scattering techniques, combined with first-principles ca

267 ide catalyst with the aid of in situ neutron scattering techniques.

268 using inelastic X-ray scattering and neutron scattering techniques.

269 organic media reveals (by small-angle X-ray scattering) that differing supramolecular assemblies are

270 ction algorithms based on rigorous dynamical scattering theories, the thin-film-based X-ray waveguide

271 By means of light scattering, this study presents absolute values of the e

272 NPNs were scattered throughout all nuclei of the BNC and had aspin

273 arent binding and cleavage defects are found scattered throughout both the coiled-coil and globular d

274 hotspot activity in each subunit and widely scattered throughout RecBCD.

275 brush) cells are solitary chemosensory cells scattered throughout the epithelia of the respiratory an

276 h soft, chalky calcite, that are irregularly scattered throughout the shell.

277 ility upon doping can be traced to increased scattering time for free charge carriers, indicating tha

278 axation time varies inversely with extrinsic scattering time.

279 the sensitivity of inelastic electron-light scattering to changes in the material dielectric functio

280 e utility of surface- and tip-enhanced Raman scattering to monitor individual bond-dissociation and b

281 We use neutron scattering to show that ferromagnetism and antiferromagn

282 Here we use inelastic neutron scattering to study magnetic fluctuations in the canonic

283 dynamic light scattering, small-angle x-ray scattering, tracer-based microrheology, and neutron spin

284 Scattering-type near-field optical microscopy (s-SNOM) i

285 , revealed by polariton interferometry using scattering-type scanning near-field optical microscopy (

286 imilar differentiation potential and forward scatter values, the cell complexity in wild type MSCs wa

287 rrelation spectroscopy and small angle X-ray scattering was confirmed by additional imaging with cryo

288 Small angle X-ray scattering was especially used to determine size paramet

289 The problem of low Raman scattering was overcome by trapping particles with 2D op

290 We use P-s scattered waves from the Moho as virtual sources to inve

291 phase behavior, we measured wide-angle x-ray scattering (WAXS) from oriented bilayers.

292 Using a QPI method that suppresses multiple scattering, we measured the dry mass content of individu

293 e, novel spectral fitting, and dynamic light scattering were combined to determine lateral lipid orga

294 om structural partial order inhibiting light scattering, while preserving mechanical stability, stiff

295 e method based on spectral small-angle X-ray scattering with a polychromatic beam for in vivo estimat

296 Neutron scattering with contrast variation provides direct evide

297 ts and were measured using spontaneous Raman scattering with narrowband continuous wave or nanosecond

298 efficient screening of charge carriers from scattering with other charge carriers, with charged defe

299 ractionation (FFF), UV, and multiangle light scattering) with subsequent chemical identification by o

300 lcium addition using rheology, dynamic light scattering, zeta potential, surface tension, and FTIR sp