ライフサイエンスコーパス: scattering

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

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

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

4 stent with interference of bulk and boundary scattering.

5 r of relative strength of single to multiple scattering.

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

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

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

9 honon anomalies in LSNO by inelastic neutron scattering.

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

11 correlated with phase breaking by polariton scattering.

12 nickel silicides using 3D medium-energy ion scattering.

13 d it plays a big role in electron and phonon scattering.

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

15 er vesicle size as measured by dynamic light scattering.

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

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

18 red (NIR) is beneficial due to reduced light scattering, absorption, phototoxicity, and autofluoresce

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

20 We identify scattering among axially spin-momentum locked states as

21 emented by spectroscopic, thermal, and x-ray scattering analyses.

22 ray crystal structures and small-angle X-ray scattering analysis of TDP2-Ub complexes reveal that the

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

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

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

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

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

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

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

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

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

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

33 X-ray scattering and ESI-MS revealed that Hf(18) is completely

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

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

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

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

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

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

40 chromatography coupled to multi-angle light scattering and native-state mass spectrometry of Yorkie

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 Using small-angle x-ray scattering and single-particle cryo-electron microscopy

44 These dual scattering and spectroscopy methods are used to demonstr

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

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

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

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

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

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

51 m, chaperone activity, and small-angle x-ray scattering) and in vivo tools (Caenorhabditis elegans sa

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

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

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

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

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

57 ic resonance spectroscopy, small-angle x-ray scattering, and multiscale simulations, we have uncovere

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

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

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

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

62 Rayleigh scattering, arising from frozen-in density fluctuations

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

64 Small-angle X-ray and neutron scattering, as well as cryo-electron microscopy, demonst

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

66 dynamic information contained in the diffuse scattering background.

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

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

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

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

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

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

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

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

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

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

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

78 Electron microscopy and small-angle X-ray scattering characterization confirm the formation of sin

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

95 such as single-crystal X-ray, dynamic light scattering (DLS), electron paramagnetic resonance (EPR),

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

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

98 ing Electron Microscopy (SEM), Dynamic Light Scattering (DLS), Nuclear Magnetic Resonance Spectroscop

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

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

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

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

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

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

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

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

107 cture determinations by the use of intrinsic scattering elements.

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

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

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

111 introduced, and fingerprints for the neutron-scattering experimental detection are provided.

112 Since scattering experiments and analytical calculations usual

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

114 Earlier neutron-scattering experiments on iron-based 123 ladder material

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

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

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

118 ical simulations benchmarked against neutron scattering experiments, we argue that the single-chain H

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

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

121 ise hydroxyapatite (such as wide angle X-ray scattering, Fourier-transform infrared spectroscopy and

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

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

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

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

126 ed light with efficiency up to 53% by single scattering from the water-air interface.

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

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

129 resolved grazing incidence small-angle X-ray scattering (GISAXS).

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

131 d through grazing incidence wide angle X-ray scattering (GIWAXS).

132 owever, the origin of macromolecular diffuse scattering has been poorly understood, limiting its appl

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

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

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

136 ieve high quality live-cell stimulated Raman scattering imaging on the basis of modified PDDA.

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

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

139 ests an important role of hyperbolic surface scattering in the damping process of hyperbolic phonon p

140 ton spectra expected from non-linear Compton scattering in the proposed LUXE experiment, showing high

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

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

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

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

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

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

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

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

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

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

151 Solvent scattering is a valuable internal reference for determin

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

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

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

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

156 Using multiangle light scattering (MALS), fluorescence lifetime imaging (FLIM),

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

158 romising for label-free imaging in optically scattering materials.

159 The scattering matrix we obtain from the experimental data d

160 al transport measurements, inelastic neutron scattering measurement, and first-principles calculation

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

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

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

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

165 Speckle contrast analysis of small-angle scattering measurements from nanoparticles reveals well-

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

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

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

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

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

171 nel through which energy is transmitted in a scattering medium(18).

172 ngle ultrashort laser pulse propagating in a scattering medium.

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

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

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

176 ne monomer concentration and interferometric scattering microscopy at the nanoparticle level.

177 Here, we use interferometric scattering microscopy to investigate a minimal acto-myos

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

179 Coherent anti-Stokes Raman scattering microscopy was used to statistically quantify

180 Stokes Raman scattering and stimulated Raman scattering modalities.

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

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

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

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

185 Strong scattering of phonon quasiparticles by anharmonicity and

186 Scattering of seismic waves can reveal subsurface struct

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

188 ispersing intensity comes from the inelastic scattering of the outgoing photoelectron.

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

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

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

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

193 (1.4%) and cytomegalovirus (6%), were rare, scattering over 12 months across all SOT recipients.

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

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

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

197 tigate the clinical implication of suspended scattering particles in motion (SSPiM) using optical coh

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

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

200 spectroscopic tools-resonant inelastic X-ray scattering, photoluminescence and optical absorption-to

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

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

203 number which show a relatively low electron scattering power.

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

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

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

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

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

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

210 Small-angle neutron scattering provides direct evidence for mesoscale magnet

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

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

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

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

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

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

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 Time-resolved resonant inelastic X-ray scattering (RIXS) is one of the developing techniques en

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

227 Here, in operando small-angle neutron scattering (SANS) is used to directly detect ion movemen

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

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

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

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

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

233 Here, we used Small Angle X-ray Scattering (SAXS) to investigate oligomerization of DnaA

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

253 ols that affect Earth's radiative balance by scattering solar radiation and serving as cloud condensa

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

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

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

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

258 A new application of stimulated Raman scattering (SRS) uses the benefit of a label-free molecu

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

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

261 Scattering strongly affects illumination and collection.

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

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

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

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

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

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

268 studied using spectroscopy, microscopy, and scattering techniques and was modeled numerically.

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

270 Light scattering techniques yield deep insights into the chang

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

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

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

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

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

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

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 al circuits in brain tissue, which is highly scattering to light.

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

282 We use neutron scattering to show that ferromagnetism and antiferromagn

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

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

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

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

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

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

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

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

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

295 Neutron scattering with contrast variation provides direct evide

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

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

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

299 ission spectroscopy (XES) and X-ray solution scattering (XSS).

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