ライフサイエンスコーパス: scatter

1 nce of porosity, exhibiting large amounts of scatter.

2 hich is transmitted to the adsorbate through scattering.

3 ng type- and energy-dependent charge carrier scattering.

4 drag thermopower-as well as enhancing phonon scattering.

5 tions upon phosphorylation by solution X-ray scattering.

6 to tissue due to significantly reduced light scattering.

7 fluorescence spectroscopy and dynamic light scattering.

8 ission electron microscopy and dynamic light scattering.

9 ass spectrometry, NMR, and small-angle X-ray scattering.

10 vel using solution NMR and small-angle x-ray scattering.

11 andgap and electrons suffer from severe back-scattering.

12 stors that switch based on the modulation of scattering.

13 r densities is dominated by Coulomb impurity scattering.

14 occurs, which does not participate in phonon scattering.

15 substrate to significantly reduce background scattering.

16 o organic thin films, thus reducing momentum scattering.

17 tion structure obtained by small-angle X-ray scattering.

18 , such as phase noises and spontaneous Raman scattering.

19 al spectroscopy and resonant inelastic X-ray scattering.

20 plain their substantial differences in light scattering.

21 elastic and quasi-elastic incoherent neutron scattering.

22 in both catalysis and surface-enhanced Raman scattering.

23 ocalized to two distinct foci; rather, it is scattered all around the nucleoid.

24 Zf-GRF X-ray structure and small-angle X-ray scattering analyses show that the Zf-GRF fold is typifie

25 ce of NEIL1 and DNA, while small-angle X-ray scattering analysis confirmed the NEIL1 mediated PCNA tr

26 In this latter case, stopped-flow light scattering analysis reveals the transport of water acros

27 Here we combined high-resolution X-ray scattering analysis with large-area Raman imaging, backs

28 The role of particle size-dependent Mie scattering and absorption efficiencies, and, scattering

29 Small angle neutron scattering and circular dichroism spectroscopy showed no

30 er is relatively high, such that collisional scattering and collision-induced dissociation are expect

31 in situ grazing-incidence small-angle X-ray scattering and complementary scanning tunneling microsco

32 In situ small/wide-angle X-ray scattering and electron microscopic measurements showed

33 ross a wide hydration range by neutron total scattering and empirical potential structure refinement

34 Small angle X-ray scattering and ensemble modeling yielded models of the P

35 mpact on spectroscopic methods such as Raman scattering and fluorescence detection in highly scatteri

36 By combining nanoFACS measurements of light scattering and fluorescence, we evaluated the sensitivit

37 rmined by numerical inversion of small angle scattering and isothermal magnetisation data.

38 poor understanding of phonon grain boundary scattering and its effect on thermal conductivity has im

39 iophysical analysis, using small angle X-ray scattering and multi-angle light scattering experiments,

40 Moreover, the study by dynamic light scattering and negative stain electron microscopy demons

41 rOPN were investigated by small-angle x-ray scattering and no significant changes were detected on t

42 terplay between time-dependent many-particle scattering and phase-space filling effects.

43 itu synchrotron-based small/wide angle X-ray scattering and photoluminescence (PL) probes, the NC-SL

44 dynamics simulations with experimental X-ray scattering and Raman spectroscopy data, we find that the

45 y simultaneous synchrotron small-angle X-ray scattering and Raman spectroscopy in a controlled gas-ph

46 3 films is determined using nuclear resonant scattering and Raman spectroscopy.

47 ectroscopy, FTIR spectroscopy, dynamic light scattering and scanning electron microscopy.

48 tract the contributions of electron-electron scattering and screening in different bands of different

49 plots exhibit larger coverage with less data scattering and significantly improved prediction bands a

50 aging in biological tissue by reducing light scattering and this has enabled accurate three-dimension

51 ion properties of probes using dynamic light scattering and transmission electron microscopy supports

52 l characterization using small-angle neutron scattering and X-ray diffraction.

53 of X-ray crystallography, small angle X-ray scattering, and complementary biophysical methods.

54 MR analyses with fluorescence, dynamic light scattering, and electron microscopy to elucidate how EGC

55 th and contraction and then cell deadhesion, scattering, and invasion.

56 bines magnetic tweezers, infrared evanescent scattering, and single-molecule FRET imaging, providing

57 mal titration calorimetry, small-angle X-ray scattering, and X-ray crystallography.

58 scanning electron microscopy, dynamic light scattering, and zeta potential analysis.

59 scattering and absorption efficiencies, and, scattering anisotropy are studied to identify the optima

60 ic fields, synchrotron emission, and Compton scattering are omnipresent in compact celestial X-ray so

61 Electron scattering at the device edge tends to bleed parasitic s

62 revealed matter-wave interference, haloes of scattered atoms, four-wave mixing and correlations betwe

63 crystal using a setup optimized for very low scattering background.

64 s is used to illuminate the tissue, with Mie scatter being detected by PIN photodiodes at eight diffe

65 spatial and temporal resolution deep within scattering brain tissues.

66 cross section when electromagnetic waves are scattered by an electrically small object.

67 ion limit, which is due primarily to optical scattering by brain tissues.

68 owth factor (HGF) induces cell migration and scattering by mechanisms that are thought to tip a local

69 nance and dielectric spectroscopies, neutron scattering, calorimetry, and ab initio calculations.

70 Here the authors show that Raman scattering can be used to measure magnetic excitations i

71 aging modalities, coherent anti-Stokes Raman scattering (CARS) and sum-frequency generation (SFG), we

72 EM) and multiplex coherent anti-Stokes Raman scattering (CARS) imaging via supercontinuum excitation

73 t arteries, using coherent anti-Stokes Raman scattering (CARS) microscopy and isotopic perfusion expe

74 mis, predominantly composed of CD3+ T cells, scattered CD20+ B cells, and relatively few PD-1+ (progr

75 nent in motor cranial nerve nuclei, and some scattered cells lie in the preoptic area and ventral par

76 ing (SPS), which introduce additional phonon scattering centers such as excess solid solution point d

77 , compressibility (1% relative uncertainty), scattering coefficients, and acoustic contrast factors f

78 ard-scattered intensity), and narrow forward scattering cone similar to giant clams.

79 of particular amino acids to enhance neutron scattering contrast, has the promise to become a powerfu

80 hile bulk investigations showed second-shell scattering contributions, indicating an inner-sphere sor

81 on and diffusion measurements, dynamic light scattering, controlled proteolysis, gel electrophoresis,

82 Potential inaccuracies in MRAC may affect scatter correction, because the attenuation image (mu-ma

83 The fluorophore scattering cross section is approximately 10-fold smalle

84 t of the polariton provides a finite Coulomb scattering cross section, such that the different types

85 6 orders of magnitude larger than the water scattering cross section.

86 al model for calculating fluorophore ORF and scattering cross sections has been developed that uses p

87 We compute the Rayleigh scattering cross sections of the nanoparticles by combin

88 Neutron-scattering curves showed only subtle changes in wall str

89 omplex was calculated from small-angle X-ray scattering data and was in good agreement with a model c

90 homopentamer) had solution small-angle X-ray scattering data consistent with the design models.

91 velope was calculated from small angle X-ray scattering data for the Bacillus subtilis glyQS T-box ri

92 mbining these results with small-angle X-ray scattering data for the complex of TRN-SR2 with truncate

93 continuum theories were used to analyze the scattering data from hexagonal arrays, revealing how the

94 On the basis of an analysis of scattering data from ten different metallic alloy liquid

95 nance energy transfer, and small-angle x-ray scattering data obtained under conditions when PANS are

96 americ form, combined with small-angle X-ray scattering data, allows the localisation of the B domain

97 ary structure information, small-angle X-ray scattering data, and any readily available tertiary cont

98 f soluble protein structure from small-angle scattering data, we construct a general multiphase model

99 ew possibilities for the analysis of Neutron scattering data.

100 bsorption spectroscopy and high-energy X-ray scattering demonstrate a correlation between the defect

101 liquid chromatography with evaporative light scattering detection.

102 e-exclusion chromatography-multi-angle light scattering, differential scanning fluorimetry, and isoth

103 lymerized and characterized by dynamic light scattering (DLS) and UV/Vis spectroscopy.

104 We use small-angle and total X-ray scattering, dynamic light scattering, transmission elect

105 eoretically model the importance of multiple scattering effects and computationally predict the impac

106 d by hyperbolic metamaterials with the light-scattering efficiency of PCs.

107 c quantities, and elastic incoherent neutron scattering (EINS) that probes local motions of a system

108 le scatter simulation (SSS) to calculate the scatter estimate.

109 ed by atom-atom distances from neutron total scattering experiments imply a substantial role for the

110 ally resolved second-order nonlinear optical scattering experiments on thiolate-protected gold cluste

111 HR-MAS (1)H NMR and neutron scattering experiments reveal that this macroscopic resp

112 se, we performed X-ray diffraction and Raman scattering experiments to benchmark our calculations and

113 Here we use scattering experiments to resolve the structure of a wid

114 lar dichroism spectroscopy and dynamic light scattering experiments verified that individual BSA mono

115 angle X-ray scattering and multi-angle light scattering experiments, revealed that ObgE is a monomer

116 Based on neutron total scattering experiments, we have determined that the loca

117 and motility factor Hepatocyte Growth Factor/Scatter Factor (HGF/SF) and its receptor, the product of

118 fect of polydispersity is to reduce the fine scattering features in the spectrum, resulting in a clos

119 nsity (heterogeneously or extremely dense vs scattered fibroglandular densities), first-degree family

120 istribution of wheat flour, photographed the scattered flour for 60 seconds every 10 seconds after si

121 to reveal GCs has led to a focus on multiply-scattered, fluorescence, two-photon, and phase imaging t

122 The absence of the axial scattering force and the enhanced gradient force enable

123 f 18.6 kBq/mL, and the count rate curves and scatter fraction curve were consistent for the alternati

124 Scatter fraction measured with a (68)Ge line source in t

125 ns using the following metrics: sensitivity, scatter fraction, contrast recovery, uniformity, count r

126 Scatter sinograms and scatter fractions did not reveal large differences regar

127 apped around a metallic cylinder, mimics the scattering from a predefined, arbitrarily-shaped dielect

128 in a manner consistent with the influence of scattering from acoustic and optical phonons.

129 Grazing incidence X-ray scattering from thin peptide films shows features of bet

130 They rely on Bragg scattering from wavelength-sized periodic modulation in

131 maging in semi-transparent specimens, tissue scattering has limited its application in the rodent bra

132 However, suppression of disorder-induced scattering has never been demonstrated in non-topologica

133 sults demonstrate that single-particle X-ray scattering has the potential to shed light on key biolog

134 By using small-angle x-ray scattering, high-resolution NMR spectroscopy, and limite

135 lla moellendorffii and Physcomitrella patens scattered in some clusters.

136 ed forward scattering with weakened backward scattering in plasmonic thin film solar cells.

137 same time, the analysis of coherent neutron scattering in the thermal and cold energy regimes reveal

138 ibute this to the enhanced electron-electron scattering in the unfilled d band of Ni.

139 Small angle X-ray scattering indicates that FP E244K is trapped in a compa

140 th on polarization conversion efficiency and scattering intensities.

141 less than approximately 0.01% of the forward-scattered intensity), and narrow forward scattering cone

142 ngth selectivity, have little loss (the back-scattering intensity is reduced to less than approximate

143 .74-2.75 A and an intense light-atom (C/N/O) scattering interaction 1.8 A from the Fe.

144 We demonstrate with HIV-1 TAR RNA that X-ray scattering interferometry (XSI) can be used to determine

145 bed in terms of matter waves, which can also scatter into the region of the geometrical shadow of the

146 The pump energy is scattered into the seed at an oblique angle with 14 J sr

147 of the core domain of p53 (p53C) using light scattering, intrinsic fluorescence, transmission electro

148 Elastic light scattering is a standard method to study aerosol particl

149 Electrophoretic light scattering is typically used to measure the zeta potenti

150 Already films with 60 microm-thick scattering layer feature a whiteness with a reflectance

151 ed as an additional proton barrier and light scattering layer.

152 Acoustic deep scattering layers (DSLs) are prominent features of the m

153 -lenses that can be reconfigured to focus or scatter light, form real or virtual images, and display

154 With their unique ability to concentrate and scatter light, plasmonic nanomaterials have been the foc

155 Here, we show that singly scattered light actually carries substantial information

156 The analysis of the scattered light allows in situ dynamic monitoring of the

157 modulated-intensity profile of elastic back-scattered light from an optically-trapped vesicle reveal

158 The scattered light from both beams is imaged onto the slit

159 full control over the phase and amplitude of scattered light is posing a great challenge.

160 By removing contributions from scattered light, we extract the dynamics of energy trans

161 ventional imaging-using predominately singly scattered light-to reveal GCs has led to a focus on mult

162 Multiple scattering limits the contrast in optical imaging of thi

163 odeling takes into account the radiation and scattering losses of the nano-sized probe neglected in p

164 nation (AF4) coupled to UV, multiangle light scattering (MALS) and differential refractive index (dRI

165 ons) of IDPs from a single small-angle x-ray scattering measurement.

166 Scatter measurements were used to measure and compare ba

167 A comparison with dynamic light scattering measurements indicates that each spike is ass

168 Raman scattering measurements of the order parameters independ

169 We examine the mobility-limiting scattering mechanisms by calculating temperature-depende

170 ull-field, and coherent imaging in optically scattering media in the fields of healthcare sciences, m

171 ve' is more akin to a chaotic propagation in scattering media, where light is driven out of coherence

172 ochromatic light transmission through highly scattering media.

173 ng stereology and coherent anti-Stokes Raman scattering microscopy.

174 l-length KGA and present a small-angle X-ray scattering model for full-length GLS2.

175 rit, which can be explained by a dislocation scattering model.

176 ry-Perot resonator, with pixels comprising a scattering nanopost on top of a distributed Bragg reflec

177 the complex in solution by small angle X-Ray scattering, nuclear magnetic resonance and surface-plasm

178 We furthermore quantify the scattering of an impact as a function of the local struc

179 by radiation, transmission, absorption, and scattering of electromagnetic waves.

180 ese results show that, by using the multiple scattering of light in a turbid medium, enhanced light-m

181 "color" white however relies on the multiple scattering of light within a randomly structured medium,

182 electrics, strategies typically focus on the scattering of low-frequency phonons by interfaces and hi

183 To separate the Raman scattering of the target gas molecules from the backgrou

184 In our experiment, the added impurities scatter off the much larger soliton, contributing to its

185 racentrifugation, NMR, and small-angle x-ray scattering on full-length ColN and its fragments.

186 We used neutron scattering on single crystals of alpha-RuCl3 to reconstr

187 e feedback is provided by amplified Rayleigh scattering on sub-micron refractive index inhomogenities

188 Here we use resonant inelastic X-ray scattering over a wide temperature range across the Verw

189 erse optimization problem for estimating the scattering parameters of a sample given its thickness an

190 rosol particles in the sense that a measured scattering pattern can be uniquely associated with the p

191 d a simple setup is introduced to obtain the scattering pattern of a tissue sample.

192 rameters of a sample given its thickness and scattering pattern.

193 Mie scatter patterns are collected at all photodiode angles

194 dictive power of the supervised learner, the scattering patterns are filtered, enriched by a regresso

195 s in a contact-free manner, wherein measured scattering patterns are interpreted to infer particle mo

196 ously to obtain the ultra-wideband diffusion scattering patterns.

197 rix elements or near the Raleigh and Compton scattering peaks of the X-ray source (molybdenum anode).

198 on measured with a (68)Ge line source in the scatter phantom was stable within the range of 40.4%-40.

199 tion of phonon standing wave amplitudes, the scattering phase shifts, and the nonlinear intermode cou

200 eoretical transport studies show that phonon scattering plays a significant role in microscopic condu

201 Here we introduce a scatter plot tool (AAScatterPlot) that easily shows the

202 We find that the resolution of the Rayleigh scattering probe is adequate to detect nanoparticles as

203 pin texture and the polarized resonant X-ray scattering process.

204 The radar forward-scattering properties of different reflection sites are

205 ieves errors of roughly 5% in predicting the scattering properties of many biological tissues.

206 that exploit the fluorophore ORF and photon scattering properties.

207 Quasi-elastic neutron scattering provided quantitative details about the dynam

208 Fermi liquid state survives-however, with a scattering rate close to the maximal value allowed.

209 Despite this, the scattering rate exhibits a T (2) dependence, which shows

210 e text] is a microscopic momentum-preserving scattering rate.

211 ty in GNRs by affecting the carrier momentum scattering rate.

212 n in hot carrier solar cells.Carrier-carrier scattering rates determine the fundamental limits of car

213 luences and report the dependence of carrier scattering rates on excess energy and carrier density.

214 ate differences in the longitudinal and Hall scattering rates, which is a non-Fermi liquid phenomenon

215 ttering and fluorescence detection in highly scattering regimes.

216 riments performed by resonance elastic light scattering (RELS) confirmed MT swelling/shrinking, ion d

217 ve existed much earlier, and there have been scattered reports of putative angiosperms from Triassic

218 We found that increasing the strength of the scattering resonance causes the increase of the condensa

219 gly depend on the presence of defect-induced scattering resonance.

220 n-glass electron-crystal", multiscale phonon scattering, resonant states, anharmonicity, etc.

221 with the importance of short-range impurity scattering resulting in a "universal" density-independen

222 From a combination of batch and flow light scattering results, we concluded that the passage flow v

223 ctroscopy (XES) and resonant inelastic X-ray scattering (RIXS).

224 esent biosensor was based on resonance light scattering (RLS) using magnetic nanoparticles (MNPs) as

225 Small-angle X-ray scattering (SAXS) also indicates that the cortactin repe

226 ssenger domain obtained by small-angle X-ray scattering (SAXS) analysis.

227 s of MotB fragments to the small angle X-ray scattering (SAXS) data revealed that the protein's C-ter

228 ultimers, consideration of small-angle X-ray scattering (SAXS) data, and location of heparin-binding

229 the dimerization curve in small-angle X-ray scattering (SAXS) experiments using isolated GluA2 ligan

230 spectroscopy (XPCS) in the small-angle X-ray scattering (SAXS) geometry to probe both the structural

231 Small-angle X-ray scattering (SAXS) measurements reveal a striking differe

232 particle dual-mode total internal reflection scattering (SD-TIRS) with a transmission grating (TG).

233 nditions by thioflavin T fluorescence, light scattering, SDS stability, and atomic force microscopy.

234 n chromatography with multiangle laser light scattering (SEC-MALLS) experiments showed that CodY is a

235 Surface enhanced hyper Raman scattering (SEHRS) is the spontaneous, two-photon excite

236 t-effective, portable surface enhanced Raman scattering (SERS) approach for the routine analysis of u

237 Surface enhanced Raman scattering (SERS) is an analytical technique which has g

238 Surface-enhanced Raman scattering (SERS) spectroscopy has evolved into a cross-

239 Surface Enhanced Raman Scattering (SERS) supported by gold nanoparticles (AuNPs

240 n techniques, such as surface-enhanced Raman scattering (SERS), allows for rapid separation, identifi

241 scopy correlated with surface enhanced Raman scattering (SERS).

242 Small-angle X-ray scattering showed that certain sequences can form well-o

243 e-to-one correspondence between the measured scattering signal and the winding number.

244 owth of a metal layer to further enhance the scattering signal.

245 ure tracking to amplifying weak normal Raman scattering signals.

246 s, including mode confinement, polarization, scattering signature, and crosstalk, which are critical

247 attenuation image (mu-map) is used in single scatter simulation (SSS) to calculate the scatter estima

248 "Dust" is formed by scattered single cells alternating with macrophages.

249 biophysical measurements (small-angle X-ray scattering, single-molecule fluorescence resonance energ

250 Scatter sinograms and scatter fractions did not reveal l

251 Positive light scatter specimens were used for downstream rapid matrix-

252 Mie scatter spectra can be detected within a few seconds wit

253 he incident light angles, resulting in a Mie scatter spectra.

254 From neutron scattering spectra, we confirmed that the B. subtilis ce

255 om the analysis of the time-domain Brillouin scattering spectra.

256 Vibrational sum-frequency scattering spectroscopy (VSFSS) is used to measure the v

257 FTIR and wide-angle X-ray scattering spectroscopy also indicated that NaOH steepin

258 Stimulated Raman scattering (SRS) describes a family of techniques first

259 erging analytical technique stimulated Raman scattering (SRS) microscopy promises a solution, as it c

260 determined a conjoined NMR-small angle x-ray scattering structure of the EV71 SLII domain and a mutan

261 These small angle X-ray scattering studies indicated that GstDnaBFL has an elong

262 Through small-angle X-ray scattering studies of sTie2 dimers in solution and model

263 Small angle X-ray scattering studies show that the 'Open' form of the prot

264 icroscopy, calorimetry and small angle X-ray scattering studies.

265 In this paper, we report a small/wide angle scattering study of wellbore cement that has been expose

266 a thorough single-crystal inelastic neutron scattering study, we demonstrate that nearest-neighbour

267 sceptibility testing straight from the light scatter suspension might provide dramatic improvement in

268 Light scatter technology has been proposed for several years a

269 uencies, lead to new laws of electromagnetic scattering that allow cross sections to be decoupled fro

270 l result regarding nonlinear inverse Thomson scattering that clearly shows an annular intensity distr

271 gin of this dependence is largely due to the scattering that depends on morphology and not absorbance

272 is the spontaneous, two-photon excited Raman scattering that occurs for molecules residing in high lo

273 onstrated that dislocations are effective at scattering the remaining mid-frequency phonons as well.

274 Despite the elastic nature of Rayleigh scattering, the feedback mechanism has been insofar deem

275 ions of the nanoparticles by combining light scattering theory for gas-particle mixtures with calcula

276 In the steady state, we find individual GMPs scattered throughout the bone marrow.

277 hich are a few kilobases in size, and widely scattered throughout the genome, coldspots have a median

278 We have developed third-harmonic scattering (THS) as an alternative method to measure gam

279 interferometry for label-free 3D imaging in scattering tissue.

280 Here we use resonant inelastic X-ray scattering to follow the evolution of charge correlation

281 noparticles in whole tissues can amplify the scattering to produce a 1.4 million-fold greater photon

282 reservoir temporarily emptied by stimulated scattering to the condensate, generating ultrashort puls

283 use nano- to millisecond time-resolved X-ray scattering to visualize the solution structural changes

284 scopy, cryo-electron microscopy, and neutron scattering, to investigate the formation of membrane sta

285 le and total X-ray scattering, dynamic light scattering, transmission electron microscopy, and a sing

286 lthough infrared GPs have been visualized by scattering-type scanning near-field optical microscopy (

287 Here we use stimulated Raman scattering under electronic pre-resonance conditions to

288 zation occurs dominantly via carrier-carrier scattering under the investigated fluences and report th

289 ium of this enzyme using small-angle neutron scattering, under conditions where we are able to contro

290 Here we combine wide-angle X-ray scattering (WAXS) with X-ray photon-correlation spectros

291 Using multi-angle light scattering, we determined that BAM2 was a tetramer, wher

292 titration calorimetry, and small-angle X-ray scattering, we show that in the homodimeric state, the O

293 croscopy and time-resolved small-angle X-ray scattering, we show that lipopolysaccharides (LPS) form

294 n BeH2 and LiBeH3 using quasielastic neutron scattering, which is especially sensitive to single-part

295 topological insulator ribbons accounting for scattering with phonons and imperfections.

296 ovides a concept to achieve enhanced forward scattering with weakened backward scattering in plasmoni

297 large pore membranes and using dynamic light scattering, with excellent agreement between values meas

298 fragments of laminar crustacean cuticle are scattered within the coprolite contents and suggest that

299 g dimensions of generic operators describing scattering within multi-channel Luttinger liquid.

300 py as a novel means to use internal electron scattering within the molecular reference frame to obtai