ライフサイエンスコーパス: scattering

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

2 drag thermopower-as well as enhancing phonon scattering.

3 tions upon phosphorylation by solution X-ray scattering.

4 to tissue due to significantly reduced light scattering.

5 fluorescence spectroscopy and dynamic light scattering.

6 ission electron microscopy and dynamic light scattering.

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

8 andgap and electrons suffer from severe back-scattering.

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

10 stors that switch based on the modulation of scattering.

11 r densities is dominated by Coulomb impurity scattering.

12 occurs, which does not participate in phonon scattering.

13 substrate to significantly reduce background scattering.

14 o organic thin films, thus reducing momentum scattering.

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

16 sonance spectroscopy and small-angle neutron scattering.

17 of the strong enhancement of the Raman light scattering.

18 ver no pore was detected by neutron in-plane scattering.

19 x with a tRNA precursor by small-angle X-ray scattering.

20 , such as phase noises and spontaneous Raman scattering.

21 al spectroscopy and resonant inelastic X-ray scattering.

22 plain their substantial differences in light scattering.

23 elastic and quasi-elastic incoherent neutron scattering.

24 in both catalysis and surface-enhanced Raman scattering.

25 hich is transmitted to the adsorbate through scattering.

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

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

28 apered molecular "shapes." Small-angle X-ray scattering analysis of the self-assembled structures ill

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

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

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

32 Small angle neutron scattering and circular dichroism spectroscopy showed no

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

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

35 has been achieved mainly by enhancing phonon scattering and consequently decreasing the thermal condu

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

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

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

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

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

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

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

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

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

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

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

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

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

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

50 3 films is determined using nuclear resonant scattering and Raman spectroscopy.

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

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

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

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

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

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

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

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

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

60 e using mass spectrometry, small-angle X-ray scattering, and negative-stain electron microscopy at ne

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

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

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

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

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

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

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

68 erpretation that the I dc serves to suppress scattering between states near the Fermi level in a stro

69 spatial and temporal resolution deep within scattering brain tissues.

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

71 amounts of heat in these materials, despite scattering by electron-phonon interactions, due to the h

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

73 Phonon scattering by nanostructures and point defects has becom

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

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

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

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

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

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

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

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

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

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

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

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

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

87 6 orders of magnitude larger than the water scattering cross section.

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

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

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

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

92 as accurately modeled from small-angle x-ray scattering data by treating ColN as a flexible system, n

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

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

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

96 Scattering data from aligned flagellar bundles confirmed

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

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

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

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

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

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

103 ew possibilities for the analysis of Neutron scattering data.

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

105 liquid chromatography with evaporative light scattering detection.

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

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

108 mechanical properties, whereas dynamic light scattering (DLS)and transmission electron microscopy (TE

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

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

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

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

113 During the scattering event, the momentum [Formula: see text] is tr

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

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

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

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

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

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

120 al neutron diffraction and inelastic neutron scattering experiments we shed light on this issue in th

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

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

123 separation of the fluorophore ORF and photon scattering features in the fluorophore resonance synchro

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

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

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

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

128 estigate plasmonic resonance driven enhanced scattering from microinclusions of low-bandgap semicondu

129 The increased forward scattering from nanoscale objects at this short waveleng

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

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

132 y in situ grazing incidence wide-angle X-ray scattering (GIWAXS) and optical reflectance, to better u

133 y XRD and grazing-incidence wide-angle X-ray scattering (GIWAXS) measurements.

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

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

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

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

138 The local impurity scattering in arbitrary configuration of conducting and

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

140 ray crystallography and by small-angle X-ray scattering in solution as well as that of its complex wi

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

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

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

144 th on polarization conversion efficiency and scattering intensities.

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

146 .74-2.75 A and an intense light-atom (C/N/O) scattering interaction 1.8 A from the Fe.

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

148 X-ray scattering interferometry (XSI) is based on site-specifi

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

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

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

152 X-ray scattering is uniquely suited to the study of disordered

153 stribution, as measured by neutron inelastic scattering, is only slightly altered.

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

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

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

157 Multiple scattering limits the contrast in optical imaging of thi

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

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

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

161 f-flight quasi-elastic and inelastic neutron scattering measurements in a wide energy window ranging

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

163 neutron diffraction and small-angle neutron scattering measurements of adsorbed CO2 in Marcellus Sha

164 Raman scattering measurements of the order parameters independ

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

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

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

168 ochromatic light transmission through highly scattering media.

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

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

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

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

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

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

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

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

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

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

179 In this work, we discovered that light scattering of metal nanoparticles can provide 3D imaging

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

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

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

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

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

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

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

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

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

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

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

191 ormation on protein dynamics via the diffuse scattering patterns that are overlaid with Bragg diffrac

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

193 he theoretically predicated structure-factor scattering peak line shape.

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

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

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

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

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

199 rpretation of experimental small-angle X-ray scattering profiles of these systems, which changes how

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

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

202 that exploit the fluorophore ORF and photon scattering properties.

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

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

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

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

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

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

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

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

211 e SiGe alloys with ab-initio electron-phonon scattering rates.

212 ttering and fluorescence detection in highly scattering regimes.

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

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

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

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

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

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

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

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

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

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

223 Using small-angle X-ray scattering (SAXS) and electron microscopy averaging, we

224 r was then refined against small-angle X-ray scattering (SAXS) data employing an established method (

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

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

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

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

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

230 The low-resolution small angle X-ray scattering (SAXS) results show that the N-terminal exten

231 We demonstrate by small-angle X-ray scattering (SAXS) that HMBPP binding to the internal dom

232 tructs in combination with small angle X-ray scattering (SAXS) to determine the structure of the main

233 rting by NMR, rheology and small angle X-ray scattering (SAXS).

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

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

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

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

238 ositions of surface-enhanced resonance Raman scattering (SERRS) nanoparticles make them promising con

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

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

241 Surface enhanced Raman scattering (SERS) nanoparticles are an attractive altern

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

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

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

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

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

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

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

249 ure tracking to amplifying weak normal Raman scattering signals.

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

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

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

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

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

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

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

257 the potential of employing stimulated Raman scattering (SRS) imaging to probe for metabolic differen

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

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

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

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

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

263 scopy (EM) and small-angle X-ray and neutron-scattering studies.

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 d on which responsive surface-enhanced Raman scattering substrates with spatially homogeneous hot spo

268 In this respect, tip-enhanced Raman scattering (TERS) has been demonstrated to be ideally su

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 tion and using the Beckman-Kirchhoff surface scattering theory with shadowing to precisely describe p

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

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

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

280 id bilayers, we employed Small Angle Neutron Scattering to probe lipid distribution across bilayer le

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 Using in situ small-angle X-ray scattering, we observe continuous growth of individual n

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

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

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

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

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

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

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