ライフサイエンスコーパス: ray

1 thiazole unit, and characterized by single X-ray.

2 cross the entire lengths of regenerating fin rays.

3 remain exposed to reflected and indirect UV rays.

4 , 7.7 years) using anthropometric and dual X-ray absorptiometry (DXA) measurements.

5 from baseline in areal BMD by dual-energy x-ray absorptiometry at the total hip through month 12 (me

6 anada, referred for a baseline dual-energy x-ray absorptiometry scan from January 1, 1996, to March 2

7 Measures of dual-energy X-ray absorptiometry-derived fat mass included the limb-to

8 BMC, and body composition via dual-energy x-ray absorptiometry.

9 ption, resonance Raman, (1)H NMR, EPR, and X-ray absorption (near-edge) spectroscopy, ESI mass spectr

10 Low X-ray absorption contrast in non-mineralised tissue can be

11 polar contributions in the uranium L3-edge X-ray absorption cross section to provide unique informati

12 ntermediate using Fe- and Mn-edge extended X-ray absorption fine structure (EXAFS) analysis and multi

13 Linear combination fitting of extended X-ray absorption fine structure (EXAFS) data using referen

14 Transmission electron microscopy and x-ray absorption fine structure analysis confirm similar p

15 The in situ extended X-ray absorption fine structure analysis shows a Ru horizo

16 s investigated by direct monitoring of the X-ray absorption fine structure of the catalyst, coupled w

17 Extended X-ray absorption fine-structure spectroscopy showed red am

18 ntrary to formulation, was confirmed using X-ray absorption near edge spectroscopy, suggesting substi

19 rated that the U M4 high energy resolution X-ray absorption near edge structure (HR-XANES) method is

20 Synchrotron-based X-ray absorption near-edge structure (XANES) spectroscopy

21 X-ray absorption spectra indicated that U(IV) in both hema

22 higher Mo loadings, indicated by Mo K-edge X-ray absorption spectra.

23 able by chemical extractions, Mossbauer or X-ray Absorption spectroscopies.

24 Here, X-ray absorption spectroscopy (XAS) and rR studies have be

25 X-ray absorption spectroscopy (XAS) is an electronic absor

26 Hg(II) biouptake pathway, we have employed X-ray absorption spectroscopy (XAS) to investigate the rel

27 nance (EPR), SQUID, UV-vis absorption, and X-ray absorption spectroscopy (XAS)) coupled with advanced

28 X-ray absorption spectroscopy and high-energy X-ray scatte

29 X-ray absorption spectroscopy and X-ray photoelectron spec

30 o(II) to Co(III), as evidenced by operando X-ray absorption spectroscopy at the Co K-edge.

31 Spatially resolved X-ray absorption spectroscopy documented a reduction of th

32 the co-localization results to iron K-edge X-ray absorption spectroscopy fitting results allowed to q

33 In operando X-ray absorption spectroscopy identified reduced Pt covere

34 X-ray absorption spectroscopy provides firm evidence for t

35 ion electron microscopy (TEM) and operando X-ray absorption spectroscopy showed that oxygen species c

36 We used X-ray absorption spectroscopy to characterize the structur

37 Analysis of chemical reactivity, in situ X-ray absorption spectroscopy, and density functional theo

38 nsmission electron microscopy and operando X-ray absorption structures to study the mechanical proper

39 X-ray absorption studies of the geometric and electronic s

40 t the element and site selectivity of soft X-ray absorption to sensitively follow the ultrafast pipi*

41 X-ray radiotherapy on cancer treatment and X-ray activated Cu-Cy nanoparticles can be efficiently des

42 onship and promote a rational synthesis of X-ray amorphous IrOx hydroxides that contain a favorable a

43 tron microscopy (HRTEM), energy dispersive X-ray analysis (EDX), atomic force microscopy (AFM), scann

44 chemistry was unequivocally established by X-ray analysis of precursor trans-(+)-5a as camphorsulfony

45 roscopic data as well as by single crystal X-ray analysis.

46 ogen concentrations observed by Dawn's Gamma Ray and Neutron Detector to assess potential volatile oc

47 that explains the seemingly contradictory X-ray and NMR data.

48 Conventional optical, X-ray and photoelectron probes often fail to provide inter

49 ight curve of GW170817, as well as the gamma-ray and X-ray emission (and possibly also the ultraviole

50 Moreover, extension of the digit rays and the patterning of the joints occur simultaneous

51 beams in the extreme ultraviolet (XUV) or X-ray, and controlling the OAM on these beams remains chal

52 Using simultaneous infrared, optical, x-ray, and radio observations of the Galactic black hole s

53 Sharks, rays, and chimaeras (Class Chondrichthyes; herein 'shark

54 is estimated that one-quarter of sharks and rays are threatened worldwide and although the global fi

55 Synchrotron mu-X-ray based techniques combined with mu-Raman spectroscopy

56 arger than 1 mum(3) in volume, whereas the X-ray beam is often attenuated to protect the detector fro

57 hat a three order of magnitude increase in X-ray brightness and over an order of magnitude increase i

58 rightening in the afterglow of a short gamma-ray burst at redshift z = 0.356, although findings indic

59 intense flashes of gamma-rays known as gamma-ray bursts (GRBs), followed by longer-lived afterglow ra

60 0817 are dissimilar to classical short gamma-ray bursts with ultrarelativistic jets.

61 Here we present NMR and X-ray characterization for the two classes of these inhibi

62 ell line panel and allowed us to obtain an X-ray co-crystal structure of the synthetic secondary meta

63 competitive with acetyl coenzyme A and an X-ray cocrystal structure reveals that binding is biased t

64 n emission computed tomography (SPECT) and X-ray computed tomography (CT) for investigating transport

65 X-ray computed tomography (CT) is a powerful noninvasive t

66 d 38.2%, 51.9%, and 36.3% of which contain X-ray, computed tomography (CT) scan, and genomic data, re

67 X-ray crystal structure analysis of both Rh complexes form

68 6 is described and rationalized using the X-ray crystal structure of 6 bound to human IDO-1, which s

69 C-F...H-C interaction was observed in the X-ray crystal structure of a fluorinated triterpenoid.

70 We report a 3.4-A resolution X-ray crystal structure of a sigma(N) fragment in complex

71 Here, we have solved the X-ray crystal structure of an EBNA1 DNA-binding domain (DB

72 An X-ray crystal structure of caspase-7 bound to a fragment h

73 Here we report the 2.7-A X-ray crystal structure of MazF-mt6.

74 We present here the X-ray crystal structure of the ADAM10 ectodomain, which, t

75 ed by a templated clipping reaction and an X-ray crystal structure shows that the squaraine gem-dimet

76 e highly organized capsules is shown by an X-ray crystal structure which features the assembly of two

77 This questions whether the available x-ray crystal structures of EPOR truly represent active or

78 Previous X-ray crystal structures of Nef in complex with key host c

79 The X-ray crystal structures of two active complexes are repor

80 X-ray crystal structures were obtained for five of the des

81 These complexes could be characterized by X-ray crystallographic analysis and employed as catalysts

82 egrees that was unambiguously confirmed by X-ray crystallographic analysis.

83 This article describes X-ray crystallographic and solution-state NMR studies of p

84 Here, we determined the X-ray crystallographic structures of two catalytically ina

85 ioinformatic, biochemical, mutational, and X-ray crystallographic studies on the unicellular alga Chl

86 This first X-ray crystallographic study of a single human CCT subunit

87 Serial X-ray crystallography allows macromolecular structure dete

88 Conventional structural methods such as X-ray crystallography and cryo-transmission electron micro

89 he CL40 and CL59 complexes with gHgL using X-ray crystallography and EM to identify their epitope loc

90 We report the low pH characterization by X-ray crystallography and EPR spectroscopy of the nitrogen

91 strictly on experimental evidence, such as X-ray crystallography and nuclear magnetic resonance (prim

92 While X-ray crystallography and nuclear magnetic resonance spect

93 nd the IgG1 CH3 homodimer was evidenced by X-ray crystallography and used to engineer examples of bsA

94 EM) can circumvent some of the problems of x-ray crystallography as a pipeline for obtaining the requ

95 X-ray crystallography confirms they have the fluorite stru

96 Protein X-ray crystallography established that 3-unsubstituted 2,4

97 ynamic regions that proved unresolvable by X-ray crystallography in homologous receptors.

98 analyzing dynamics of crystalline proteins.X-ray crystallography is the main method for protein struc

99 However, X-ray crystallography of these intermediates is severely h

100 An X-ray crystallography study of the rabbit muscle GPb inhib

101 hod for protein structure determination is X-ray crystallography which relies on the availability of

102 on NMR relaxation dispersion measurements, X-ray crystallography, and structure-based chemical shift

103 BDD) guided by structural information from X-ray crystallography, computational studies, and NMR solu

104 e shown to possess a novel binding mode by X-ray crystallography, in which the triazolo N1 atom coord

105 Here, we combine X-ray crystallography, native mass spectrometry, single-ch

106 Freeze-trapping x-ray crystallography, nuclear magnetic resonance, and com

107 By combination of X-ray crystallography, SAXS and EM, together with biochemi

108 ully characterized by NMR spectroscopy and X-ray crystallography.

109 ed, and its stereochemistry established by X-ray crystallography.

110 Structures of 1 and 2 are confirmed by X-ray crystallography.

111 nd NMR spectroscopy, DFT calculations, and X-ray crystallography.

112 tions, which is most commonly performed by X-ray crystallography.

113 dosobenzene-metal adducts characterized by X-ray crystallography.

114 y, IR spectroscopy, mass spectrometry, and X-ray crystallography.

115 rimetry, small-angle X-ray scattering, and X-ray crystallography.

116 racterized by spectroscopic studies and by X-ray crystallography.

117 posed on the basis of NMR spectroscopy and X-ray crystallography.

118 Guided by microscale X-ray CT, nanoscale X-ray CT is used to investigate the size and morphology of

119 Guided by microscale X-ray CT, nanoscale X-ray CT is used to investigate the si

120 The X-ray data show how Tyr34 maintains solvent exclusion and

121 d on previously published 3.8-A resolution X-ray data.

122 ron microscopy (SEM), UV-Vis spectroscopy, X-ray diffraction (XRD) analysis and Fourier transform inf

123 melting curve in molybdenum by synchrotron X-ray diffraction analysis of crystalline microstructures,

124 In situ X-ray diffraction analysis reveals that the material under

125 X-ray diffraction analysis showed that calcium carbonate i

126 In situ single-crystal X-ray diffraction analysis was carried out at 298 K using

127 rotein ternary adduct was characterized by X-ray diffraction analysis.

128 complex was prepared and characterized by X-ray diffraction analysis.

129 zed by multinuclear NMR and single-crystal X-ray diffraction analysis.

130 included transmission electron microscopy, X-ray diffraction and asymmetrical flow field-flow fractio

131 X-ray diffraction and reciprocal space maps identify the i

132 ent materials quality, as characterized by X-ray diffraction and surface area analysis.

133 Through X-ray diffraction and X-ray photoelectron spectroscopy, th

134 We used low-angle x-ray diffraction at the European Synchrotron Radiation Fa

135 Single-crystal X-ray diffraction confirmed structures that resemble a spi

136 TTPA was crystallized and X-ray diffraction data were collected to a resolution of 1

137 e mechanics and micrometer-nanometer-scale X-ray diffraction from synchrotron light in intact ventric

138 orders of magnitude of sharp increases in X-ray diffraction intensity.

139 synchrotron radiation-based high-pressure X-ray diffraction is used to quantify the influence of dre

140 X-ray diffraction of precipitates showed that Mnt interlay

141 lectron microscopy, UV-Visible spectra and X-ray diffraction pattern.

142 Here, utilizing the synchrotron X-ray diffraction technique, we for the first time, experi

143 cluding synchrotron-based grazing incident X-ray diffraction to observe crystal structure and chemica

144 nalysis (fwhm) was performed on the powder X-ray diffraction traces and showed that the higher concen

145 X-ray diffraction tracks the light-induced femtosecond coh

146 roscopy and low-temperature single-crystal X-ray diffraction, and in the gas phase by quantum-chemica

147 omprehensive structural characterizations (X-ray diffraction, electron microscopy, Raman, and UV-visi

148 ome structure has been confirmed by powder X-ray diffraction, high-resolution transmission electron m

149 Via 2D X-ray diffraction, highly ordered and textured crystals fo

150 By combining x-ray diffraction, molecular dynamics simulations, and ele

151 rized by transmission electron microscopy, X-ray diffraction, Raman spectroscopy, X-ray photoelectron

152 by in situ time-resolved synchrotron-based X-ray diffraction, remarkably agreeing with the sorption i

153 was analyzed for polymorphism using powder X-ray diffraction, solid fat content by pulsed nuclear mag

154 ture and purity were verified using powder X-ray diffraction, transmission electron microscopy, Raman

155 n situ high-pressure synchrotron radiation X-ray diffraction, we reveal a polymorphic transition from

156 nd polymer single crystals are analyzed by X-ray diffraction, which is the first case of a scsc two-d

157 atomic force microscopy, grazing incident X-ray diffraction, X-ray photoelectron spectroscopy, and F

158 Fe Mossbauer, magnetometry, single crystal X-ray diffraction, XAS, and EXAFS for 6.

159 wed by in situ variable temperature powder X-ray diffraction.

160 ries were analyzed using synchrotron-based X-ray diffraction.

161 ulose were detected by NMR and synchrotron X-ray diffraction.

162 n of a mammalian mitochondrion by coherent x-ray diffractive imaging (CXDI) using synchrotron radiati

163 -up of 3.1+/-1.6 years, 939 had at least 1 x-ray during the follow-up period.

164 molybdopterin cofactors, in a variant of the Ray-Dutt twist of classical coordination chemistry, whic

165 of GW170817, as well as the gamma-ray and X-ray emission (and possibly also the ultraviolet and opti

166 an all-optical scheme for ultra-bright gamma-ray emission and dense positron production with lasers a

167 ting black hole or neutron star often show x-ray emission extending to high energies (>10 kilo--elect

168 remely energetic and long-lived prompt gamma-ray emission from GRB 160625B.

169 the compounds were measured using variable X-ray energies in the vicinity of the U L3 edge in the TXR

170 sfer maximizes the XRS signal at the given X-ray energy and enhances nondipole contributions compared

171 Mechanistic and X-ray evidence is presented that supports that the reactio

172 X-ray fibre diffraction, hydrogen-deuterium exchange and s

173 terygian subgroup, the acanthomorph or spiny-rayed fishes.

174 y, it is found in both cases that incident X-ray fluences then restore the [Fe{H2 B(pz)2 }2 (bipy)] m

175 with a low power benchtop total reflection X-ray fluorescence (TXRF) system has been developed for mu

176 X-ray fluorescence (XRF) microscopy, quantified with eleme

177 X-ray fluorescence imaging of pinna cross-sections reveale

178 of gadolinium retention in the tibia with x-ray fluorescence in a laboratory at McMaster University.

179 Grazing incidence and grazing emission X-ray fluorescence spectroscopy (GI/GE-XRF) are techniques

180 omolecular structure determination at both X-ray free electron lasers (XFELs) and, more recently, syn

181 hy of biological objects-an application of X-ray free-electron lasers that greatly enhances our abili

182 field causes an increase in galactic cosmic ray (GCR) flux.

183 ically shielding skin from direct harmful UV rays; however, skin may still remain exposed to reflecte

184 Here we use 2D and 3D X-ray imagery on Noril'sk nickel sulfide, combined with si

185 nstrated by reconstructing neutron and gamma-ray images.

186 sicrystals, we performed synchrotron-based X-ray imaging experiments on a decagonal phase with compos

187 e temperatures characteristic of light- or X-ray-induced excited-spin-state trapping.

188 -phenylpyridine) and their applications in X-ray-induced photodynamic therapy (X-PDT) of colon cancer

189 We used energy-sampling and rapid-scan X-ray Kbeta emission and K-edge absorption spectroscopy as

190 r prompt, brief and intense flashes of gamma-rays known as gamma-ray bursts (GRBs), followed by longe

191 Using x-ray magnetic circular and linear dichroism techniques, w

192 en 5f and 6d electronic states by means of X-ray magnetic circular dichroism.

193 visualization study using fast synchrotron X-ray micro-tomography to provide new insights into these

194 In vivo x-ray microcomputed tomography of dehydrating leaves of fo

195 is investigated here using the synchrotron X-ray microdiffraction.

196 A combination of synchrotron based X-ray microprobe and bulk techniques was used to study the

197 Complementary scanning transmission X-ray microscopy revealed that these aggregates are strong

198 ercolation of metallic melt is provided by X-ray microtomography of primitive achondrite Northwest Af

199 ColN-T is invisible in the high-resolution x-ray model and yet accounts for 90 of the toxin's 387 ami

200 Synchrotron X-ray nanofluorescence was applied to map the trace elemen

201 , implementation of synchrotron-based hard X-ray nanotomography in Al-Cu alloys to measure kinetics o

202 irst time an InGaP (GaInP) photon counting X-ray photodiode has been developed and shown to be suitab

203 nd cluster packing on both supports, while x-ray photoelectron and absorption spectroscopy demonstrat

204 Using near-ambient pressure X-ray photoelectron spectroscopy (NAP-XPS) we show that a

205 glassy carbon electrode (GCE), as shown by X-ray photoelectron spectroscopy (XPS) measurements.

206 erized by UV, circular dichroism (CD), and X-ray photoelectron spectroscopy (XPS).

207 eory calculations and further confirmed by X-ray photoelectron spectroscopy analysis.

208 us gating voltage regions, as confirmed by X-ray photoelectron spectroscopy and atomic force microsco

209 X-ray photoelectron spectroscopy reveals that, at pH </= 3

210 atalyst during the reaction, quasi in situ X-ray photoelectron spectroscopy showed that the surface i

211 X-ray absorption spectroscopy and X-ray photoelectron spectroscopy studies of SNNO/LSMO hete

212 scopy, grazing incident X-ray diffraction, X-ray photoelectron spectroscopy, and Fourier transform in

213 Through X-ray diffraction and X-ray photoelectron spectroscopy, the as-grown tungsten(VI

214 py, X-ray diffraction, Raman spectroscopy, X-ray photoelectron spectroscopy, UV-vis absorption spectr

215 and over an order of magnitude increase in X-ray photon energy is achieved by passing a 3 GeV electro

216 ne wide-angle X-ray scattering (WAXS) with X-ray photon-correlation spectroscopy (XPCS) in the small-

217 <100>, <111>, and <751> orientations using X-ray pole figures.

218 Through synchrotron x-ray powder diffraction and tomography measurements, uran

219 n dispersive spectrum elemental line scan, X-ray powder diffractions and Raman spectroscopy.

220 photon energies of 8.3 kiloelectronvolts) X-ray pulses is qualitatively different: our experimental

221 into CH3CN solutions of the salts afforded X-ray quality crystals of five compounds with hydroxyl gro

222 ding ultra-short high-brightness pulses of X-ray radiation have great potential for a wide impact on

223 was probed using state of the art dynamic X-ray radiography.

224 nfirm that Cu-Cy nanoparticles may improve X-ray radiotherapy on cancer treatment and X-ray activated

225 lved elemental depth profiling in the soft X-ray range with a laboratory source, opening, for example

226 anges were detected in the high-resolution X-ray reflectivity data with monotonic increase in roughne

227 significantly improved fit of experimental x-ray reflectivity data.

228 In this work, synchrotron X-ray reflectivity measurements, accompanied by large-scal

229 ion edges of matter, which lie in the soft X-ray regime above 200 eV, permit the probing of electroni

230 The scaffold protein X-ray repair cross-complementing 1 (XRCC1) interacts with

231 ine-shape of the measured resonant elastic X-ray response can be explained with the "site-selective"

232 mo-multimers, consideration of small-angle X-ray scattering (SAXS) data, and location of heparin-bind

233 e of the dimerization curve in small-angle X-ray scattering (SAXS) experiments using isolated GluA2 l

234 ion spectroscopy (XPCS) in the small-angle X-ray scattering (SAXS) geometry to probe both the structu

235 Small-angle X-ray scattering (SAXS) measurements reveal a striking dif

236 Here we combine wide-angle X-ray scattering (WAXS) with X-ray photon-correlation spec

237 PE2 Zf-GRF X-ray structure and small-angle X-ray scattering analyses show that the Zf-GRF fold is typ

238 esence of NEIL1 and DNA, while small-angle X-ray scattering analysis confirmed the NEIL1 mediated PCN

239 d by in situ grazing-incidence small-angle X-ray scattering and complementary scanning tunneling micr

240 In situ small/wide-angle X-ray scattering and electron microscopic measurements sho

241 Small angle X-ray scattering and ensemble modeling yielded models of t

242 Biophysical analysis, using small angle X-ray scattering and multi-angle light scattering experime

243 ated rOPN were investigated by small-angle x-ray scattering and no significant changes were detected

244 in situ synchrotron-based small/wide angle X-ray scattering and photoluminescence (PL) probes, the NC

245 ed by simultaneous synchrotron small-angle X-ray scattering and Raman spectroscopy in a controlled ga

246 he complex was calculated from small-angle X-ray scattering data and was in good agreement with a mod

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

248 resonance energy transfer, and small-angle x-ray scattering data obtained under conditions when PANS

249 tetrameric form, combined with small-angle X-ray scattering data, allows the localisation of the B do

250 condary structure information, small-angle X-ray scattering data, and any readily available tertiary

251 ay absorption spectroscopy and high-energy X-ray scattering demonstrate a correlation between the def

252 e results demonstrate that single-particle X-ray scattering has the potential to shed light on key bi

253 Small angle X-ray scattering indicates that FP E244K is trapped in a c

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

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

256 Small-angle X-ray scattering showed that certain sequences can form we

257 Through small-angle X-ray scattering studies of sTie2 dimers in solution and m

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

259 al microscopy, calorimetry and small angle X-ray scattering studies.

260 thermal titration calorimetry, small-angle X-ray scattering, and X-ray crystallography.

261 By using small-angle x-ray scattering, high-resolution NMR spectroscopy, and li

262 mal titration calorimetry, and small-angle X-ray scattering, we show that in the homodimeric state, t

263 ptical spectroscopy and resonant inelastic X-ray scattering.

264 eractions upon phosphorylation by solution X-ray scattering.

265 The weak gamma rays seen in EM170817 are dissimilar to classical short

266 X-ray single-crystal analysis of four of the synthesized b

267 e Linac Coherent Light Source (LCLS) is an X-ray source of unmatched brilliance, that is advancing ma

268 direct observation of nano-scale coherent x-ray sources in a laser plasma.

269 erators to produce compact ultraviolet and X-ray sources, has attracted considerable interest for a f

270 Here we combine operando hard X-ray spectroscopic imaging and phase-field modeling to el

271 e chemically analysed by energy dispersive X-ray spectroscopy (EDX), inductively coupled plasma mass

272 on microscopy (STEM) and energy dispersive X-ray spectroscopy in STEM (EDX-STEM).

273 d shown to be suitable for photon counting X-ray spectroscopy when coupled to a low-noise charge-sens

274 tom ligands and verified using small angle x-ray spectroscopy, allows us to calculate the heat releas

275 py, Raman and wavelength/energy dispersive X-ray spectroscopy.

276 : pectoral fin shape, swimming behavior, fin ray stiffness, and mechanosensory sensitivity.

277 sulfur clusters and the paucity of protein X-ray structural data.

278 An X-ray structural investigation of the cerium imido complex

279 Here we report the 2.1 A X-ray structure and molecular function of ClbS, a gene pro

280 Moreover, an APE2 Zf-GRF X-ray structure and small-angle X-ray scattering analyses

281 nfluence of temperature by determining the X-ray structure of Aqy1 at room temperature (RT) at 1.3 A

282 for therapeutic intervention, however GPCR X-ray structures are mostly restricted to their inactive i

283 Knowledge of their single-crystal X-ray structures has been instrumental to enable advanced

284 structural analysis of drug binding using X-ray structures obtained at 100 K.

285 In this study, we present the first X-ray structures of barbiturates bound to GLIC, a cationic

286 X-ray structures of homopolymeric L-ferritin obtained by f

287 yrrole-5-carboxamide for which we obtained X-ray structures of the most potent hit (compound 19, IC50

288 ress in imaging defects using electron and X-ray techniques, in situ three-dimensional imaging of def

289 mbranes that could easily be analyzed with X-ray techniques.

290 High-flux X-ray tomography enabled us to observe both growth and mel

291 Here, a cryoptychographic X-ray tomography method is employed to obtain a full 3D st

292 ocessing framework in full field cryo soft X-ray tomography to computationally extend the depth of fi

293 e stage, the latter through micro-computed X-ray tomography.

294 zed by Scanning Electron Microscopy (SEM), X-ray-tomography and Fourier-Transform Infrared spectrosco

295 Ray tracing simulations support the measurement results.

296 IOL power was calculated for all patients by ray tracing, aiming for postoperative emmetropia.

297 nsets show rapid increase of hard and soft X-rays, ultra-violet emission with large Doppler blue shif

298 Our work implies that gamma-ray vortices should be produced in various situations in

299 and active multiple myeloma, if whole-body X-ray (WBXR) is negative and whole-body MRI is unavailable

300 dvances in free electron laser technology, X-rays with small enough bandwidth have become available,