ライフサイエンスコーパス: X-ray

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

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

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

4 Canada, referred for a baseline dual-energy x-ray absorptiometry scan from January 1, 1996, to March

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

6 ensity, typically assessed using dual-energy X-ray absorptiometry.

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

8 orption, resonance Raman, (1)H NMR, EPR, and X-ray absorption (near-edge) spectroscopy, ESI mass spec

9 Low X-ray absorption contrast in non-mineralised tissue can

10 dipolar contributions in the uranium L3-edge X-ray absorption cross section to provide unique informa

11 Spectroelectrochemical X-ray absorption data further reveal systematic spectral

12 BCO) by simultaneous ionic liquid gating and X-ray absorption experiments.

13 intermediate using Fe- and Mn-edge extended X-ray absorption fine structure (EXAFS) analysis and mul

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

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

16 The in situ extended X-ray absorption fine structure analysis shows a Ru hori

17 was investigated by direct monitoring of the X-ray absorption fine structure of the catalyst, coupled

18 Extended X-ray absorption fine-structure spectroscopy showed red

19 contrary to formulation, was confirmed using X-ray absorption near edge spectroscopy, suggesting subs

20 strated that the U M4 high energy resolution X-ray absorption near edge structure (HR-XANES) method i

21 Synchrotron-based X-ray absorption near-edge structure (XANES) spectroscop

22 X-ray absorption spectra indicated that U(IV) in both he

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

24 ctable by chemical extractions, Mossbauer or X-ray Absorption spectroscopies.

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

26 X-ray absorption spectroscopy (XAS) is an electronic abs

27 s Hg(II) biouptake pathway, we have employed X-ray absorption spectroscopy (XAS) to investigate the r

28 sonance (EPR), SQUID, UV-vis absorption, and X-ray absorption spectroscopy (XAS)) coupled with advanc

29 X-ray absorption spectroscopy and high-energy X-ray scat

30 X-ray absorption spectroscopy and X-ray photoelectron sp

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

32 Spatially resolved X-ray absorption spectroscopy documented a reduction of

33 g the co-localization results to iron K-edge X-ray absorption spectroscopy fitting results allowed to

34 In operando X-ray absorption spectroscopy identified reduced Pt cove

35 X-ray absorption spectroscopy provides firm evidence for

36 ssion electron microscopy (TEM) and operando X-ray absorption spectroscopy showed that oxygen species

37 We used X-ray absorption spectroscopy to characterize the struct

38 Analysis of chemical reactivity, in situ X-ray absorption spectroscopy, and density functional th

39 l and long-range structure probes, including X-ray absorption spectroscopy, pair distribution functio

40 es by Cu K-edge, Cu L2,3-edge, and Cl K-edge X-ray absorption spectroscopy.

41 ransmission electron microscopy and operando X-ray absorption structures to study the mechanical prop

42 X-ray absorption studies of the geometric and electronic

43 oit the element and site selectivity of soft X-ray absorption to sensitively follow the ultrafast pip

44 ions showing that NGC 5907 ULX is instead an x-ray accreting neutron star (NS) with a spin period evo

45 e X-ray radiotherapy on cancer treatment and X-ray activated Cu-Cy nanoparticles can be efficiently d

46 tionship and promote a rational synthesis of X-ray amorphous IrOx hydroxides that contain a favorable

47 ectron microscopy (HRTEM), energy dispersive X-ray analysis (EDX), atomic force microscopy (AFM), sca

48 eochemistry was unequivocally established by X-ray analysis of precursor trans-(+)-5a as camphorsulfo

49 ctroscopic data as well as by single crystal X-ray analysis.

50 med by DFT quantum chemical calculations and X-ray analysis.

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

52 Conventional optical, X-ray and photoelectron probes often fail to provide int

53 AM beams in the extreme ultraviolet (XUV) or X-ray, and controlling the OAM on these beams remains ch

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

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

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

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

58 Here we present NMR and X-ray characterization for the two classes of these inhi

59 -cell line panel and allowed us to obtain an X-ray co-crystal structure of the synthetic secondary me

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

61 orm for magnetic resonance imaging (MRI) and x-ray computed tomography (CT) enabled by the gadolinium

62 ton emission computed tomography (SPECT) and X-ray computed tomography (CT) for investigating transpo

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

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

65 X-ray crystal structure analysis of both Rh complexes fo

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

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

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

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

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

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

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

73 In this study, we determined the X-ray crystal structure of the PEAK1 pseudokinase domain

74 ared by a templated clipping reaction and an X-ray crystal structure shows that the squaraine gem-dim

75 the highly organized capsules is shown by an X-ray crystal structure which features the assembly of t

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

77 X-ray crystal structures of example compounds from this

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

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

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

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

82 The X-ray crystallographic analysis confirms that while CIP

83 degrees that was unambiguously confirmed by X-ray crystallographic analysis.

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

85 Here, we determined the X-ray crystallographic structures of two catalytically i

86 bioinformatic, biochemical, mutational, and X-ray crystallographic studies on the unicellular alga C

87 This first X-ray crystallographic study of a single human CCT subun

88 Serial X-ray crystallography allows macromolecular structure de

89 Conventional structural methods such as X-ray crystallography and cryo-transmission electron mic

90 the CL40 and CL59 complexes with gHgL using X-ray crystallography and EM to identify their epitope l

91 We report the low pH characterization by X-ray crystallography and EPR spectroscopy of the nitrog

92 r strictly on experimental evidence, such as X-ray crystallography and nuclear magnetic resonance (pr

93 While X-ray crystallography and nuclear magnetic resonance spe

94 and the IgG1 CH3 homodimer was evidenced by X-ray crystallography and used to engineer examples of b

95 yoEM) can circumvent some of the problems of x-ray crystallography as a pipeline for obtaining the re

96 X-ray crystallography confirms they have the fluorite st

97 Protein X-ray crystallography established that 3-unsubstituted 2

98 dynamic regions that proved unresolvable by X-ray crystallography in homologous receptors.

99 n analyzing dynamics of crystalline proteins.X-ray crystallography is the main method for protein str

100 However, X-ray crystallography of these intermediates is severely

101 An X-ray crystallography study of the rabbit muscle GPb inh

102 ethod for protein structure determination is X-ray crystallography which relies on the availability o

103 oton NMR relaxation dispersion measurements, X-ray crystallography, and structure-based chemical shif

104 (SBDD) guided by structural information from X-ray crystallography, computational studies, and NMR so

105 tions of the Cu(II) corresponding complex by X-ray crystallography, EPR, and XAS spectroscopic method

106 ere shown to possess a novel binding mode by X-ray crystallography, in which the triazolo N1 atom coo

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

108 e mechanism underlying these dynamics, using X-ray crystallography, NMR spectroscopy, and ab initio q

109 Freeze-trapping x-ray crystallography, nuclear magnetic resonance, and c

110 By combination of X-ray crystallography, SAXS and EM, together with bioche

111 fully characterized by NMR spectroscopy and X-ray crystallography.

112 ized, and its stereochemistry established by X-ray crystallography.

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

114 and NMR spectroscopy, DFT calculations, and X-ray crystallography.

115 actions, which is most commonly performed by X-ray crystallography.

116 iodosobenzene-metal adducts characterized by X-ray crystallography.

117 opy, IR spectroscopy, mass spectrometry, and X-ray crystallography.

118 lorimetry, small-angle X-ray scattering, and X-ray crystallography.

119 haracterized by spectroscopic studies and by X-ray crystallography.

120 ifferent affinities was evidenced by NMR and X-ray crystallography.

121 roposed on the basis of NMR spectroscopy and X-ray crystallography.

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

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

124 The X-ray data show how Tyr34 maintains solvent exclusion an

125 sed on previously published 3.8-A resolution X-ray data.

126 ctron microscopy (SEM), UV-Vis spectroscopy, X-ray diffraction (XRD) analysis and Fourier transform i

127 e melting curve in molybdenum by synchrotron X-ray diffraction analysis of crystalline microstructure

128 In situ X-ray diffraction analysis reveals that the material und

129 X-ray diffraction analysis showed that calcium carbonate

130 In situ single-crystal X-ray diffraction analysis was carried out at 298 K usin

131 -protein ternary adduct was characterized by X-ray diffraction analysis.

132 I) complex was prepared and characterized by X-ray diffraction analysis.

133 rized by multinuclear NMR and single-crystal X-ray diffraction analysis.

134 s included transmission electron microscopy, X-ray diffraction and asymmetrical flow field-flow fract

135 X-ray diffraction and reciprocal space maps identify the

136 llent materials quality, as characterized by X-ray diffraction and surface area analysis.

137 Through X-ray diffraction and X-ray photoelectron spectroscopy,

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

139 Single-crystal X-ray diffraction confirmed structures that resemble a s

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

141 ere mechanics and micrometer-nanometer-scale X-ray diffraction from synchrotron light in intact ventr

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

143 n, synchrotron radiation-based high-pressure X-ray diffraction is used to quantify the influence of d

144 X-ray diffraction of precipitates showed that Mnt interl

145 electron microscopy, UV-Visible spectra and X-ray diffraction pattern.

146 Here, utilizing the synchrotron X-ray diffraction technique, we for the first time, expe

147 including synchrotron-based grazing incident X-ray diffraction to observe crystal structure and chemi

148 analysis (fwhm) was performed on the powder X-ray diffraction traces and showed that the higher conc

149 X-ray diffraction tracks the light-induced femtosecond c

150 ctroscopy and low-temperature single-crystal X-ray diffraction, and in the gas phase by quantum-chemi

151 comprehensive structural characterizations (X-ray diffraction, electron microscopy, Raman, and UV-vi

152 action processes, as demonstrated by in situ X-ray diffraction, galvanostatic intermittent titration

153 agome structure has been confirmed by powder X-ray diffraction, high-resolution transmission electron

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

155 By combining x-ray diffraction, molecular dynamics simulations, and e

156 terized by transmission electron microscopy, X-ray diffraction, Raman spectroscopy, X-ray photoelectr

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

158 n was analyzed for polymorphism using powder X-ray diffraction, solid fat content by pulsed nuclear m

159 ucture and purity were verified using powder X-ray diffraction, transmission electron microscopy, Ram

160 in situ high-pressure synchrotron radiation X-ray diffraction, we reveal a polymorphic transition fr

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

162 by atomic force microscopy, grazing incident X-ray diffraction, X-ray photoelectron spectroscopy, and

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

164 lowed by in situ variable temperature powder X-ray diffraction.

165 turies were analyzed using synchrotron-based X-ray diffraction.

166 ion using small-angle neutron scattering and X-ray diffraction.

167 llulose were detected by NMR and synchrotron X-ray diffraction.

168 ion of a mammalian mitochondrion by coherent x-ray diffractive imaging (CXDI) using synchrotron radia

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

170 ve of GW170817, as well as the gamma-ray and X-ray emission (and possibly also the ultraviolet and op

171 reting black hole or neutron star often show x-ray emission extending to high energies (>10 kilo--ele

172 f the compounds were measured using variable X-ray energies in the vicinity of the U L3 edge in the T

173 ansfer maximizes the XRS signal at the given X-ray energy and enhances nondipole contributions compar

174 Mechanistic and X-ray evidence is presented that supports that the react

175 X-ray fibre diffraction, hydrogen-deuterium exchange and

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

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

178 X-ray fluorescence (XRF) microscopy, quantified with ele

179 X-ray fluorescence imaging of pinna cross-sections revea

180 nt of gadolinium retention in the tibia with x-ray fluorescence in a laboratory at McMaster Universit

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

182 cromolecular structure determination at both X-ray free electron lasers (XFELs) and, more recently, s

183 aphy of biological objects-an application of X-ray free-electron lasers that greatly enhances our abi

184 ect lithography on NC films with e-beams and X-rays has gone through an important development as it h

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

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

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

188 =2-phenylpyridine) and their applications in X-ray-induced photodynamic therapy (X-PDT) of colon canc

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

190 Using x-ray magnetic circular and linear dichroism techniques,

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

192 c visualization study using fast synchrotron X-ray micro-tomography to provide new insights into thes

193 In vivo x-ray microcomputed tomography of dehydrating leaves of

194 l is investigated here using the synchrotron X-ray microdiffraction.

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

196 Complementary scanning transmission X-ray microscopy revealed that these aggregates are stro

197 percolation of metallic melt is provided by X-ray microtomography of primitive achondrite Northwest

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

199 Synchrotron X-ray nanofluorescence was applied to map the trace elem

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

201 first time an InGaP (GaInP) photon counting X-ray photodiode has been developed and shown to be suit

202 and cluster packing on both supports, while x-ray photoelectron and absorption spectroscopy demonstr

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

204 s were studied for their HER activity and by X-ray photoelectron spectroscopy (XPS) for the first tim

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

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

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

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

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

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

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

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

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

214 copy, X-ray diffraction, Raman spectroscopy, X-ray photoelectron spectroscopy, UV-vis absorption spec

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

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

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

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

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

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

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

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

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

224 confirm that Cu-Cy nanoparticles may improve X-ray radiotherapy on cancer treatment and X-ray activat

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

226 changes were detected in the high-resolution X-ray reflectivity data with monotonic increase in rough

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

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

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

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

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

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

233 homo-multimers, consideration of small-angle X-ray scattering (SAXS) data, and location of heparin-bi

234 ape of the dimerization curve in small-angle X-ray scattering (SAXS) experiments using isolated GluA2

235 ation spectroscopy (XPCS) in the small-angle X-ray scattering (SAXS) geometry to probe both the struc

236 Small-angle X-ray scattering (SAXS) measurements reveal a striking d

237 Here we combine wide-angle X-ray scattering (WAXS) with X-ray photon-correlation sp

238 APE2 Zf-GRF X-ray structure and small-angle X-ray scattering analyses show that the Zf-GRF fold is t

239 presence of NEIL1 and DNA, while small-angle X-ray scattering analysis confirmed the NEIL1 mediated P

240 ied by in situ grazing-incidence small-angle X-ray scattering and complementary scanning tunneling mi

241 In situ small/wide-angle X-ray scattering and electron microscopic measurements s

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

243 Biophysical analysis, using small angle X-ray scattering and multi-angle light scattering experi

244 ylated rOPN were investigated by small-angle x-ray scattering and no significant changes were detecte

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

246 ysed by simultaneous synchrotron small-angle X-ray scattering and Raman spectroscopy in a controlled

247 the complex was calculated from small-angle X-ray scattering data and was in good agreement with a m

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

249 r resonance energy transfer, and small-angle x-ray scattering data obtained under conditions when PAN

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

251 secondary structure information, small-angle X-ray scattering data, and any readily available tertiar

252 -ray absorption spectroscopy and high-energy X-ray scattering demonstrate a correlation between the d

253 ese results demonstrate that single-particle X-ray scattering has the potential to shed light on key

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

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

256 Here we use resonant inelastic X-ray scattering over a wide temperature range across th

257 the spin texture and the polarized resonant X-ray scattering process.

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

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

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

261 ical microscopy, calorimetry and small angle X-ray scattering studies.

262 sothermal titration calorimetry, small-angle X-ray scattering, and X-ray crystallography.

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

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

265 optical spectroscopy and resonant inelastic X-ray scattering.

266 nteractions upon phosphorylation by solution X-ray scattering.

267 X-ray single-crystal analysis of four of the synthesized

268 Raleigh and Compton scattering peaks of the X-ray source (molybdenum anode).

269 The Linac Coherent Light Source (LCLS) is an X-ray source of unmatched brilliance, that is advancing

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

271 elerators to produce compact ultraviolet and X-ray sources, has attracted considerable interest for a

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

273 ere chemically analysed by energy dispersive X-ray spectroscopy (EDX), inductively coupled plasma mas

274 tron microscopy (STEM) and energy dispersive X-ray spectroscopy in STEM (EDX-STEM).

275 and shown to be suitable for photon counting X-ray spectroscopy when coupled to a low-noise charge-se

276 ustom ligands and verified using small angle x-ray spectroscopy, allows us to calculate the heat rele

277 copy, Raman and wavelength/energy dispersive X-ray spectroscopy.

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

279 An X-ray structural investigation of the cerium imido compl

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

281 Moreover, an APE2 Zf-GRF X-ray structure and small-angle X-ray scattering analyse

282 influence of temperature by determining the X-ray structure of Aqy1 at room temperature (RT) at 1.3

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

284 Knowledge of their single-crystal X-ray structures has been instrumental to enable advance

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

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

287 X-ray structures of homopolymeric L-ferritin obtained by

288 X-ray structures of the KcsA channel suggest that this i

289 ]pyrrole-5-carboxamide for which we obtained X-ray structures of the most potent hit (compound 19, IC

290 X-ray structures revealed that the residues adjacent to

291 ogress in imaging defects using electron and X-ray techniques, in situ three-dimensional imaging of d

292 membranes that could easily be analyzed with X-ray techniques.

293 High-flux X-ray tomography enabled us to observe both growth and m

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

295 processing framework in full field cryo soft X-ray tomography to computationally extend the depth of

296 ife stage, the latter through micro-computed X-ray tomography.

297 lyzed by Scanning Electron Microscopy (SEM), X-ray-tomography and Fourier-Transform Infrared spectros

298 onsets show rapid increase of hard and soft X-rays, ultra-violet emission with large Doppler blue sh

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

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