ライフサイエンスコーパス: ray

1 arious arrangements can be patterned using X-ray.

2 on of linear skull fractures on plain-film X-rays.

3 ed equations and compared with dual-energy x-ray absorptiometry measurements in a subgroup.

4 and a body fat assessment via dual-energy x-ray absorptiometry.

5 ectroscopic methods, particularly operando X-ray absorption and Raman spectroscopy, to study the mech

6 including In K-edge and Ga K-edge extended X-ray absorption fine structure (EXAFS); resonant soft X-r

7 te visible pump soft X-ray probe near-edge X-ray absorption fine structure (NEXAFS) spectroscopy meas

8 Extended X-ray absorption fine structure characterization and densi

9 l sites, as shown by infrared and extended X-ray absorption fine structure spectra.

10 cies, as studied by high energy-resolution X-ray absorption near edge structure (HR-XANES) spectrosco

11 rticles in the PMCs and acquired Ca-L(2,3) X-ray absorption near-edge spectra of these Ca-rich partic

12 emission spectroscopy (XES) with Fe K-edge X-ray absorption near-edge structure (XANES), we demonstra

13 It also enables the acquisition of local X-ray absorption spectra (XAS) on single particles of the

14 We review oxygen K-edge X-ray absorption spectra of both molecules and solids.

15 We have combined X-ray absorption spectroscopic (XAS) fingerprinting and in

16 ith a Si/Al ratio of 15 and 2.6 wt% Cu, by X-ray absorption spectroscopies (XANES and EXAFS) and diff

17 rption spectroscopy (SEIRAS), in situ soft X-ray absorption spectroscopy (Cu L-edge), and online gas

18 through a combination of grazing incidence X-ray absorption spectroscopy (GIXAS) and X-ray diffractio

19 During the last decades, X-ray absorption spectroscopy (XAS) has become an indispen

20 oscopy (AC-STEM), UV-vis spectroscopy, and X-ray absorption spectroscopy (XAS).

21 X-ray absorption spectroscopy analysis discovered that zer

22 X-ray absorption spectroscopy revealed V(V) reduction to V

23 X-ray absorption spectroscopy showed that >90% of all Pb s

24 We use synchrotron X-ray absorption spectroscopy to study the distribution an

25 Complementary experimental (X-ray absorption spectroscopy) and theoretical (Density Fu

26 uction), a conclusion further supported by X-ray absorption spectroscopy, (57)Fe Mossbauer studies, a

27 razing-angle X-ray scattering/diffraction, X-ray absorption spectroscopy, and Raman techniques, we fo

28 dback on the system chemistry from in situ X-ray absorption spectroscopy.

29 s spectrometry, infrared spectroscopy, and X-ray absorption spectroscopy.

30 distinction was probed via fluorine K-edge X-ray absorption spectroscopy.

31 uclear magnetic resonance spectroscopy and X-ray absorption spectroscopy.

32 om Fe(1)(II)-N(4) sites via in-temperature X-ray absorption spectroscopy.

33 rization techniques, including synchrotron X-ray absorption, fluorescence, and diffraction methods, s

34 Single-crystal X-ray analyses on MOF-1 showed that Cu(+2) ion was 6-coord

35 n, as shown via previous energy-dispersive X-ray analysis (EDX) elemental mapping and crystal structu

36 In addition, single-crystal X-ray analysis was used to elucidate the structural featur

37 cterized by multinuclear NMR spectroscopy, X-ray analysis, as well as their calculated NICS values, u

38 types was corroborated by a single-crystal X-ray analysis.

39 d to control the cross-correlation between x-ray and microbunched electrons.

40 lating various news items about the use of X-rays and literature about Roentgen's discovery by journa

41 rmitting its characterization by NMR, EPR, X-ray, and HRMS.

42 ere CO is photolyzed from the heme iron by X-rays at cryogenic temperatures (100 K).

43 cumulates in the liver, where it increases x-ray attenuation due to its iodine content.

44 obtained by exploiting the negligible cosmic-ray background deep underground at the Laboratory for Un

45 sed to reconstruct the spectrum of the gamma-ray beam.

46 due to the nonuniform illumination by the X-ray beam.

47 sion (XMM-Newton) revealed(4) an extended, X-ray-bright gaseous atmosphere with a virial temperature

48 thod will enable searches for further soft-X-ray clock transitions(8,12) in HCIs, which are required

49 X-ray co-crystal structure analysis and ultracentrifugatio

50 The X-ray co-crystal structure of an early lead (12) revealed

51 alities which were characterized by the 3D X-ray Computed Tomography (CT) scan and used to train a Ra

52 mn experiments imaged with high-resolution X-ray computed tomography are used to measure aggregate st

53 The unique nanoscale X-ray computed tomography verifies the well-distributed io

54 We used rhizoboxes, X-ray computed tomography, grafting, auxin transport measu

55 vironmental radioactive materials and cosmic rays contributes to this observed difference.

56 l was further corroborated by obtaining an X-ray crystal structure of a derivative.

57 ons between AcpP and FabD to elucidate the X-ray crystal structure of a type II ACP-AT complex.

58 We determined the X-ray crystal structure of N2, combined with monitoring se

59 We previously determined the X-ray crystal structure of the bacterial RNA polymerase en

60 A 2.1 angstrom X-ray crystal structure of the FigC N-citrylornithine deca

61 The 1.65- angstrom resolution X-ray crystal structure of YaaA reveals that the protein p

62 We report the synthesis, X-ray crystal structure, and molecular recognition propert

63 cle and inhibitory mechanism, we report 11 x-ray crystal structures of human VKOR and pufferfish VKOR

64 Here we report X-ray crystal structures of MEK bound to the scaffold KSR

65 We present X-ray crystal structures of the peptide-free state of HLA-

66 X-ray crystal structures of variously modified ASL(Arg1)(I

67 information, together with analysis of the x-ray crystal structures, provides a starting point for th

68 In this study, X-ray crystallographic analysis has been used to authentic

69 X-ray crystallographic analysis of three compounds (11a, 1

70 ion of 1 was established by single-crystal X-ray crystallographic analysis using Cu Kalpha radiation.

71 Drawing on X-ray crystallographic information, we designed GS-6207 to

72 owing the 2011 report of a high-resolution X-ray crystallographic structure resolving the site of cat

73 s, solution-phase biophysical studies, and X-ray crystallographic structures of hexamers formed by ma

74 Here we present solution and X-ray crystallographic studies that indicate a potential r

75 A comprehensive X-ray crystallographic study (12 crystal structures), invo

76 of the C5_MG4-CirpT complex was solved by X-ray crystallography (at 2.7 angstrom).

77 Using serial femtosecond X-ray crystallography (SFX), we have determined the pristi

78 Structure determination by X-ray crystallography and cryo-electron microscopy not onl

79 X-ray crystallography and mutagenesis confirmed a structur

80 ized using a combination of single-crystal X-ray crystallography and paramagnetic (1)H NMR spectrosco

81 f forming hexamers that can be observed by X-ray crystallography and SDS-PAGE.

82 es of metal centers derived from zero dose X-ray crystallography can advance our mechanistic understa

83 X-ray crystallography experiments allowed structural assig

84 In this work, the serial X-ray crystallography method was successfully adopted to p

85 X-ray crystallography of 11s and related thieno[3,2-d]pyri

86 X-ray crystallography revealed that a potent, reversible,

87 X-ray crystallography revealed the structure of Bs164, the

88 X-ray crystallography reveals that these CNT mimics exhibi

89 Single crystal X-ray crystallography showed that in some cases, fulvenes

90 imentally solved its apo-structure through X-ray crystallography to a resolution of 2.60 angstrom.

91 Here, we used X-ray crystallography to investigate these Dsl1-SNARE inte

92 n of Pv-M17 by cryoelectron microscopy and X-ray crystallography together with solution studies revea

93 X-ray crystallography validated the dimeric mechanism of i

94 ion of cryo-electron microscopy (cryo-EM), x-ray crystallography, and computational predictions were

95 etic mobility macromolecular analysis, EM, X-ray crystallography, and enzyme assays.

96 ng kinetic analyses, fluorescence binding, X-ray crystallography, and gel filtration experiments with

97 f VCBC-Cullin5 has recently been solved by X-ray crystallography, and, using molecular dynamics simul

98 Experimental evidence (e.g., X-ray crystallography, electron paramagnetic resonance, el

99 Compounds 1 and 2 were characterized by X-ray crystallography, electronic and NMR spectroscopy, an

100 at are not amenable to characterization by x-ray crystallography, NMR or EM.

101 f single-particle cryoelectron microscopy, X-ray crystallography, NMR, and other biophysical methods.

102 mainstay structural biology techniques are X-ray crystallography, nuclear magnetic resonance (NMR) im

103 the N terminus insertion and, as shown by X-ray crystallography, partly by Tyr-172 inserting into a

104 mechanistic docking, machine learning, and X-ray crystallography, pointing the way for future terpene

105 With X-ray crystallography, we detected an unexpected photochem

106 Using X-ray crystallography, we have discovered a domain-swap ho

107 Using x-ray crystallography, we show how a preTCR applies the co

108 rements, steady-state enzyme kinetics, and X-ray crystallography, we show that the P167S/D240G double

109 cessfully synthesized and fully studied by X-ray crystallography, X-ray photoelectron spectroscopy, h

110 Hpz=pyrazole) and further characterized by X-ray crystallography.

111 olution mass spectrometry (HRMS), NMR, and X-ray crystallography.

112 TMOP-PH(2) (3a) have been characterized by X-ray crystallography.

113 y and, in many cases, using single-crystal X-ray crystallography.

114 ty mechanisms using molecular dynamics and X-ray crystallography.

115 he pyrG promoter using soak-trigger-freeze X-ray crystallography.

116 ta-amino-alpha-ketone group was secured by X-ray crystallography.

117 estigated their binding modalities through X-ray crystallography.

118 electron microscopy with energy dispersive X-ray detection.

119 We find that X-ray detectors based on PSCs exhibit high sensitivity of

120 X-ray absorption spectroscopy (GIXAS) and X-ray diffraction (GIXRD).

121 ion and morphology were observed by powder-X-ray diffraction (p-XRD), transmission electron microscop

122 nditions, while in situ synchrotron powder X-ray diffraction (PXRD) enables us to monitor the evoluti

123 odel compound, we use operando synchrotron X-ray diffraction (XRD) and nuclear magnetic resonance (NM

124 etry (DSC), polarised light microscopy and X-ray diffraction (XRD) techniques.

125 X-ray diffraction (XRD), gel permeation chromatography (GP

126 tudies as well as crystalline-sponge-based X-ray diffraction analyses.

127 hniques in conjunction with single-crystal X-ray diffraction analysis.

128 reported SrB(3) C(3) ,([1]) single-crystal X-ray diffraction and computational modelling indicate tha

129 ordering of the Al atoms, as evident from X-ray diffraction and electron microscopy.

130 on, as demonstrated by in situ synchrotron X-ray diffraction and Raman studies.

131 X-ray diffraction and reflectivity measurements yield exte

132 ned laboratory and in operando synchrotron X-ray diffraction and scattering experiments with geochemi

133 rmed by high-resolution synchrotron powder X-ray diffraction and state-of-the-art scanning transmissi

134 4 2m was solved by means of single crystal X-ray diffraction as a 6-component twin due to pseudocubic

135 ) has been characterized by single-crystal X-ray diffraction as a solvent-separated ion triplet with

136 Using X-ray diffraction computed tomography, we show that the di

137 studied using crystal truncation rod (CTR) X-ray diffraction coupled with density functional theory (

138 Grazing-incidence X-ray diffraction data confirms that anodic halogenation o

139 X-ray diffraction data indicate that with elevated dATP, m

140 X-ray diffraction evidence indicates that with elevated dA

141 ourier-transform infrared spectroscopy and X-ray diffraction observations confirmed that the NLs have

142 rable crystal lattice distortion in powder X-ray diffraction patterns.

143 rimetry, polarizing optical microscopy and X-ray diffraction provided insight into the unique self-as

144 icroscopies as well as electron and powder X-ray diffraction reveal a complex lamellar structure of b

145 Single-crystal X-ray diffraction reveals that Y6 molecules cofacially pac

146 and austenite [gamma-Fe(0)], appear in the X-ray diffraction spectra minutes after the addition of fe

147 X-ray diffraction studies showed that cis- and trans-1,3-d

148 based on results of in situ single-crystal X-ray diffraction studies up to 27 GPa, we report the disc

149 A combination of single-crystal X-ray diffraction studies, solution and solid-state magnet

150 15)N, (29)Si, and (1)H DOSY NMR as well as X-ray diffraction studies.

151 d 2) was substantiated with single crystal X-ray diffraction study.

152 2)H(25)), which, although shown by in situ X-ray diffraction to be highly crystalline in the reaction

153 rrangement, confirmed in situ using powder X-ray diffraction, allows adsorbent design trade-offs to b

154 , Fourier transform infrared spectroscopy, X-ray diffraction, and electron microscopy.

155 Fourier transform infrared spectroscopy, X-ray diffraction, and gelatinization assays revealed that

156 l evidence arising from the application of X-ray diffraction, and vibrational, electronic, and X-ray

157 Operando experiments by X-ray diffraction, Mossbauer spectroscopy, and galvanostat

158 lyzing the crystal size distribution using x-ray diffraction, transmission electron microscopy and in

159 as characterized step by step using powder X-ray diffraction, transmission electron microscopy, therm

160 ized by elemental analysis, single-crystal X-ray diffraction, UV/Vis absorption, cyclic voltammetry (

161 aterials, as measured by N(2) sorption and X-ray diffraction.

162 NMR spectrometry as well as single-crystal X-ray diffraction.

163 ectroscopy, thermogravimetric analysis and X-ray diffraction.

164 d, and their structures were determined by X-ray diffraction.

165 experimental/computational approach using X-ray diffraction; UV/vis, MCD, IR, EPR, and NMR spectrosc

166 tes the application of in-situ, neutron or X-ray, diffraction techniques to correlating SF strengthen

167 The iodine then absorbs X-rays during radiotherapy (RT), creating free radicals an

168 ation of NMR, Raman, and energy-dispersive X-ray (EDX) spectroscopies.

169 bining femtosecond Fe K(alpha) and K(beta) X-ray emission spectroscopy (XES) with Fe K-edge X-ray abs

170 tion site-occupation is determined through X-ray emission spectroscopy (XES).

171 sitive femtosecond Fe K(alpha) and K(beta) X-ray emission spectroscopy at an X-ray free-electron lase

172 repeater (SGR) bursts were detected in gamma-ray energies.

173 by the combined stressors of stiffness and X-ray exposure.

174 py, multispectral imaging (MSI), and macro X-ray fluorescence (MA-XRF) with minimally invasive surfac

175 d spectroscopy (NIRS) and total reflection X-ray fluorescence (TXRF).

176 Synchrotron-based macro-X-ray fluorescence (XRF) mapping brings to light the prese

177 ion microscopy of proteins and synchrotron X-ray fluorescence imaging of trace metals, both performed

178 high-affinity lanthanide ion binding, and X-ray fluorescence microscopy (XFM).

179 In this work, X-ray fluorescence microscopy was used to measure diffusio

180 tron radiation induced micro- and submicro-X-ray fluorescence spectroscopy (SR-XRF), gadolinium was d

181 before and after fungal interaction using X-ray fluorescence, laser ablation inductively coupled pla

182 t phenomena in condensed matter systems at X-ray free electron laser (FEL) sources.

183 ial femtosecond crystallography (SFX) with X-ray free electron lasers (XFELs) allows structure determ

184 K(beta) X-ray emission spectroscopy at an X-ray free-electron laser (FEL).

185 Intense x-ray free-electron laser (XFEL) pulses hold great promise

186 al femtosecond crystallography(1) using an X-ray free-electron laser(2) to observe light-induced stru

187 tawatt-class infrared laser facilities and x-ray free-electron lasers; despite substantial theoretica

188 per, unmodified fin and a lower portion with rays highly modified into specialized filaments.

189 ning started within the first 10 fs of the X-ray illumination at intensity levels between 10(17) and

190 bound in the active site under comparable X-ray illumination, indicating a much more rigid protein a

191 Furthermore, PSCs exhibit high X-ray imaging capability thanks to its negligible signal d

192 urther demonstrated that synchrotron-based X-ray imaging enabled uncovering finer details of the vari

193 Large-area X-ray imaging is one of the most widely used imaging modal

194 ry testing, electrocardiography, and plain x-ray imaging may often suffice for such patients, but giv

195 ility of synchrotron-based nanotomographic X-ray imaging methods, namely holotomography and transmiss

196 We have used single and multi-bunch, X-ray imaging to differentiate distinct phases of failure

197 e properties translate to high-performance X-ray imaging with sensitivity up to 173 muC Gy(air) (-1)

198 ens (AIE-Au) to achieve efficient low-dose X-ray-induced photodynamic therapy (X-PDT) with negligible

199 An increase in X-ray intensity of all synthesized iodine-containing polym

200 ing decompression process with femtosecond x-ray laser pulses at different pump-probe delay times.

201 On the basis of spatially aligned X-ray ligands, alternative substituents and compound cores

202 Using neutron radiography (NR), X-ray micro-computed tomography (micro-CT), fluorescence m

203 Using cryo-soft X-ray microscopy we imaged intracellular calcium-containin

204 ds, namely holotomography and transmission X-ray microscopy, for the quantitative 3D analysis of the

205 y or affected by myocardial fibrosis using X-ray microtomography.

206 ctroscopy from the European Space Agency's X-ray Multi-Mirror Mission (XMM-Newton) revealed(4) an ext

207 ed more than 30 megaseconds of XMM-Newton (X-ray Multi-Mirror Mission) blank-sky observations to test

208 Here, high-resolution, 3D synchrotron X-ray nano-holotomography images of white matter samples f

209 mprising dry small particles, as proven by X-ray nanotomography.

210 Ray parenchyma fraction (RPF) and seasonal NSC dynamics

211 As a proof-of-concept, an X-ray phase contrast under bending conditions was construc

212 n a wide range of liquids, using ultrafast X-ray phase-contrast imaging.

213 lly reduced and characterized by Raman and X-ray photoelectron spectroscopies in addition to microsco

214 X-ray photoelectron spectroscopy (XPS) and attenuated tota

215 Raman and X-Ray photoelectron spectroscopy (XPS) revealed that the s

216 In the present study, we employed X-ray photoelectron spectroscopy and Fourier-transform inf

217 Furthermore, valence band analysis by X-ray photoelectron spectroscopy and photoluminescence spe

218 Hard-x-ray photoelectron spectroscopy is a valuable source of i

219 X-ray photoelectron spectroscopy recommends the chemical i

220 Ambient-pressure x-ray photoelectron spectroscopy showed that water added t

221 he exposed samples were investigated using X-ray photoelectron spectroscopy, Fourier transform infrar

222 nd fully studied by X-ray crystallography, X-ray photoelectron spectroscopy, hydrogen evolution exper

223 Scanning electron microscopy, X-ray photoelectron spectroscopy, transmission electron mi

224 ained by means of diffraction, optical and X-ray photoelectron spectroscopy.

225 As more than 98.5% of the X-ray photon flux is attenuated within the steel injector

226 he refractive and absorptive properties of X-ray photons.

227 ort a femtosecond time-resolved X-ray pump/X-ray probe experiment on protein nanocrystals.

228 We demonstrate visible pump soft X-ray probe near-edge X-ray absorption fine structure (NEX

229 photoactive yellow protein (PYP) with MHz X-ray pulse rates.

230 Extremely short X-ray pulses from a free-electron laser are helping to cla

231 an XFEL (EuXFEL) delivers femtosecond (fs) X-ray pulses in trains spaced 100 ms apart whereas pulses

232 The ability to deliver two coherent X-ray pulses with precise time-delays ranging from a few f

233 ere, we report a femtosecond time-resolved X-ray pump/X-ray probe experiment on protein nanocrystals.

234 tiffness, within the range of high MD, and X-ray radiation have an approximately additive effect on i

235 different heme protein crystal species by X-ray radiation.

236 Finally, phase-contrast CT uses x-ray refraction properties to improve spatial and soft-ti

237 ntal data from the water window to the keV x-ray regime.

238 press in Malaga reported the discovery of X-rays, relating various news items about the use of X-ray

239 During the third session, 29 soft-gamma-ray repeater (SGR) bursts were detected in gamma-ray ene

240 tion fine structure (EXAFS); resonant soft X-ray scattering (R-SoXS); ultraviolet photoelectron spect

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

242 yo-EM structure, combined with small-angle X-ray scattering (SAXS), also allowed us to predict the ge

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

244 ted with the help of small- and wide-angle x-ray scattering and complementary neutron diffraction exp

245 s effect on corneal collagen architecture, x-ray scattering and electron microscopy data were collect

246 s made at room temperature using inelastic X-ray scattering and neutron scattering techniques.

247 Simultaneous measurements of resonant X-ray scattering and transport reveal that this drastic re

248 Small-angle X-ray scattering data revealed that in the presence of tRF

249 rlo simulations constrained by high energy x-ray scattering data.

250 Small- and wide-angle X-ray scattering examines the packing of PE chains into se

251 py imaging, cryo-EM tomography and in-situ X-ray scattering methods.

252 Small angle X-ray scattering was especially used to determine size par

253 -free method based on spectral small-angle X-ray scattering with a polychromatic beam for in vivo est

254 Combining oxygen sensing, X-ray scattering, and Atomic Force Microscopy, we show tha

255 imetry (DSC), grazing-incidence wide-angle X-ray scattering, and microscopy can be related directly t

256 ssays; and immunofluorescence, small-angle X-ray scattering, and MS-based analyses, we report that GA

257 nalytical ultracentrifugation, small-angle X-ray scattering, molecular dynamics simulations and a DNa

258 resonance spectroscopy (PDS), small-angle x-ray scattering, targeted protein cross-linking, and cryo

259 edoping of a conjugated polymer system via X-ray scattering.

260 sting sponge phase observed by small-angle x-ray scattering.

261 By using in situ grazing-angle X-ray scattering/diffraction, X-ray absorption spectroscop

262 monary disease severity on CXRs (pulmonary x-ray severity (PXS) score), using weakly-supervised pretr

263 lar dynamics simulations revealed that the x-ray spectra are sensitive to structural dynamics at the

264 fraction, and vibrational, electronic, and X-ray spectroscopies that exist, along with the results of

265 X-ray spectroscopy (i.e., XAS and EDX) and diffraction ind

266 microscopy coupled with energy dispersive X-ray spectroscopy (TEM-EDX) is a powerful tool for determ

267 Recent advanced EPR and Mn K-edge X-ray spectroscopy studies converge upon the HO model.

268 ed at the desired position using a focused X-ray spot of sub-50-nm size.

269 X-ray structural analyses of the PIs complexed with wild-t

270 The design, synthesis, and X-ray structural analysis of hybrid HIV-1 protease inhibit

271 X-ray structure determination revealed an NTD consisting o

272 Here, we report the X-ray structure of a closed bacterial TMEM175 channel in c

273 The X-ray structure of a truncated monomer of Type III Dio (Di

274 rotein 1D3Z (to within 2.4 angstrom of the X-ray structure) using only N-H RDCs from one alignment me

275 rimers with cross sections consistent with X-ray structures and reports from surface-induced dissocia

276 X-ray structures in complex with HIV-1 RT/dsDNA showed bin

277 We report multiple cryo-EM and X-ray structures in four different states, including three

278 On the basis of X-ray structures of a CNS-penetrating reactivator, monoxim

279 Single-crystal X-ray structures of Re[Cl(8)TpCF(3)PC](O), Re[Cl(8)TpCH(3)

280 function, we investigated the cryo-EM and X-ray structures of Rep68-ssDNA complexes.

281 Metal centers in X-ray structures of small organometallic or coordination c

282 Here we describe the high-resolution X-ray structures of the heterodimer of Gc and the Gn head

283 X-ray structures of the receptors in complex with 10 new a

284 In X-ray structures, changes in the 220-loop of the receptor-

285 o cavities from recently described protein X-ray structures.

286 t X-rays, whether obtained in conventional X-ray suites or with portable units, are the first-line im

287 clusters and complete characterization by X-ray, TGA, UV-vis, and ICP studies.

288 in has a better absorption coefficient for X-rays than eumelanin.

289 ap," in which some temporally incident light rays to the nasal retina pass anterior to the IOL and so

290 Cryo-soft x-ray tomography analysis revealed that SMAPs had a carbon

291 udy, we propose multi-scale phase contrast x-ray tomography as a tool to unravel the pathophysiology

292 Using synchrotron X-ray tomography, light and transmission electron microsco

293 Here, we use ray tracing to predict the spatial and temporal dynamics

294 Four articles that explore using ray-tracing optical modeling suggest an "illumination ga

295 Methods: A fast ray-tracing time-of-flight projector was implemented and

296 The temporal resolution of X-ray transient absorption experiments with this beamline

297 hybrid SPECT/CT systems, replacing low-end x-ray tubes with high-end multislice CT scanners equipped

298 corded using highly coherent and divergent x-ray waveguide radiation.

299 ngs are the main organ involved, and chest X-rays, whether obtained in conventional X-ray suites or w

300 Second, beryllium-7 is a product of cosmic rays which are themselves directly linked to solar activ