ライフサイエンスコーパス: synchrotron

1 d with vacuum-ultraviolet (VUV) light from a synchrotron.

2 structure of X-ray radiation, produced by a synchrotron.

3 ond PYP dynamics to timescales accessible at synchrotrons.

4 ))(2) in three-dimensional momentum space by synchrotron and laser-based angle-resolved photoemission

5 ents for its successful commercialization in synchrotron and medical imaging.

6 By pairing in situ synchrotron and quartz crystal microbalance measurements

7 e of Li2Mg2P3O9N was determined from ex situ synchrotron and time-of-flight neutron diffraction data

8 wed improved detection limits over and above synchrotron and UV imaging which had both been performed

9 rast imaging at the Swiss Light Source (SLS) synchrotron and X-ray projection microscopy via an LWFA

10 A combination of synchrotron based X-ray microprobe and bulk techniques w

11 The aim of the present study was a synchrotron-based characterization of micro- and nanosiz

12 icle, it is demonstrated how a multispectral synchrotron-based deep-UV photoluminescence microimaging

13 at the subnanometer scale, confirmed through synchrotron-based diffraction and aberration corrected e

14 ng a "toolbox" of high-level laboratory- and synchrotron-based electron and soft X-ray spectroscopies

15 field-dependent aberrations of a full-field synchrotron-based extreme ultraviolet microscope.

16 t study on chronic algal toxicity to combine synchrotron-based Fourier transform infrared spectromicr

17 n situ characterisation techniques including synchrotron-based grazing incident X-ray diffraction to

18 ports, for the first time, implementation of synchrotron-based hard X-ray nanotomography in Al-Cu all

19 We used synchrotron-based imaging to investigate whether airway

20 Here we show, using a novel synchrotron-based in vivo imaging technique, that wild-t

21 aves (i.e. leaf midveins and petioles) using synchrotron-based in vivo x-ray microcomputed tomography

22 Synchrotron-based in-situ small angle X-ray scattering (

23 We have previously demonstrated using synchrotron-based infrared microspectroscopy that the st

24 ter acidic incubation was investigated using synchrotron-based K-edge X-ray absorption near-edge stru

25 Synchrotron-based macro-X-ray fluorescence (XRF) mapping

26 was imaged simultaneously and in situ using synchrotron-based micro X-ray fluorescence (mu-XRF), X-r

27 esolution, which was strongly congruent with synchrotron-based models.

28 Using synchrotron-based nano-x-ray fluorescence and complement

29 this work, we demonstrate the capability of synchrotron-based nanotomographic X-ray imaging methods,

30 ty functional theory (DFT) calculations, and synchrotron-based near ambient X-ray photoelectron spect

31 In this work, we employ synchrotron-based near-field infrared nano-spectroscopy

32 Synchrotron-based nuclear resonance vibrational spectros

33 nealing in situ under high pressure by using synchrotron-based small angle x-ray scattering (SAXS).

34 By using in situ synchrotron-based small/wide angle X-ray scattering and

35 Ambient pressure in situ synchrotron-based spectroscopic techniques have been cor

36 , and samples from remediation columns using synchrotron-based techniques and molecular modeling.

37 Combining a series of synchrotron-based techniques with Raman spectroscopy and

38 Using an advanced synchrotron-based wide-field IR imaging system and state

39 arious microspectroscopic methods, including synchrotron-based X-ray absorption fine structure spectr

40 Synchrotron-based X-ray absorption near-edge structure (

41 ganic and inorganic P species in soils using synchrotron-based X-ray absorption near-edge structure (

42 Recently, synchrotron-based X-ray absorption spectroscopy (XAS) ha

43 We used synchrotron-based X-ray absorption spectroscopy to measu

44 dvanced high-speed, high-spatial resolution, synchrotron-based X-ray computed microtomography (sCT) w

45 The tubes were scanned by synchrotron-based X-ray computed tomography to visualise

46 ination of transmission electron microscopy, synchrotron-based X-ray diffraction, and phase-field mod

47 l LDHs was followed by in situ time-resolved synchrotron-based X-ray diffraction, remarkably agreeing

48 the late 19th centuries were analyzed using synchrotron-based X-ray diffraction.

49 ation of a tnt1 insertional mutant line, and synchrotron-based X-ray fluorescence assays were carried

50 ier transform infrared spectromicroscopy and synchrotron-based X-ray fluorescence imaging were first

51 We further demonstrated that synchrotron-based X-ray imaging enabled uncovering finer

52 ting pathways of quasicrystals, we performed synchrotron-based X-ray imaging experiments on a decagon

53 Our dynamic and 3D synchrotron-based X-ray imaging results reveal the marke

54 thods were confirmed by the 3D techniques of synchrotron-based X-ray imaging.

55 To determine how synchrotron-based X-ray micro-tomography (micro-CT) can

56 -ray (EDX) spectroscopy and combined it with synchrotron-based X-ray total scattering, pair distribut

57 We used synchrotron-based, grazing incidence, wide-angle x-ray s

58 Here, we employed in situ heating, synchrotron-based, X-ray diffraction to quantitatively i

59 canning crystallography using a microfocused synchrotron beam that allowed for the collection of two

60 of pigmented areas by non-invasive, infrared synchrotron beam.

61 The introduction of an X-ray synchrotron beamline designed to be tunable to long wave

62 d optimization (CAMEO) is implemented at the synchrotron beamline to accelerate the interconnected ta

63 ems using x-ray scattering measurements at a synchrotron beamline.

64 hms on autonomously-steered experiments at a synchrotron beamline.

65 ght Source II (NSLS-II) 70 keV monochromatic synchrotron beamline.

66 nd X-ray source at the Advanced Light Source synchrotron beamlines, but the excessive radiation damag

67 Advanced in situ synchrotron characterization reveals insights into the c

68 ctral component with power comparable to the synchrotron component.

69 lack hole system V404 Cygni, showing a rapid synchrotron cooling event in its 2015 outburst, we prese

70 MGy per dataset in static and time-resolved synchrotron crystallography experiments at RT.

71 A novel time-lapse synchrotron deep-UV microscopy methodology was developed

72 spatial resolution thanks to the advances in synchrotron design that dramatically increase coherent f

73 In operando synchrotron diffraction and in operando X-ray absorption

74 ricacies may indicate the detection limit of synchrotron diffraction and TEM.

75 perature while acquiring consecutive in situ synchrotron diffraction patterns from the beginning to t

76 sults support the omega(-4/3) scaling of the synchrotron emission model as a limiting efficiency of t

77 The coherent synchrotron emission model, when adequately corrected fo

78 relativistic particles required to power the synchrotron emission of the radio filaments within and i

79 rved radiation: inverse Compton emission and synchrotron emission of ultrarelativistic electrons.

80 ion rate(6), unusual gas chemistry, enhanced synchrotron emission(7,8), and a multitude of radio-emit

81 custom microfluidic cell for an in operando synchrotron experiment using X-ray attenuation.

82 used high-fidelity simulations, coupled with synchrotron experiments, to capture fast multitransient

83 h of this research is being done using large synchrotron facilities or relatively low-flux microfocus

84 vantage of the relatively recent advances in synchrotron facilities.

85 de at the microfocus beamline of the Indus-2 synchrotron facility.

86 Synchrotron Fourier transform infrared (S-FTIR) microspe

87 Synchrotron-Fourier transform infrared (S-FTIR) microspe

88 ter beta-turn structure was also observed by synchrotron-Fourier transform infrared (S-FTIR) microspe

89 Then, we use data derived from synchrotron FTIR studies of the T. rex vessels to analys

90 Synchrotron generated monochromatic X-rays can be precis

91 Using surface sensitive synchrotron grazing incidence small angle X-ray scatteri

92 the membrane surface, as detected by in situ synchrotron grazing-incidence X-ray diffraction.

93 erein we present a new methodology employing synchrotron hard X-ray fluorescence to observe the conce

94 ed layer-structured dinitride, using in-situ synchrotron high-pressure x-ray diffraction measurements

95 We report a synchrotron Laue diffraction study on the microstructure

96 meter-nanometer-scale X-ray diffraction from synchrotron light in intact ventricular trabeculae from

97 on fine structure microscope at the National Synchrotron Light Source can probe the surface chemistry

98 able detection response under BNL's National Synchrotron Light Source II (NSLS-II) 70 keV monochromat

99 solution of 1.95 A, from data collected at a synchrotron light source.

100 Undulator based synchrotron light sources and Free Electron Lasers (FELs

101 haracterization techniques using X-rays from synchrotron light sources, such as micro-computed tomogr

102 pability is now provided at third generation synchrotron light sources, where X-ray fluorescence micr

103 rodisc with nanoscale resolution, and with a synchrotron-limited temporal resolution of 70 ps.

104 arger pressure range exploiting the upgraded synchrotron machines, and directly transferred to time-r

105 (9-11) favours emission models that describe synchrotron masers or electromagnetic pulses powered by

106 mination beyond the limitations imposed upon synchrotron measurements by radiation damage.

107 ugh single-particle, multimodal, and in situ synchrotron measurements.

108 We used synchrotron methods to understand the modes underlying c

109 Here we use synchrotron micro computed tomography to analyse the cra

110 Furthermore, this is the first time synchrotron microCT with monochromatic X-rays is employe

111 We used synchrotron microtomography to describe the fossil denti

112 most basal stem osteichthyan, visualized by synchrotron microtomography, reveals a developmental rel

113 mbining immunohistochemistry, histology, and synchrotron microtomography, we reconstructed models of

114 Here we apply synchrotron Mossbauer source spectroscopy in laser-heate

115 Time-domain synchrotron Mossbauer spectroscopy (SMS) based on the Mo

116 Synchrotron mu-X-ray based techniques combined with mu-R

117 osized particle content were evaluated using synchrotron mu-X-ray fluorescence spectroscopy (XRF), na

118 roducts were characterized using SEM-EDS and synchrotron muXRD and muXRF.

119 ng a combination of single crystal X-ray and synchrotron/neutron powder diffraction, combined with im

120 The focus is on synchrotron nuclear magnetic resonance spectroscopy, X-r

121 rer, than those previously published using a synchrotron or fluorescence in situ hybridisation (FISH)

122 This study demonstrates that synchrotron PB-X-PCI, combined with image processing too

123 following lung injury, using high-resolution synchrotron phase-contrast CT.

124 xplained by inverse Compton up-scattering of synchrotron photons by high-energy electrons.

125 Herein, a combination of in situ synchrotron powder and single-crystal diffraction, infra

126 roducible reaction conditions, while in situ synchrotron powder X-ray diffraction (PXRD) enables us t

127 try and further confirmed by high-resolution synchrotron powder X-ray diffraction and state-of-the-ar

128 stallographic refinements of high-resolution synchrotron powder X-ray diffraction data give unphysica

129 In situ monitoring by synchrotron powder X-ray diffraction revealed that speci

130 study using a combination of single crystal/synchrotron powder X-ray diffraction, solid-state (7) Li

131 s well as from the temperature variations of synchrotron powder X-ray diffractions and differential s

132 time-efficient 3D multiscale capabilities of synchrotron Propagation-based X-Ray Phase Contrast Imagi

133 experiments of pPv-(Mg0.75,Fe0.25)SiO3 using synchrotron radial X-ray diffraction in a membrane-drive

134 Synchrotron radiation (SR)-based X-ray methods are power

135 Further synchrotron radiation analysis of a number of these entr

136 and ion coincidence techniques combined with synchrotron radiation and compared with high-level theor

137 is based on the combination of polychromatic synchrotron radiation and ptychographic imaging with a r

138 e 2H to the 1T phase, which was confirmed by synchrotron radiation and spherical aberration TEM.

139 this study, we employed orthogonal cellular synchrotron radiation based spectro-microscopies to inve

140 protein purified from wine, was analyzed by Synchrotron Radiation Circular Dichroism (SRCD) spectros

141 Thermal melt synchrotron radiation circular dichroism spectroscopic b

142 chieved by use of high-resolution (c. 5 mum) synchrotron radiation computed tomography (SRCT) to visu

143 glow emission is generally well explained as synchrotron radiation emitted by electrons accelerated b

144 e billion times greater than is available at synchrotron radiation facilities.

145 temperature, has now been adapted for use in synchrotron radiation facilities.

146 low-angle x-ray diffraction at the European Synchrotron Radiation Facility to check whether the O- t

147 nal cord samples were imaged postmortem at a synchrotron radiation facility.

148 By taking advantage of Synchrotron Radiation Fourier Transform Infrared micro-s

149 generation of X-rays and gamma-rays based on synchrotron radiation from free electrons, emitted in ma

150 tal-organic chemical vapor deposition, using synchrotron radiation high-resolution X-ray diffraction

151 In our studies performed by means of synchrotron radiation induced micro- and submicro-X-ray

152 International synchrotron radiation laboratory.

153 Using high-resolution synchrotron radiation microtomography (SRmuCT), we three

154 The droplet flow is synchronized with synchrotron radiation SAXS measurements to probe protein

155 ution powder X-ray diffraction studies using synchrotron radiation shed light for the first time to t

156 ocage, E. coli bacterioferritin (Bfr), using synchrotron radiation small-angle X-ray scattering (SAXS

157 The high brilliance of modern synchrotron radiation sources facilitates experiments wi

158 ase space for achieving ultrashort undulator synchrotron radiation suitable for users and even for ac

159 sing the "panoramic synthesis" technique and synchrotron radiation to obtain the full reaction map, f

160 canning transmission electron microscopy and synchrotron radiation X-ray absorption spectroscopy toge

161 st time 3D image analysis was carried out by synchrotron radiation X-ray computed microtomography, wh

162 Using high-resolution synchrotron radiation X-ray diffraction, our investigati

163 Here by employing in situ high-pressure synchrotron radiation X-ray diffraction, we reveal a pol

164 sing combined high-resolution laboratory and synchrotron radiation x-ray techniques.

165 Here, using epitaxial thin-film growth, synchrotron radiation, impedance spectroscopy, and densi

166 les." Focusing on the TMD2 fragment, we used synchrotron radiation-based circular dichroism to confir

167 Herein, synchrotron radiation-based high-pressure X-ray diffract

168 Furthermore, synchrotron radiation-based micro-FTIR spectra revealed

169 Operando synchrotron radiation-based X-ray spectroscopic characte

170 In this study, we applied synchrotron radiation-FTIR (SR-FTIR) microspectroscopy a

171 c scanning-by using spectroelectrochemistry, synchrotron radiation-X-ray photoelectron spectroscopy,

172 cts that extend beyond what is possible with synchrotron radiation.

173 band photoelectron spectra using soft X-ray synchrotron radiation.

174 ved photoemission spectroscopy (ARPES) using synchrotron radiation.

175 (STEM) and single-crystal diffraction using synchrotron radiation.

176 erent x-ray diffractive imaging (CXDI) using synchrotron radiation.

177 ation damage artifacts caused by the intense synchrotron radiation.

178 eciprocal space maps during the growth using synchrotron radiation.

179 ons and demonstrate the feasibility of using synchrotron-radiation CD for mechanistic studies of prot

180 ing reaction can be followed by stopped-flow synchrotron-radiation circular dichroism (CD) spectrosco

181 Combining synchrotron-radiation X-ray measurements with spectrosco

182 allenging, but recent advances in high-speed synchrotron radiography now permit the study of highly t

183 present study reports a first application of synchrotron RE-AFM-IR to interrogate biological soft mat

184 to demonstrate not only the applicability of Synchrotron RE-AFM-IR to soft biological matters with su

185 Synchrotron resonance-enhanced infrared atomic force mic

186 Diffraction methods, synchrotron resonant diffraction, and multiple-wavelengt

187 ion of investigative techniques that include synchrotron resonant diffraction, X-ray multiwavelength

188 ermined at 2.0 angstrom resolution by serial synchrotron rotation crystallography at a cryogenic temp

189 in human brain tissue can be achieved using synchrotron scanning transmission x-ray microscopy (STXM

190 observed by a combination of high-resolution synchrotron single-crystal and powder X-ray diffraction

191 Synchrotron single-crystal X-ray data (100 K) allowed th

192 Using synchrotron small angle x-ray scattering (SAXS) techniqu

193 Here we use synchrotron small-angle X-ray diffraction to determine t

194 loride solution are analysed by simultaneous synchrotron small-angle X-ray scattering and Raman spect

195 techniques, including X-ray absorption at a synchrotron source using a customized in situ cell.

196 e use directly the undulator spectrum from a synchrotron source, selecting two separate harmonics pos

197 n can provide an alternative to conventional synchrotron sources for high resolution imaging of eutec

198 with the higher brightness of 4th generation synchrotron sources.

199 ing timing patterns and X-ray pulse width at synchrotron sources.

200 arable to the X-ray pulse width from typical synchrotron sources.

201 electron lasers (XFELs) and, more recently, synchrotron sources.

202 Here we used synchrotron spectromicroscopy to observe the nanoscale m

203 In-situ characterization using synchrotron spectroscopies and density functional theory

204 Advanced synchrotron techniques, post structural characterization

205 ion of PbI(2) excited by X-ray pulses from a synchrotron, thus enabling non-contact in-situ cryotherm

206 Synchrotron tomography and dissection show that the arth

207 -based catalysts is achieved by using online synchrotron vacuum ultraviolet photoionization mass spec

208 tant for new facilities located at XFELs and synchrotrons which often have higher repetition rate, lo

209 Here we have employed in situ synchrotron wide-angle X-ray scattering and transmission

210 rrelation of elemental maps obtained at ANKA synchrotron with qBEI images (quantitative backscattered

211 Electron energy loss and synchrotron X-ray absorption near-edge structure spectro

212 Here, using a combination of synchrotron X-ray absorption spectroscopy and in situ tr

213 Furthermore, in-situ synchrotron X-ray absorption spectroscopy is used for th

214 We use synchrotron X-ray absorption spectroscopy to study the d

215 phase characterization techniques, including synchrotron X-ray absorption, fluorescence, and diffract

216 Here we show from synchrotron X-ray absorption, STEM imaging and DFT model

217 scanning tunneling microscopy/spectroscopy, synchrotron X-ray and angle-resolved photoemission, and

218 A suite of high-resolution synchrotron X-ray characterizations, coupled with a crys

219 tural information, previously obtained using synchrotron X-ray computed tomography (XCT), with synchr

220 -state NMR nuclear magnetic resonance (NMR), synchrotron X-ray diffraction (SXRD), in situ X-ray pair

221 05)O(2) as a model compound, we use operando synchrotron X-ray diffraction (XRD) and nuclear magnetic

222 Microbeam synchrotron X-ray diffraction (XRD) and X-ray fluorescen

223 a high-slope melting curve in molybdenum by synchrotron X-ray diffraction analysis of crystalline mi

224 time-resolved studies, including high-energy synchrotron X-ray diffraction and diffuse reflectance in

225 PFWO single crystals using a combination of synchrotron X-ray diffraction and high-resolution electr

226 tion enables detailed structural analysis by synchrotron X-ray diffraction and high-resolution transm

227 his work, we study MIL-101 under pressure by synchrotron X-ray diffraction and infrared (IR) spectros

228 n and extraction, as demonstrated by in situ synchrotron X-ray diffraction and Raman studies.

229 We combined laboratory and in operando synchrotron X-ray diffraction and scattering experiments

230 uctural and vibrational investigations using synchrotron X-ray diffraction and terahertz spectroscopy

231 n is thoroughly investigated with real-time, synchrotron X-ray diffraction computed tomography, sugge

232 Rietveld refinement using synchrotron X-ray diffraction data reveals the spatial a

233 Here we combine in situ synchrotron X-ray diffraction experiments and computatio

234 n of state of silicon has been determined by synchrotron x-ray diffraction experiments up to 105.2 GP

235 een characterized both experimentally, using synchrotron X-ray diffraction in laser-heated diamond-an

236 ral and tissue mechanics were measured using synchrotron X-Ray diffraction of bone sections under loa

237 g density-functional theory and experimental synchrotron X-ray diffraction studies, we construct a mo

238 scopy, transmission electron microscopy, and synchrotron X-ray diffraction studies.

239 Here, utilizing the synchrotron X-ray diffraction technique, we for the firs

240 We used time-resolved synchrotron X-ray diffraction to study tarantula muscle

241 ility of ruthenium has been investigated via synchrotron X-ray diffraction using a resistively heated

242 d 30 GPa, respectively, using single-crystal synchrotron X-ray diffraction, infrared spectroscopy, an

243 achieved using XPS, TGA-MS, high resolution synchrotron X-ray diffraction, pair distribution functio

244 switching is revealed by joint studies with synchrotron X-ray diffraction, X-ray absorption fine str

245 he associated structural changes via in situ synchrotron X-ray diffraction.

246 laser-heated diamond anvil cell coupled with synchrotron X-ray diffraction.

247 hanges in cellulose were detected by NMR and synchrotron X-ray diffraction.

248 d for the first time based on single-crystal synchrotron X-ray experiments (100-450 K) and transmissi

249 eams, called minibeams, which are known from synchrotron x-ray experiments to spare tissues.

250 Synchrotron X-ray fluorescence and X-ray absorption spec

251 mission-depletion microscopy of proteins and synchrotron X-ray fluorescence imaging of trace metals,

252 Transmitted light microscopy and synchrotron X-ray fluorescence imaging revealed fluctuat

253 We used synchrotron X-ray fluorescence imaging, histology, and i

254 rotron X-ray computed tomography (XCT), with synchrotron X-ray fluorescence microscopy (XRF) and X-ra

255 y screen for iron in the pigeon lagena using synchrotron X-ray fluorescence microscopy coupled with t

256 Here, we employed synchrotron X-ray footprinting to probe the solution-sta

257 combining in-situ high-speed high-resolution synchrotron x-ray imaging experiments and multi-physics

258 A high-speed synchrotron X-ray imaging technique was used to investig

259 We used ultrahigh-speed synchrotron x-ray imaging to quantify the phenomenon of

260 Spatially resolved synchrotron X-ray measurements revealed different charac

261 n Latimeria chalumnae using conventional and synchrotron X-ray micro-computed tomography as well as m

262 ional dynamic visualization study using fast synchrotron X-ray micro-tomography to provide new insigh

263 (MRT) is based on a spatial fractionation of synchrotron X-ray microbeams at the microscale level.

264 t high-resolution virtual sectioning through synchrotron X-ray microcomputed tomography allows a prec

265 y polycrystal is investigated here using the synchrotron X-ray microdiffraction.

266 Semiquantitative synchrotron X-ray microtomography phase mapping requires

267 Here, high-resolution, 3D synchrotron X-ray nano-holotomography images of white ma

268 metal soap deterioration, were studied using synchrotron X-ray nano-tomography and unilateral nuclear

269 Synchrotron X-ray nanofluorescence was applied to map th

270 Benefiting from the recent advances of synchrotron X-ray nanoprobes, we demonstrate three-dimen

271 local structure and phonon vibrations using synchrotron X-ray pair distribution function (PDF) (100-

272 Here, synchrotron X-ray PDF analysis is compared to techniques

273 For the first time, time-lapse synchrotron X-ray phase contrast computed tomography (CT

274 Here we use synchrotron X-ray phase contrast imaging to study cold h

275 iew of the investigated tissue, we exploited synchrotron X-ray phase contrast tomography (XPCT), prov

276 Using synchrotron X-ray phase contrast-enhanced tomography we

277 of the nanoparticles have been determined by synchrotron X-ray photoelectron spectroscopy (XPS), near

278 y the Rietveld refinement of high-resolution synchrotron X-ray powder diffraction (SXRD) data and the

279 Herein, combined solid-state NMR and synchrotron X-ray powder diffraction analyses show the A

280 Through synchrotron x-ray powder diffraction and tomography meas

281 of two solid materials have been solved from synchrotron X-ray powder diffraction data using simulate

282 s type to date) were evaluated using in situ synchrotron X-ray powder diffraction of samples within a

283 tigated in situ with high-speed, high-energy synchrotron X-ray radiography.

284 In this work, synchrotron X-ray reflectivity measurements, accompanied

285 n carbide (SiC) wafers were quantified using synchrotron X-ray rocking curve mapping (RCM), and were

286 -domain thermoreflectance (TDTR) and in situ synchrotron X-ray scattering, we report a reversible, li

287 With the rapid evolution of synchrotron X-ray sources, the demand for high-precision

288 ectron microscopy tools, in conjunction with synchrotron X-ray techniques and first-principle calcula

289 nanoparticles and the capability of in situ synchrotron X-ray techniques in studying the correspondi

290 he recent development of in situ high energy synchrotron X-ray techniques offers an excellent opportu

291 Here, using complementary in situ synchrotron x-ray techniques, we reveal thermal-driven s

292 Here we report, using synchrotron X-ray tomographic imaging of incremental too

293 we report the use of fast low-dose pink-beam synchrotron X-ray tomography in combination with mechani

294 Using synchrotron X-ray tomography, light and transmission ele

295 etical model, first-principles calculations, synchrotron X-ray/neutron diffraction, atom-probe tomogr

296 de a diesel injection nozzle is imaged using synchrotron X-rays from the Advanced Photon Source at Ar

297 r-in-salt" and "salt-in-water" regimes using synchrotron X-rays, which produce electrons at the solid

298 According to depth profile synchrotron XPS and X-ray diffraction (XRD) analysis, me

299 lts obtained from ab initio calculations and synchrotron XPS measurements emphasize the importance of

300 is further investigated by combining in situ synchrotron XRD and solid-state NMR techniques.