ライフサイエンスコーパス: synchrotron

1 excitation source, typically derived from a synchrotron.

2 innovating tools at both the laboratory and synchrotron.

3 resolution x-ray computed tomography using a synchrotron.

4 hrough non-thermal radiation emission called synchrotron.

5 is beyond the capability of 3(rd) generation synchrotrons.

6 oyed for room-temperature data collection at synchrotrons.

7 Based on synchrotron analysis, W was incorporated into the shell

8 od by high-resolution microscopy images, and synchrotron and neutron diffraction experiments, as well

9 ontrast tomography (DCT) using monochromatic synchrotron and polychromatic laboratory X-ray sources h

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

11 Large-scale x-ray sources, such as synchrotrons and x-ray free electron lasers, are becomin

12 or filling the large performance gap between synchrotron- and current X-ray tube-based sources.

13 MgCl2) has been studied experimentally using synchrotron angle-dispersive powder x-ray diffraction an

14 Raman spectroscopy, synchrotron angle-dispersive X-ray diffraction (ADXRD),

15 ver, due to their size and cost, large-scale synchrotrons are not available for more routine applicat

16 were determined using in situ high pressure synchrotron axial and radial x-ray diffraction.

17 We demonstrate here by synchrotron based infrared microspectroscopy in transmis

18 retaining comparable acquisition time to the synchrotron based measurements.

19 focal laser scanning microscopic imaging and synchrotron based microscopic X-ray fluorescence mapping

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

21 apping of Ar atoms is detected in situ using synchrotron-based ambient pressure X-ray photoelectron s

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

23 We apply VUV synchrotron-based experiments combined with state-of-the

24 alinity-induced aggregates was determined by synchrotron-based extended X-ray absorption fine structu

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

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

27 Here, using synchrotron-based high-energy x-ray diffraction and time

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

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

30 's hepatopancreas based on wet chemistry and synchrotron-based investigations.

31 Synchrotron-based Laue microdiffraction has been widely

32 Using a combination of synchrotron-based measurements, empirical dynamic simula

33 Employment of synchrotron-based methods (XPS; reference-free total ref

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

35 ution in duckweed roots was visualized using synchrotron-based micro X-ray fluorescence (XRF) mapping

36 Synchrotron-based nanoprobe X-ray fluorescence (nano-XRF

37 A thorough characterization, including synchrotron-based near edge X-ray absorption fine struct

38 Using a synchrotron-based non-resonant X-ray magnetic diffractio

39 technique are comparable to those with other synchrotron-based PI-TOF-MS reactors, and it is anticipa

40 successfully loaded in the MOF pores, namely synchrotron-based powder diffraction, physisorption anal

41 ve conformations of CypA, confirming earlier synchrotron-based results.

42 Synchrotron-based small- and wide-angle X-ray scattering

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

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

45 The advantages and limitations of these synchrotron-based techniques are discussed and compared

46 In addition, synchrotron-based techniques such as differential pair d

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

48 sequent mineralogical characterization using synchrotron-based X-ray diffraction and X-ray absorption

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

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

51 Here we employ synchrotron-based X-ray fluorescence microscopy (XFM) to

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

53 n UiO-66, UiO-67, MOF-808, and NU-1000 using synchrotron-based X-ray powder diffraction, X-ray absorp

54 articles growing from an Al-Si-Cu liquid via synchrotron-based X-ray tomography.

55 Synchrotron-based XANES data collected in situ on indivi

56 ment of ions during decay and illustrate how synchrotron-based XFM is uniquely suited study these ion

57 Using a synchrotron-based, high-performance XPCI system, we prov

58 ex modifications to a DSC to mount it in the synchrotron beam.

59 that serial millisecond crystallography at a synchrotron beamline equipped with high-viscosity inject

60 in is subject to positional ambiguity at the synchrotron, but is fully resolved with SFX.

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

62 The time resolution for serial synchrotron crystallography experiments has been limited

63 a we collected at a free-electron laser, the synchrotron data are of slightly lower resolution, howev

64 phases were also detected; using the in situ synchrotron data as a guide three of them were isolated

65 more complete than a model determined using synchrotron data from recombinantly produced, much large

66 ion than those of a lower resolution (4.1 A) synchrotron data set.

67 f these alternative conformations with eight synchrotron datasets spanning 100-310 K.

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

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

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

71 In situ synchrotron diffraction reveals no 2-phase transformatio

72 ns of Ti-Nb alloys during heating by in situ synchrotron diffraction.

73 Synchrotron-diffraction experiments and proton-affinity

74 ds would naturally give rise to the observed synchrotron emission in galaxy cores and to the formatio

75 Strong magnetic fields, synchrotron emission, and Compton scattering are omnipre

76 e proposed laboratory instrument and current synchrotron end stations is on the order of several orde

77 estigated with batch kinetic experiments and synchrotron EXAFS analyses.

78 is currently provided by either large-scale synchrotron facilities with limited beamtime access or b

79 ement of high image quality at two different synchrotron facilities, but also with commercial x-ray e

80 Synchrotron facilities, which deliver a beam of high bri

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

82 ts demonstrate Se-SAD, routinely employed at synchrotrons for novel structure determination, is now p

83 ocytic cells (U937) upon IAV infection using synchrotron Fourier-transform infrared (FTIR) and deep U

84 Combining synchrotron-generated monoenergetic X-rays, intracellula

85 is a novel preclinical technique, which uses synchrotron-generated X-rays for the treatment of brain

86 PCBM on the P3HT crystallization dynamics by synchrotron grazing incidence X-ray diffraction.

87 We employ the high-speed synchrotron hard X-ray imaging and diffraction technique

88 nsmission electron microscopy (cryo-TEM) and synchrotron hard X-ray microprobe (SHXM) data sets to pr

89 reach the risky dose level, while classical synchrotron imaging can degrade aDNA significantly.

90 oach, combining histology, microCT and X-ray-synchrotron imaging to shed light on the way these insec

91 1.5-minute intervals using phase-contrast synchrotron imaging, at positive end-expiratory pressure

92 its unerupted permanent teeth, visualized by synchrotron imaging.

93 rformed using the nonperturbing technique of synchrotron infrared absorption.

94 Above 80 GPa, in situ synchrotron infrared experiments show the unequivocal sp

95 enzymes adsorbed on a carbon electrode using synchrotron infrared microspectroscopy combined with pro

96 mononucleotide, to demonstrate the power of synchrotron infrared microspectroscopy relative to conve

97 We then demonstrate the applicability of synchrotron infrared microspectroscopy to adsorbed prote

98 n are elucidated by first-principles theory, synchrotron investigations, ab initio molecular dynamics

99 ement is achieved with small apertures using synchrotron IR relative to a thermal IR source.

100 on site, though not as compact as, e.g., the synchrotron knot.

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

102 ntly, the technique has been extended from a synchrotron light source to utilise a lab-based microfoc

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

104 ted, providing an alternative to large-scale synchrotron light sources.

105 FTIR), and X-ray diffraction (muSR-XRD) with synchrotron light.

106 tions, which leads to elliptically polarized synchrotron-like radiation with flexible tunability on r

107 However, the use of a synchrotron limits practicality and accessibility of XFC

108 positron (antielectron) from the analysis of synchrotron losses at the Large Electron-Positron collid

109 e use bulk and submicron-scale spectroscopic synchrotron methods to examine the in situ transformatio

110 We used synchrotron methods to understand the modes underlying c

111 In situ synchrotron micro X-Ray diffraction, Raman spectroscopy

112 Synchrotron microfocus scanning X-ray diffraction data o

113 Using propagation phase-contrast synchrotron microtomography (PPC-SRmuCT) to visualize th

114 Using X-ray synchrotron microtomography, we show that Rhacolepis fos

115 ation: the macroscopic growth is tracked via synchrotron microtomography, while the submicron feature

116 ploying single crystal X-ray diffraction and synchrotron Mossbauer source spectroscopy.

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

118 inly provided by a few dedicated large-scale synchrotron or free-electron laser (FEL) facilities.

119 The high-energy X-rays of the synchrotron permit the recording of powder diffraction p

120 n in a Pb-free beta-Sn based solder joint by synchrotron polychromatic X-ray microdiffraction.

121 From synchrotron powder diffraction data, we were able to ret

122 harmonic generation (SHG) microscopy-guided synchrotron powder X-ray diffraction (PXRD) for the dete

123 a2S2 --> MS2 + 2 NaCl (M = Fe, Co, Ni) using synchrotron powder X-ray diffraction and differential sc

124 hod using sequential measurements by in situ synchrotron powder X-ray diffraction has been developed

125 Optimised synchrotron protocols and simple rules introduced here a

126 educe the total volume of material probed by synchrotron PXRD.

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

128 compounds were recorded using monochromatic synchrotron radiation and megaelectronvolt (MeV) proton

129 tic X-ray scattering at the N 1s level using synchrotron radiation and the soft X-ray free-electron l

130 itivity were compared to those obtained with synchrotron radiation based 3D confocal mu-X-ray fluores

131 It can also provide synchrotron radiation beam emittance cooling for laser-p

132 The sample compartment for high-throughput synchrotron radiation circular dichroism (HT-SRCD) has b

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

134 Synchrotron radiation circular dichroism spectroscopy co

135 Remarkably, using temperature-dependent synchrotron radiation circular dichroism spectroscopy to

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

137 CPMS imaging was demonstrated to corroborate synchrotron radiation confocal X-ray fluorescence (SR-XR

138 illiance is comparable with third generation synchrotron radiation facilities running at similar phot

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

140 transform infrared (ATR-FTIR) spectroscopy, Synchrotron radiation FTIR (S-FTIR) and Raman microspect

141 Exploiting synchrotron radiation generated by the Imaging and Medic

142 he prompt phase is produced via fast-cooling synchrotron radiation in a large-scale magnetic field th

143 International synchrotron radiation laboratory.

144 Synchrotron radiation phase-contrast computed nanotomogr

145 By using synchrotron radiation photoemission spectroscopy (SRPES)

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

147 Importantly, in addition to the synchrotron radiation source, this approach has been dem

148 s, thus solving the X-ray optical problem at synchrotron radiation sources and X-ray free-electron la

149 The ever-increasing brightness of synchrotron radiation sources demands improved X-ray opt

150 , we perform in situ X-ray diffraction using synchrotron radiation to monitor the pre- and postnuclea

151 Synchrotron radiation X-ray computed microtomography (SR

152 y, an accurate and sensitive method based on synchrotron radiation X-ray computed microtomography (SR

153 reversible, and our in situ high-temperature synchrotron radiation X-ray diffraction experiments at d

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

155 the high elemental sensitivity of microprobe synchrotron radiation X-ray fluorescence (SR-XRF) and X-

156 Synchrotron radiation X-ray tomographic microscopy of th

157 e low energy electrons or vacuum-ultraviolet synchrotron radiation) for product detection with increa

158 While the method is here demonstrated using synchrotron radiation, its low coherence requirements su

159 e a range of methods (including FT-FIR using synchrotron radiation, nanoindentation and skin delivery

160 co's broadband spectrum is characteristic of synchrotron radiation, requiring relativistic electrons.

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

162 both conventional globar and high-resolution synchrotron radiation-based IR sources.

163 py (SEM), atomic force microscopy (AFM), and synchrotron radiation-X-ray photoelectron spectroscopy (

164 n X-ray photoelectron spectroscopy (XPS) and synchrotron radiation-XPS (SR-XPS) analysis of 10-100 nm

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

166 ourier transform far infra-red (FT-FIR) with synchrotron radiation.

167 easured in total reflection conditions using synchrotron radiation.

168 y crystals for structure determination using synchrotron radiation.

169 ation damage artifacts caused by the intense synchrotron radiation.

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

171 ached to catalytic particles is mapped using synchrotron-radiation-based infrared nanospectroscopy wi

172 nd microspectroscopic characterization using synchrotron-radiation-based X-ray absorption spectroscop

173 d printed circuit boards has been studied by synchrotron radiography.

174 bule bundles at 37 degrees C, as revealed by synchrotron SAXS and TEM.

175 The discovery, preparation, and synchrotron scanning of the Australopithecus afarensis p

176 aphic data and can be routinely collected at synchrotrons.Serial crystallography was developed for pr

177 Here we show by synchrotron small-angle X-ray diffraction of frog (Rana

178 Using synchrotron small-angle X-ray diffraction to probe time-

179 raumatic and traumatic fracture states using synchrotron small-angle x-ray scattering (SAXS) at low a

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

181 iolet excitation provided by DISCO beamline (synchrotron Soleil) combined with microscopy allows spec

182 "dip &pull" approach, with a "tender" X-ray synchrotron source (2 keV-7 keV), we are able to access

183 transient absorption (XTA) spectroscopy at a synchrotron source as a relaxed (d,d) state, the lowest

184 l angle x-ray scattering at a high intensity synchrotron source, combined with model-free analysis of

185 d using a free electron laser or ultrabright synchrotron source, provides significantly more experime

186 ) experiments using the high X-ray flux of a synchrotron source.

187 escribed that couples the high brilliance of synchrotron-sourced infrared microscopy with attenuated

188 Tunable synchrotron-sourced photoionization time-of-flight mass

189 ial crystallography at last generation X-ray synchrotron sources and free electron lasers enabled dat

190 At low emittance synchrotron sources it has become possible to perform st

191 oCT for bovine tail IVD using laboratory and synchrotron sources.

192 es that are difficult to solve using current synchrotron sources.

193 und ratios as those which can be obtained at synchrotron sources.

194 ter timescales in diffraction experiments at synchrotron sources.

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

196 from red abalone (Haliotis rufescens), using synchrotron spectromicroscopy.

197 In contrast, in the synchrotron structure, the Fe-CO bond is cleaved; CO rel

198 fer on a time scale that has eluded previous synchrotron studies.

199 These complementary synchrotron techniques required minimal sample preparati

200 aging and Medical Beamline at the Australian Synchrotron, we studied radiation-induced nontargeted ef

201 This was confirmed with synchrotron X-ray absorption near edge structure measure

202 X-ray diffraction (HT-XRD), ex-situ XRD and synchrotron X-ray absorption near edge structure spectro

203 emical characterization techniques including synchrotron X-ray absorption spectroscopy (XAS) and theo

204 micrometric mapping of Ce speciation through synchrotron X-ray absorption spectroscopy and production

205 sion electron microscopy in conjunction with synchrotron X-ray absorption spectroscopy, we show that

206 Here we demonstrate how synchrotron X-ray analyses can non-destructively charact

207 t pressure, as evidenced by real-time powder synchrotron X-ray and neutron diffraction, and second ha

208 Thorough investigation by synchrotron X-ray and neutron powder diffraction indicat

209 ng the intense radiation fields of a focused synchrotron x-ray beam, we drove dissolution at the calc

210 Mice were locally irradiated with a synchrotron X-ray broad beam and a multiplanar microbeam

211 e we perform in situ mechanical testing with synchrotron X-ray computed micro-tomography at temperatu

212 Importantly, synchrotron X-ray computed microtomography (SR-muCT) all

213 the first time the application of high-speed synchrotron X-ray computed tomography and radiography, i

214 The new cages were characterized by synchrotron X-ray crystallography, high-resolution mass

215 direction) were characterized by local probe synchrotron X-ray diffraction (mu-XRD) using a focused X

216 We present in situ high-pressure synchrotron X-ray diffraction (XRD) and Raman spectrosco

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

218 icroscopy, electron microprobe analysis, and synchrotron X-ray diffraction analysis.

219 High-resolution synchrotron X-ray diffraction and high-resolution transm

220 of MAPbI3 (MA=methylammonium) using in situ synchrotron X-ray diffraction and laser-excited photolum

221 Synchrotron X-ray diffraction and pair distribution func

222 ysis of the reaction coordinate with in situ synchrotron X-ray diffraction and pair distribution func

223 We combine synchrotron X-ray diffraction and Raman spectroscopy in

224 These phases were identified using in situ synchrotron X-ray diffraction and Raman spectroscopy.

225 o permeate model prokaryotic membranes using synchrotron x-ray diffraction and that it is sufficient

226 izations are performed by the combination of synchrotron X-ray diffraction at small angles and in sit

227 s are simultaneously monitored using in situ synchrotron X-ray diffraction during the growth of BaTiO

228 Using synchrotron x-ray diffraction in diamond anvil cells and

229 Here, using synchrotron x-ray diffraction in laser-heated diamond an

230 Synchrotron x-ray diffraction measurements demonstrate t

231 Angle-dispersive synchrotron X-ray diffraction measurements on Ir2P powde

232 In situ synchrotron X-ray diffraction monitoring of the reaction

233 Here, we show using synchrotron X-ray diffraction on high-pO2 floating zone-

234 In situ synchrotron X-ray diffraction studies were conducted in

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

236 performed measurements of Raman scattering, synchrotron x-ray diffraction, and visible transmission

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

238 Based on in situ synchrotron X-ray diffraction, the mechanism of the room

239 ect how the amorphous phases form, including synchrotron X-ray diffraction, transmission electron mic

240 and near the glass transition temperature by synchrotron X-ray diffraction, uncovering novel behaviou

241 mes too small for structure determination by synchrotron X-ray diffraction, we use micro-electron dif

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

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

244 integrated technique of laser-heated DAC and synchrotron X-ray diffraction.

245 In situ synchrotron X-ray diffuse scattering and inelastic neutr

246 of micronutrient localization in seeds using synchrotron X-ray fluorescence (SXRF).

247 ion electron microscopy with micro- and nano-synchrotron X-ray fluorescence to image unequivocally fo

248 Here we investigate the effects of synchrotron X-ray irradiation on aDNA from Pleistocene b

249 the trabecular bone core was performed using synchrotron X-ray micro-CT linked to image analysis soft

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

251 re mostly formed in isolation as revealed by synchrotron X-ray micro-tomography.

252 Synchrotron X-ray microdiffraction (SXRD) and scanning e

253 Here we employ synchrotron X-ray microdiffraction to evaluate the quali

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

255 unsaturated sand packs were measured with a synchrotron X-ray microprobe, and inverse modeling was u

256 An in situ synchrotron X-ray microtomography experiment, flowing CO

257 Using time-resolved (4D) synchrotron X-ray microtomography we have imaged a compl

258 Synchrotron X-ray nanofluorescence was applied to map th

259 The synchrotron X-ray pair distribution function acquired be

260 High-energy synchrotron X-ray pair distribution function analysis co

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

262 Here, we use the high-spatial resolution of synchrotron X-ray Photo Emission Electron Microscopy (XP

263 report a powerful new technique: hyphenating synchrotron X-ray powder diffraction (XRD) with differen

264 lite SSZ-70 has been elucidated by combining synchrotron X-ray powder diffraction (XRPD), high-resolu

265 nitored the progress of milling reactions by synchrotron X-ray powder diffraction (XRPD).

266 Synchrotron X-ray powder diffraction and Rietveld refine

267 Through synchrotron x-ray powder diffraction and tomography meas

268 By using new-generation in situ synchrotron X-ray powder diffraction combined with Rietv

269 s, low temperature phase was determined from synchrotron X-ray powder diffraction data and its densit

270 High-resolution synchrotron X-ray powder diffraction reveals a continuou

271 Using high-energy in situ synchrotron X-ray powder diffraction, we monitor the cry

272 Through in situ synchrotron X-ray powder diffraction, we visualize how t

273 de (MAPbI3) using time-of-flight neutron and synchrotron X-ray powder diffraction.

274 ersensitive to X-ray photons used in typical synchrotron X-ray protein crystallography experiments.

275 Using a single 100 ps synchrotron x-ray pulse, we have measured, by K-edge abs

276 vant FTS conditions and monitored in situ by synchrotron X-ray radiation.

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

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

279 al pair distribution functions obtained from synchrotron X-ray scattering confirmed that isolated oxo

280 Our findings demonstrate that synchrotron X-ray scattering is a viable method for stud

281 Here, advanced nondestructive wide-angle synchrotron X-ray scattering techniques combined with sc

282 show through a direct comparison of in situ synchrotron X-ray scattering with density functional the

283 Here, by using in situ synchrotron X-ray scattering, we show that in the hetero

284 orporated into lab-based and next-generation synchrotron X-ray sources, they bring unprecedented desi

285 -1 under several endmember conditions, using synchrotron X-ray spectroscopic measurements complemente

286 icles, which is further confirmed by in-situ synchrotron X-ray studies and large-scale simulation.

287 Through a combination of synchrotron X-ray techniques and high-resolution images

288 grees C over 1 week through a combination of synchrotron X-ray techniques and wet-chemical analyses.

289 a 15th century oil painting was examined by synchrotron X-ray techniques.

290 ng a specialized thermomechanical setup to a synchrotron X-ray tomographic microscopy endstation at t

291 Using quantitative in situ synchrotron X-ray tomographic microscopy, we show an add

292 Both synchrotron X-ray tomography and EBSD characterization r

293 quantified in 3D by means of high resolution synchrotron X-ray tomography.

294 17.5Cu5 metallic glass is investigated using synchrotron x-ray total scattering method up to 38.4 GPa

295 A bright mum-sized source of hard synchrotron x-rays (critical energy Ecrit > 30 keV) base

296 Using synchrotron X-rays and Raman spectroscopy we challenge t

297 provides a useful means to focus high-energy synchrotron X-rays from a bending magnet or wiggler sour

298 charomyces cerevisiae)--using hard (7.9 keV) synchrotron x-rays.

299 Complementary measurements by Raman and synchrotron XRD are in excellent agreement with the clas

300 fferent pathways using in-situ STEM, in-situ synchrotron XRD, and DFT electronic structure calculatio