ライフサイエンスコーパス: photoelectron

1 rom the inelastic scattering of the outgoing photoelectron.

2 ly 20 eV) significantly less than low-energy photoelectrons.

3 eading to better harvesting of the generated photoelectrons.

4 luster packing on both supports, while x-ray photoelectron and absorption spectroscopy demonstrate a

5 ess this, we utilized a combination of X-ray photoelectron and absorption spectroscopy to identify al

6 tetracyanobenzene anion (TCNB(-)) using both photoelectron and photodetachment spectroscopies of cryo

7 this review, recent experimental advances in photoelectron and photoelectron-photofragment coincidenc

8 We provide evidence via complementary X-ray photoelectron and Raman spectroscopy that sputter deposi

9 ke important contributions to the low-energy photoelectron and secondary electron spectrum from many

10 These interactions between spin-polarized photoelectrons and chiral molecules are physically manif

11 We continuously control the energy of the photoelectrons and introduce an asymmetry in their emiss

12 s-phase are observed, as is the liquid-phase photoelectron angular anisotropy.

13 rferences of pathways can be observed in the photoelectron angular distribution and in the past they

14 hat considers the Coulomb-laser coupling and photoelectron angular distribution in streaking trace ge

15 o show that screening influences high-energy photoelectrons ( approximately 20 eV) significantly less

16 High energy photoelectrons are shown to be a powerful tool for molec

17 sses owing to a greater yield of the trapped photoelectrons being extracted to the external circuit.

18 As a result, high-energy photoelectrons can serve as a direct probe of spin-depen

19 Spectral modeling of photoelectrons can serve as a valuable tool when combine

20 This phenomenon is consistent with the photoelectron data, which shows depletion in the spectra

21 es, and show a full real-time picture of the photoelectron dynamics in the combined action of the las

22 spectra, which contain signatures of direct photoelectron emission as well as emission of thermalize

23 Further, a photoelectron emission model is proposed to describe lig

24 This process is attributed to the photoelectron emission of the charges trapped in the sur

25 opy, whereby the kinetic energy and angle of photoelectrons emitted from a sample surface are measure

26 ral information that extends well beyond the photoelectron escape depth.

27 ere we use a combination of liquid-jet X-ray photoelectron experiments and molecular dynamics simulat

28 h photoemission we show that the lifetime of photoelectrons from the d band of Cu are longer by appro

29 the nonadiabatic subcycle ionization on the photoelectron hologram.

30 Strong field photoelectron holography has been proposed as a means fo

31 instant of photoexcitation, energy-resolved photoelectron images revealed a highly non-equilibrium d

32 ride clusters are studied by high-resolution photoelectron imaging and ab initio calculations.

33 B(6)(-) and AlB(6)(-), using high-resolution photoelectron imaging and quantum chemical calculations.

34 In a high-resolution photoelectron imaging and theoretical study of the IrB(3

35 Here, femtosecond time-resolved photoelectron imaging is used to show that photoexcitati

36 range of wavelengths using a high-resolution photoelectron imaging spectrometer, which reveal both th

37 ctroscopy (NIPES) along with high-resolution photoelectron imaging spectroscopy.

38 Here, we use time-resolved photoelectron imaging to probe the isomerisation coordin

39 cular ionization cross sections arising from photoelectron impact, possibly resulting in spin-polariz

40 The mechanism behind this photoelectron-induced reduction was revealed to be conce

41 The photoelectron is pulled out from a localized inner-shell

42 f the material band structure in determining photoelectron lifetimes and corresponding electron escap

43 anges to the rapid evolution of high-density photoelectron mediated secondary collisional ionization

44 aces was directly visualized by the scanning photoelectron microscopy (SPEM), in particular for the c

45 We use ultrafast nonlinear coherent photoelectron microscopy to generate attosecond videos o

46 the time-energy relation in molecular-frame photoelectron momentum distributions shows the way of pr

47 t experimental advances in photoelectron and photoelectron-photofragment coincidence spectroscopy are

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

49 Our results demonstrate that the photoelectron signal dispersed in time, energy and angle

50 Peaks in the photoelectron spectra are considerably narrower than in

51 Well-resolved photoelectron spectra are obtained and interpreted with

52 Vibrationally resolved photoelectron spectra have been obtained and compared wi

53 C-O moieties in HA determined from the X-ray photoelectron spectra of the C 1s region.

54 Here we report on photoelectron spectra of the C[Formula: see text] anion,

55 The operando photoelectron spectra support assignment of these newly

56 e to record both valence and core-level band photoelectron spectra using soft X-ray synchrotron radia

57 By comparing experimental photoelectron spectra with time-dependent density functi

58 tKAN3H8b(-) yield tautomer-specific resonant photoelectron spectra.

59 Ultraviolet photoelectron spectral readouts display the changes in t

60 Ultraviolet photoelectron spectral widths were found to depend on su

61 Herein, we present a combined anion photoelectron spectroscopic and density functional theor

62 s, multinuclear NMR ((1)H, (11)B), and X-ray photoelectron spectroscopic characterization.

63 ar PbTiO(3) matrix, as revealed by our x-ray photoelectron spectroscopic results.

64 Here, we present a gas-phase photoelectron spectroscopic study on the archetypical io

65 e in excellent agreement with a recent anion photoelectron spectroscopic study.

66 UV-Vis, far-IR, and X-ray photoelectron spectroscopies evidence the reduction of H

67 reduced and characterized by Raman and X-ray photoelectron spectroscopies in addition to microscopies

68 (23)Na solid-state NMR, Mossbauer, and X-ray photoelectron spectroscopies, are employed as probes of

69 crystal arrays is confirmed via infrared and photoelectron spectroscopies.

70 IF) spectrometry, and ambient-pressure X-ray photoelectron spectroscopy (AP-XPS).

71 um mechanics (QM) and ambient-pressure X-ray photoelectron spectroscopy (APXPS) experiments.

72 Here, we show that ambient pressure X-ray photoelectron spectroscopy (APXPS) with a conventional X

73 s was performed using ambient pressure X-ray photoelectron spectroscopy (APXPS), Fourier transform in

74 A combination of near-ambient pressure X-ray photoelectron spectroscopy (NAP-XPS) and CO temperature-

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

76 (-) anions were investigated by negative ion photoelectron spectroscopy (NIPES) along with high-resol

77 nvestigated in the gas phase by negative-ion photoelectron spectroscopy (NIPES), velocity-map imaging

78 scopy (AFM), and synchrotron radiation-X-ray photoelectron spectroscopy (SR-XPS) were used to elucida

79 th temperature, temperature-programmed X-ray photoelectron spectroscopy (TP-XPS) experiments are perf

80 evel offset (epsilon(h)(UPS)) by ultraviolet photoelectron spectroscopy (UPS) for CnT and CnDT SAMs a

81 asurements of epsilon(h)(UPS) by ultraviolet photoelectron spectroscopy (UPS) for OPT n and OPD n SAM

82 lectrical conductors and exhibit ultraviolet-photoelectron spectroscopy (UPS) signatures expected of

83 soft X-ray scattering (R-SoXS); ultraviolet photoelectron spectroscopy (UPS); Fourier transform-infr

84 y ion mass spectrometry (ToF-SIMS) and X-ray photoelectron spectroscopy (XPS) analyses indicated bind

85 X-ray photoelectron spectroscopy (XPS) analysis revealed that

86 Report, Nakamura et al argue that our x-ray photoelectron spectroscopy (XPS) analysis was affected b

87 as a valuable tool when combined with X-ray photoelectron spectroscopy (XPS) analysis.

88 t X-ray absorption spectroscopy (XAS), X-ray photoelectron spectroscopy (XPS) and atomic multiplet cl

89 X-ray photoelectron spectroscopy (XPS) and attenuated total re

90 X-ray photoelectron spectroscopy (XPS) and electrochemical imp

91 cterization of the prepared samples by X-ray photoelectron spectroscopy (XPS) and optimization of the

92 substrate electrode surfaces based on X-ray photoelectron spectroscopy (XPS) and synchrotron radiati

93 ystem performance is validated through X-ray photoelectron spectroscopy (XPS) and the spatial distrib

94 ution interface, and observe with both X-ray photoelectron spectroscopy (XPS) and XUV-RA the existenc

95 scopy (FTIR), X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS) and zeta potential meas

96 entified by fitting of high-resolution X-ray photoelectron spectroscopy (XPS) C 1s and O 1s spectra.

97 nning electron microscopy (FE-SEM) and X-ray photoelectron spectroscopy (XPS) characterization result

98 X-ray photoelectron spectroscopy (XPS) characterized a transie

99 dded within the polymer matrix, whilst X-ray Photoelectron Spectroscopy (XPS) confirmed that they exi

100 Infrared spectroscopy (ATR-FTIR) and X-ray photoelectron spectroscopy (XPS) confirmed the role of p

101 Nuclear magnetic resonance (NMR) and X-ray photoelectron spectroscopy (XPS) demonstrate formation o

102 Nuclear magnetic resonance (NMR) and X-ray photoelectron spectroscopy (XPS) demonstrate the covalen

103 ure published data obtained by in situ X-ray photoelectron spectroscopy (XPS) for the concentration o

104 studied for their HER activity and by X-ray photoelectron spectroscopy (XPS) for the first time; MoB

105 g Microscopy (STM) in combination with X-ray Photoelectron spectroscopy (XPS) has been utilized to ch

106 electron microscopy (PEEM) and imaging X-ray photoelectron spectroscopy (XPS) have over the years bee

107 X-ray photoelectron spectroscopy (XPS) is one of the most used

108 X-ray photoelectron spectroscopy (XPS) measurements confirms n

109 asma-Mass Spectrometry (LA-ICP-MS) and X-ray photoelectron spectroscopy (XPS) measurements, which wer

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

111 ed here using a combination of SPR and X-ray photoelectron spectroscopy (XPS) measurements.

112 Ex situ X-ray photoelectron spectroscopy (XPS) of the 2-ABT modified e

113 Raman and X-Ray photoelectron spectroscopy (XPS) revealed that the synth

114 ) While surface characterization using X-ray photoelectron spectroscopy (XPS) showed the presence of

115 Fourier transform infrared (FTIR), and X-ray photoelectron spectroscopy (XPS) spectroscopy confirmed

116 cterizations by Raman spectroscopy and X-ray photoelectron spectroscopy (XPS) support the presence of

117 Zeta potential measurements and X-ray photoelectron spectroscopy (XPS) were used to analyse th

118 y-dispersive X-ray spectroscopy (EDS), X-ray photoelectron spectroscopy (XPS), and (10)B and (11)B so

119 ransmission Electron Microscopy (TEM), X-ray Photoelectron Spectroscopy (XPS), and Nanoparticle Size

120 -ray spectroscopy (EDS), quasi in situ X-ray photoelectron spectroscopy (XPS), and operando X-ray abs

121 sion electron microscopy (HAADF-STEM), X-ray photoelectron spectroscopy (XPS), and powder X-ray diffr

122 , X-ray absorption spectroscopy (XAS), X-ray photoelectron spectroscopy (XPS), and Raman microscopy.

123 Various techniques, such as X-ray photoelectron spectroscopy (XPS), confirmed the occurren

124 spectroscopy, photoluminescence (PL), x-ray photoelectron spectroscopy (XPS), Fourier transform infr

125 Fluorescence detection, X-ray photoelectron spectroscopy (XPS), infrared spectra (FT-I

126 es have been determined by synchrotron X-ray photoelectron spectroscopy (XPS), near-edge X-ray absorp

127 ional theory (DFT), ion chromatograph, X-ray photoelectron spectroscopy (XPS), particle size analysis

128 ochemical exposure in combination with X-ray photoelectron spectroscopy (XPS), scanning electron micr

129 odified surfaces were characterized by X-ray photoelectron spectroscopy (XPS), scanning electron micr

130 opy, X-ray diffraction analysis (XRD), X-ray photoelectron spectroscopy (XPS), UV-Vis-NIR spectroscop

131 ure characterization methods including X-ray photoelectron spectroscopy (XPS), V and S X-ray absorpti

132 erometry, cyclic voltammetry (CV), and X-ray photoelectron spectroscopy (XPS), we demonstrate that hi

133 ransmission electron microscopy (TEM), X-ray photoelectron spectroscopy (XPS), X-ray diffraction (XRD

134 ), powder X-ray diffraction (PXRD) and X-ray photoelectron spectroscopy (XPS).

135 ochemical mass spectrometry (OEMS) and X-ray photoelectron spectroscopy (XPS).

136 hment on the compacts was confirmed by X-ray photoelectron spectroscopy (XPS).

137 ng was observed based on quasi in situ X-ray photoelectron spectroscopy (XPS).

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

139 ng electron microscopy (SEM) and Fe 2p X-ray photoelectron spectroscopy (XPS).

140 er (VSM), X-ray diffraction (XRD), and X-ray photoelectron spectroscopy (XPS).

141 ), surface plasmon resonance (SPR) and X-ray photoelectron spectroscopy (XPS).

142 mission electron microscopy (TEM), and X-ray photoelectron spectroscopy (XPS).

143 iO2 powder using near-ambient-pressure X-ray photoelectron spectroscopy (XPS).

144 smission electron microscopy (TEM) and X-ray photoelectron spectroscopy (XPS).

145 mly modified columns were assessed via X-ray photoelectron spectroscopy (XPS).

146 n and Brunauer Emmett-Teller (BET) and X-ray Photoelectron Spectroscopy (XPS).

147 sform infrared spectroscopy (FTIR) and X-ray photoelectron spectroscopy (XPS).

148 Angle-resolved X-ray photoelectron spectroscopy analyses indicate that GNSs c

149 Evidence from high resolution X-ray photoelectron spectroscopy analyses indicated that the u

150 X-ray photoelectron spectroscopy analysis confirmed the presen

151 The X-ray photoelectron spectroscopy analysis confirms the presenc

152 probable adsorption mechanism based on X-ray photoelectron spectroscopy analysis was also proposed in

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

154 d the reduction of Cr(VI) according to X-ray photoelectron spectroscopy analysis.

155 of a mixed B/Bi target and characterized by photoelectron spectroscopy and ab initio calculations.

156 we report the results obtained via combined photoelectron spectroscopy and ab initio studies of the

157 egradation mechanism of GaS(0.87) with X-ray photoelectron spectroscopy and annular dark-field scanni

158 ating voltage regions, as confirmed by X-ray photoelectron spectroscopy and atomic force microscopy e

159 and 8-hydroxyquinoline molecules using anion photoelectron spectroscopy and density functional theory

160 Here, a combined anion photoelectron spectroscopy and density functional theory

161 ion of oxygen defects as determined by X-ray photoelectron spectroscopy and electron paramagnetic res

162 ion, and characterized by a synergy of anion photoelectron spectroscopy and electronic structure calc

163 Using X-ray photoelectron spectroscopy and Fourier transform infrare

164 In the present study, we employed X-ray photoelectron spectroscopy and Fourier-transform infrare

165 Using operando ambient pressure X-ray photoelectron spectroscopy and high pressure scanning tu

166 With the aid of experimental photoelectron spectroscopy and highly correlated ab init

167 Furthermore, valence band analysis by X-ray photoelectron spectroscopy and photoluminescence spectro

168 be H-Pt-CH(3) (-) by a synergy between anion photoelectron spectroscopy and quantum chemical calculat

169 C-Pt-H(CO(2))](-) by a synergy between anion photoelectron spectroscopy and quantum chemical calculat

170 on cluster (PrB7(-) ) are investigated using photoelectron spectroscopy and quantum chemistry.

171 (-) and ReB(2) O(-) and investigated them by photoelectron spectroscopy and quantum-chemical calculat

172 y infrared, electronic absorption, and X-ray photoelectron spectroscopy and revealed formation of a s

173 olled electron-impact irradiation with X-ray photoelectron spectroscopy and scanning electron microsc

174 haracterized using Raman spectroscopy, X-ray photoelectron spectroscopy and scanning tunneling micros

175 nd probed their structures and bonding using photoelectron spectroscopy and theoretical calculations.

176 rk, where temperature-dependent negative ion photoelectron spectroscopy and theoretical studies demon

177 r anions (Bn-) have allowed systematic joint photoelectron spectroscopy and theoretical studies, reve

178 roscopy, scanning electron microscopy, X-ray photoelectron spectroscopy and transmission electron mic

179 troscopy, powdered X-ray spectroscopy, X-ray photoelectron spectroscopy and UV-Vis diffused reflectan

180 ristics were assessed by TEM, SEM-EDX, X-ray photoelectron spectroscopy and vibrating sample magnetom

181 to bind with mercury as determined by X-ray photoelectron spectroscopy and X-ray absorption fine str

182 vanced in situ electron microscopy and X-ray photoelectron spectroscopy are used to demonstrate that

183 al organic films was analyzed by ultraviolet photoelectron spectroscopy at room temperature.

184 Photoelectron spectroscopy confirms that Ag acts as a p-

185 Temperature-programmed desorption and X-ray photoelectron spectroscopy data provide information abou

186 r at surfaces and interfaces, angle-resolved photoelectron spectroscopy has become a core technique i

187 Experiments using ambient pressure X-ray photoelectron spectroscopy indicate that methane dissoci

188 Using ambient pressure X-ray photoelectron spectroscopy interpreted with quantum mech

189 Recent angle-resolved photoelectron spectroscopy investigations provided insig

190 Hard-x-ray photoelectron spectroscopy is a valuable source of infor

191 Finally, X-ray photoelectron spectroscopy is used to characterize the P

192 Here we report liquid jet X-ray photoelectron spectroscopy measurements that provide dir

193 Photoelectron spectroscopy of microjets expanded into va

194 quantum state specificity by high-resolution photoelectron spectroscopy of the vinylidene anions H2CC

195 X-ray photoelectron spectroscopy of these electrochemically tr

196 Raman and X-ray photoelectron spectroscopy on BN films show no significa

197 by means of operando ambient-pressure X-ray photoelectron spectroscopy performed at the solid/liquid

198 troscopy, scanning tunneling microscopy, and photoelectron spectroscopy provide unique information ab

199 X-ray photoelectron spectroscopy recommends the chemical inter

200 The X-ray photoelectron spectroscopy results indicated that Fe(0)

201 g and predominated the powder surface (X-ray photoelectron spectroscopy results) in both camel and bo

202 ay absorption spectroscopy and ex situ X-ray photoelectron spectroscopy reveal that PbO(2) is unpertu

203 nctional theory calculations and ultraviolet photoelectron spectroscopy reveal that the effective wor

204 oscopy together with ex situ Raman and X-ray photoelectron spectroscopy reveal the reversibility of m

205 X-ray photoelectron spectroscopy revealed significant core-lev

206 X-ray photoelectron spectroscopy revealed that an effective mo

207 X-ray photoelectron spectroscopy revealed that the hydroxyl gr

208 Angle-resolved photoelectron spectroscopy reveals a quasi-1D valence ba

209 X-ray photoelectron spectroscopy reveals that, at pH </= 3.5,

210 upled with atomic force microscopy and X-ray photoelectron spectroscopy reveals the architectures to

211 In situ ambient pressure X-ray photoelectron spectroscopy reveals up to a fourfold enha

212 yst during the reaction, quasi in situ X-ray photoelectron spectroscopy showed that the surface is me

213 Ambient-pressure x-ray photoelectron spectroscopy showed that water added to me

214 X-ray absorption spectroscopy and X-ray photoelectron spectroscopy studies of SNNO/LSMO heterost

215 aramagnetic resonance spectroscopy and X-ray photoelectron spectroscopy studies suggest that the chem

216 aramagnetic resonance spectroscopy and X-ray photoelectron spectroscopy studies suggested that the ch

217 UV-vis spectroscopy and X-ray photoelectron spectroscopy suggest that a substituent's

218 X-ray photoelectron spectroscopy suggests that NaCu(4)Se(4) is

219 rcame this limitation by applying soft x-ray photoelectron spectroscopy to characterize excess electr

220 We employed ambient pressure X-ray photoelectron spectroscopy to investigate the electronic

221 d X-ray diffraction, and Mossbauer and X-ray photoelectron spectroscopy to investigate their morpholo

222 8H8I2) produces m-C8H8 in gas phase; we used photoelectron spectroscopy to probe the first two electr

223 hanges in the physical properties of SAMs to photoelectron spectroscopy to unambiguously assign bindi

224 mbient conditions and (ii) contactless X-ray photoelectron spectroscopy under ultrahigh vacuum.

225 X-ray photoelectron spectroscopy was used to characterize the

226 properties with degree of functionalization, photoelectron spectroscopy was used to map the occupied

227 ering beyond the dipole limit and hard X-ray photoelectron spectroscopy we establish the dual nature

228 croscopy, X-ray diffraction, Raman and X-ray photoelectron spectroscopy were employed to characterize

229 transmission electron microscopy, and X-ray photoelectron spectroscopy were used to understand the n

230 Here we apply time-resolved photoelectron spectroscopy with a seeded extreme ultravi

231 Here we combine ambient pressure X-ray photoelectron spectroscopy with quantum mechanics to exa

232 Nuclear magnetic resonance(11), X-ray photoelectron spectroscopy(12) and cryogenic transmissio

233 structural and transport measurements, X-ray photoelectron spectroscopy, and ab initio calculations a

234 ed by scanning tunneling spectroscopy, X-ray photoelectron spectroscopy, and complementary density fu

235 y, grazing incident X-ray diffraction, X-ray photoelectron spectroscopy, and Fourier transform infrar

236 d using a quartz crystal microbalance, X-ray photoelectron spectroscopy, and infrared spectroscopy, s

237 urier transform infrared spectroscopy, X-ray photoelectron spectroscopy, and ion-exchange measurement

238 X-ray spectroscopy, X-ray diffraction, X-ray photoelectron spectroscopy, and nitrogen adsorption-deso

239 O-poor environment, in agreement with X-ray photoelectron spectroscopy, and O-H bond formation of H

240 ectron microscopy and energy-dependent X-ray photoelectron spectroscopy, and prove the existence of v

241 heir intermediate phases of borophene; X-ray photoelectron spectroscopy, and scanning tunneling micro

242 ed reflection/absorption spectroscopy, X-ray photoelectron spectroscopy, and surface plasmon resonanc

243 scopic images before and after growth, x-ray photoelectron spectroscopy, and x-ray diffraction invest

244 n microscopy, ultra violet-visible and X-ray photoelectron spectroscopy, and Zeta-potential.

245 immobilization, which was confirmed by X-ray Photoelectron Spectroscopy, Atomic Force Microscopy and

246 ound molecules through high-resolution X-ray photoelectron spectroscopy, atomic force microscopy, and

247 ay diffraction, magnetic measurements, X-ray photoelectron spectroscopy, cyclic voltammetry, and dens

248 We employed microwave conductivity, X-ray photoelectron spectroscopy, diffuse reflectance spectros

249 eparation was directly proved by ultraviolet photoelectron spectroscopy, electrochemical impedance sp

250 xposed samples were investigated using X-ray photoelectron spectroscopy, Fourier transform infrared s

251 he trade include near-ambient-pressure X-ray photoelectron spectroscopy, high-pressure scanning tunne

252 ully studied by X-ray crystallography, X-ray photoelectron spectroscopy, hydrogen evolution experimen

253 y forming the Mo Se bond, confirmed by X-ray photoelectron spectroscopy, in which the formed MoSe(2)

254 d by transmission electron microscopy, X-ray photoelectron spectroscopy, infrared spectra, ultraviole

255 s of the foam were characterized using X-ray photoelectron spectroscopy, inverse gas chromatography,

256 Combined with in situ ambient-pressure X-ray photoelectron spectroscopy, IR, and Raman spectroscopic

257 lectrochemistry, synchrotron radiation-X-ray photoelectron spectroscopy, near edge X-ray absorption f

258 in the AuNP suspensions, as judged by X-ray photoelectron spectroscopy, nuclear magnetic resonance e

259 X-ray photoelectron spectroscopy, Raman spectroscopy, together

260 DFT calculations, X-ray photoelectron spectroscopy, Raman, and FTIR show that th

261 formation of the SAM was confirmed by X-ray photoelectron spectroscopy, scanning electron microscopy

262 urier transform infrared spectroscopy, X-ray photoelectron spectroscopy, scanning electron microscopy

263 s formation are elucidated by means of X-Ray photoelectron spectroscopy, scanning transmission electr

264 Through X-ray diffraction and X-ray photoelectron spectroscopy, the as-grown tungsten(VI) su

265 Scanning electron microscopy, X-ray photoelectron spectroscopy, transmission electron micros

266 X-ray diffraction, Raman spectroscopy, X-ray photoelectron spectroscopy, UV-vis absorption spectra, a

267 r the metallic glasses, measured using X-ray photoelectron spectroscopy, was higher by 0.2 eV to 0.4

268 LTS reaction, as well as complementary X-ray photoelectron spectroscopy, we observed the activation a

269 A powerful approach is angle-resolved photoelectron spectroscopy, whereby the kinetic energy a

270 In situ techniques (X-ray photoelectron spectroscopy, X-ray absorption spectroscop

271 mbination of powder X-ray diffraction, X-ray photoelectron spectroscopy, X-ray fluorescence spectrosc

272 spectroscopy, Raman spectroscopy, and X-ray photoelectron spectroscopy.

273 n iron-deficient sulfide, according to X-ray photoelectron spectroscopy.

274 including XRD, electron microscopy and X-ray photoelectron spectroscopy.

275 silicon substrate, as demonstrated by X-ray photoelectron spectroscopy.

276 croscopy, X-ray diffraction, Raman and X-ray photoelectron spectroscopy.

277 spin resonance, UV-vis-NIR, and ultraviolet photoelectron spectroscopy.

278 s decrease of Mn valence measured from X-ray photoelectron spectroscopy.

279 ing synchrotron-based ambient pressure X-ray photoelectron spectroscopy.

280 d by means of diffraction, optical and X-ray photoelectron spectroscopy.

281 have been investigated by using negative ion photoelectron spectroscopy.

282 elative to more traditional methods based on photoelectron spectroscopy.

283 haracterized by Raman spectroscopy and X-ray photoelectron spectroscopy.

284 r transform infrared spectroscopy, and X-ray photoelectron spectroscopy.

285 the tethered catalysts, determined by X-ray photoelectron spectroscopy.

286 NiO(x) membrane, which is confirmed by X-ray photoelectron spectroscopy.

287 ns, and synchrotron-based near ambient X-ray photoelectron spectroscopy.

288 l strain microscopy and sputter-etched X-ray photoelectron spectroscopy.

289 Theoretical simulations of the photoelectron spectrum discovered the coexistence of two

290 uble ionisation spectra resemble the valence photoelectron spectrum in form, and their main features

291 band for a quartet state is missing from the photoelectron spectrum indicating that the anion has a s

292 The photoelectron spectrum of the m-quinonimide anion shows

293 Modeling of the photoelectron spectrum of the ortho isomer shows that th

294 ting this radical isomerization pathway with photoelectron transfer agents allows us to override the

295 he target compounds, while commonly employed photoelectron transfer catalysts such as [Ru(bpy)3]Cl2 o

296 F + CH3OH --> HF + CH3O reaction using slow photoelectron velocity-map imaging spectroscopy of cryoc

297 ization potential of the adsorbed molecules, photoelectrons were collected that originated from both

298 (57)Fe Mossbauer, x-ray photoelectron, x-ray absorption, and electron-nuclear do

299 rization of solid-phase products using X-ray photoelectron (XPS) and absorption spectroscopies (XAS)

300 Changes in photoelectron yield as a function of bias applied to ele