ライフサイエンスコーパス: photoelectron

1 (MS), and spectroscopy (vibration and X-ray photoelectron).

2 ing depth limited by the escape depth of the photoelectrons.

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

4 eading to better harvesting of the generated photoelectrons.

5 is capable of detecting high kinetic energy photoelectrons (7 keV) at a pressure up to 110 Torr has

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

7 tudied in situ using surface sensitive X-ray photoelectron and adsorption spectroscopy techniques [X-

8 jugated with nMgO and characterized by X-ray photoelectron and Fourier transform infrared spectroscop

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

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

11 Ultraviolet photoelectron and reflectance spectroscopies, combined w

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

13 X-ray photoelectron and X-ray absorption spectroscopies establ

14 rinciple accessible from experiment, through photoelectron and X-ray spectroscopy.

15 e between liquid and solid dense phases with photoelectrons and directly probe important phenomena oc

16 icroscopy, nuclear magnetic resonance, X-ray photoelectron, and infrared spectroscopy, and time-of-fl

17 tional molecular structure information using photoelectron angular distributions (PADs) that have ave

18 This feat is accomplished by measuring photoelectron angular distributions within the frame of

19 tries (2-4%) are observed in the mass-tagged photoelectron angular distributions.

20 On the basis of the photoelectron anisotropy distribution, the electron is p

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

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

23 affords the assignment of the lowest energy photoelectron band in all investigated nucleosides and n

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

25 measure the difference in lifetimes between photoelectrons born into free electron-like states and t

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

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

28 omers may be differentiated by mass-selected photoelectron circular dichroism using an electron-ion c

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

30 scanning tunnelling microscopy, supported by photoelectron diffraction and density functional theory,

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

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

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

34 o measure differences in transport times for photoelectrons from localized core levels and delocalize

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

36 We showed that photoelectron hologram can be well described only when t

37 the nonadiabatic subcycle ionization on the photoelectron hologram.

38 results help paving the way for establishing photoelectron holography for probing spatial and dynamic

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

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

41 Herein, we report the first precise photoelectron imaging spectroscopy of europium (Eu), wit

42 Herein, by using photoelectron imaging spectroscopy, we provide original

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

44 tudy the resulting strong-field dynamics via photoelectron imaging.

45 therapy by increasing the emission of Auger-photoelectrons in the nm-mum range.

46 Ag-shell thickness, which effect the Au-core photoelectron intensity.

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

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

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

50 X-ray photoelectron microscopy was used to investigate the ban

51 The negative ion photoelectron (NIPE) spectrum of 1,2,4,5-tetraoxatetrame

52 pectra concomitant with the appearance of Br photoelectron peaks in X-ray photoelectron (XP) spectra.

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

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

55 s of BSA fragments and the enhancement of Au photoelectron signal after trypsin cleavage were corresp

56 The photoelectron spectra (PES) of palladium clusters are si

57 Peaks in the photoelectron spectra are considerably narrower than in

58 Well-resolved photoelectron spectra are obtained and interpreted with

59 The photoelectron spectra display a relatively simple spectr

60 Isomer-specific photoelectron spectra of detachment to the radical groun

61 s, and inorganic phosphate demonstrates that photoelectron spectra of nucleotides arise as a spectral

62 Photoelectron spectra of RuGen(-) clusters are measured

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

64 We report high-resolution photoelectron spectra of the simplest carbanions, CH(3)(

65 parison between tunneling and angle-resolved photoelectron spectra reveals the spatial inhomogeneity

66 The operando photoelectron spectra support assignment of these newly

67 lens in combination with ion cooling yields photoelectron spectra with <2 cm(-1) resolution.

68 X-ray photoelectron spectro-scopy measurements and density fun

69 X-ray photoelectron spectroscopic (XPS) analysis of C and N bi

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

71 X-ray photoelectron spectroscopic and pair distribution functi

72 Cyclic voltammetric data, and ultraviolet photoelectron spectroscopic studies carried out at gold

73 lms using photoluminescence, Raman and x-ray photoelectron spectroscopies.

74 Using ambient-pressure X-ray photoelectron spectroscopy (AP-XPS), we studied the adso

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

76 Ambient-pressure X-ray photoelectron spectroscopy (APXPS) and high-pressure sca

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

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

79 Angle-resolved photoelectron spectroscopy (ARPES) is used to study thes

80 Near ambient pressure X-ray photoelectron spectroscopy (NAP-XPS) is a promising meth

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

82 ctroscopy and by near-ambient pressure X-ray photoelectron spectroscopy (NAP-XPS).

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

84 Anion photoelectron spectroscopy (PES) and electron energy-los

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

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

87 o BN isosteres of indole using a combined UV-photoelectron spectroscopy (UV-PES)/computational chemis

88 method and showed good agreement with X-ray photoelectron spectroscopy (which is surface sensitive).

89 ilms before and after the treatment by X-ray photoelectron spectroscopy (XPS) also evidencing the cor

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

91 X-ray photoelectron spectroscopy (XPS) analysis results showed

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

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

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

95 isms are also investigated in terms of X-ray photoelectron spectroscopy (XPS) and electrochemical mea

96 s of CMP are proposed according to the X-ray photoelectron spectroscopy (XPS) and electrochemical mea

97 X-ray photoelectron spectroscopy (XPS) and electron microprobe

98 led plasma-mass spectrometry (ICP-MS), X-ray photoelectron spectroscopy (XPS) and Fourier-transform i

99 nd adsorption spectroscopy techniques [X-ray photoelectron spectroscopy (XPS) and near edge X-ray ads

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

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

102 iosensor surfaces were optimized using X-ray photoelectron spectroscopy (XPS) and the ultra-high freq

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

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

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

106 during the biosensor construction and X-ray photoelectron spectroscopy (XPS) experiments confirmed c

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

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

109 IPY-type fluorescence, photometry, and X-ray photoelectron spectroscopy (XPS) label allows estimation

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 orm infrared spectroscopy (FT-IR), and X-ray photoelectron spectroscopy (XPS) showed that the nanowir

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

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

115 study were to evaluate the ability of X-ray photoelectron spectroscopy (XPS) to differentiate rice m

116 troscopy, x-ray diffraction (XRD), and x-ray photoelectron spectroscopy (XPS) were employed for ligni

117 ray absorption spectroscopy (XAS), and X-ray photoelectron spectroscopy (XPS) were used to determine

118 ectron microscopy (TEM), Raman spectroscopy, photoelectron spectroscopy (XPS), and SQUID magnetometry

119 by the MIP cavities was monitored with X-ray photoelectron spectroscopy (XPS), as manifested by a neg

120 ysis, UV-vis, energy-dispersive X-ray, X-ray photoelectron spectroscopy (XPS), attenuated total refle

121 new nanoparticle was characterized by X-ray photoelectron spectroscopy (XPS), dynamic light scatteri

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

123 ombination of X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS), in-field Mossbauer spe

124 d triclosan in batch experiments using X-ray photoelectron spectroscopy (XPS), Raman spectroscopy, an

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

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

127 irrors and AgNPs was confirmed through X-ray photoelectron spectroscopy (XPS), transmission electron

128 riate MOFs (MTV-MOFs) were examined by X-ray photoelectron spectroscopy (XPS), ultraviolet-visible di

129 ransmission electron microscopy (TEM), X-ray photoelectron spectroscopy (XPS), UV-vis diffuse reflect

130 the sensor surface was monitored using X-ray photoelectron spectroscopy (XPS), while the binding of c

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

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

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

134 aracterized by electrochemistry and by X-ray photoelectron spectroscopy (XPS).

135 -ray absorption spectroscopy (XAS) and X-ray photoelectron spectroscopy (XPS).

136 neling microscopy and spectroscopy and X-ray photoelectron spectroscopy (XPS).

137 flection X-ray fluorescence (TXRF) and X-ray photoelectron spectroscopy (XPS).

138 ction (GA-ATR) FT-IR spectroscopy, and X-ray photoelectron spectroscopy (XPS).

139 in the presence of liquids by means of X-ray photoelectron spectroscopy (XPS).

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

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

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

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

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

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

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

147 X-ray photoelectron spectroscopy analysis of ABP and ACP confi

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

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

150 Here, using time-resolved photoelectron spectroscopy and ab initio calculations, w

151 ike structures of CoB16(-), characterized by photoelectron spectroscopy and ab initio calculations.

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

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

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

155 urier transform infrared spectroscopy, X-ray photoelectron spectroscopy and atomic force microscopy.

156 is hydrophobic ligand was confirmed by X-ray photoelectron spectroscopy and contact angle goniometry

157 X-ray photoelectron spectroscopy and electrochemistry confirm

158 fides has been evaluated by conducting X-ray photoelectron spectroscopy and electron microscopy studi

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

160 itial CO loss as determined by in situ X-ray photoelectron spectroscopy and mass spectrometry.

161 The CoB18 (-) cluster was characterized by photoelectron spectroscopy and quantum chemistry calcula

162 Here, we use photoelectron spectroscopy and quantum chemistry calcula

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

164 ased on a combination of detailed core-level photoelectron spectroscopy and quantum-chemical calculat

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

166 X-ray photoelectron spectroscopy and scanning electron microsc

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

168 tal dichalcogenides by using microbeam X-ray photoelectron spectroscopy and scanning tunnelling micro

169 ulating films of WO3 Here, we use hard X-ray photoelectron spectroscopy and spectroscopic ellipsometr

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

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

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

173 orption mechanisms were assessed using X-ray photoelectron spectroscopy and X-ray absorption spectros

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

175 Liquid-jet photoelectron spectroscopy can be used to directly study

176 Photoelectron spectroscopy confirms that Ag acts as a p-

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

178 X-ray diffraction and X-ray photoelectron spectroscopy experiments were used to exam

179 Negative-ion photoelectron spectroscopy has shown the adiabatic detac

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

181 X-ray photoelectron spectroscopy indicated that the predominan

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

183 X-ray photoelectron spectroscopy invariably detected elemental

184 Recent angle-resolved photoelectron spectroscopy investigations provided insig

185 Time-resolved photoelectron spectroscopy is performed on thymine and t

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

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

188 X-ray photoelectron spectroscopy of C 1s and Br 3d core levels

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

190 X-ray photoelectron spectroscopy of these electrochemically tr

191 ared spectroscopy, and high resolution X-ray photoelectron spectroscopy of TPI-carbons to elucidate t

192 In situ, depth-resolved X-ray photoelectron spectroscopy of various graphene-coated tr

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

194 ro charge by means of ambient pressure X-ray photoelectron spectroscopy performed under polarization

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

196 X-ray photoelectron spectroscopy results show ferrate resultan

197 Moreover, the X-ray photoelectron spectroscopy results show that the valence

198 X-ray photoelectron spectroscopy revealed significant core-lev

199 X-ray photoelectron spectroscopy revealed that an effective mo

200 X-ray photoelectron spectroscopy revealed that the hydroxyl gr

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

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

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

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

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

206 razing incidence x-ray diffraction and x-ray photoelectron spectroscopy studies indicating that the f

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

208 hy, X-ray absorption spectroscopy, and X-ray photoelectron spectroscopy suggest that reduction of 1 a

209 and surface oxygen concentrations from X-ray photoelectron spectroscopy suggests that surface sites g

210 trochemical impedance spectroscopy and X-ray photoelectron spectroscopy techniques.

211 nization aerosol mass spectrometry and X-ray photoelectron spectroscopy to confirm these predictions.

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

213 8H8I2) produces m-C8H8 in gas phase; we used photoelectron spectroscopy to probe the first two electr

214 onal spectroscopy and ambient pressure X-ray photoelectron spectroscopy under catalytically relevant

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

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

217 X-ray photoelectron spectroscopy was utilized to determine the

218 nfrared spectroscopy, ellipsometry and X-ray photoelectron spectroscopy were used to follow the stepw

219 ere investigated by mass spectrometry, anion photoelectron spectroscopy, and computations.

220 rature scanning tunnelling microscopy, X-ray photoelectron spectroscopy, and density functional theor

221 IR reflection absorption spectroscopy, X-ray photoelectron spectroscopy, and electrochemical impedanc

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

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

224 on, by IR and Raman spectroscopy, XRD, X-ray photoelectron spectroscopy, and Mossbauer spectroscopy c

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

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

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

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

229 ransform infrared (FTIR) spectroscopy, X-ray photoelectron spectroscopy, and time-of-flight secondary

230 uded size, surface charge, morphology, X-ray photoelectron spectroscopy, and transmission Fourier tra

231 nance spectroscopy, mass spectrometry, X-ray photoelectron spectroscopy, and X-ray absorption spectro

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

233 icrographs, x-ray diffraction spectra, x-ray photoelectron spectroscopy, as well as TFT output and tr

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

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

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

237 mbining inelastic tunneling spectroscopy, UV photoelectron spectroscopy, electronic structure calcula

238 X-ray photoelectron spectroscopy, EPR, and magnetometry suppor

239 m interface, performed using liquid microjet photoelectron spectroscopy, has been interpreted to sugg

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

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

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

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

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

245 X-ray photoelectron spectroscopy, Raman microscopy and spectro

246 X-ray photoelectron spectroscopy, Raman spectroscopy, together

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

248 samples on SiC(000) combining angle-resolved photoelectron spectroscopy, scanning tunneling microscop

249 utherford backscattering spectrometry, X-ray photoelectron spectroscopy, spectroscopic ellipsometry,

250 mined using a novel approach combining X-ray photoelectron spectroscopy, surface tension measurements

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

252 trospray ionization mass spectrometry, X-ray photoelectron spectroscopy, thermogravimetric analysis a

253 e scanning tunneling microscopy (STM), X-ray photoelectron spectroscopy, transmission infrared spectr

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

255 circular dichroism, combined with hard X-ray photoelectron spectroscopy, we derived a complete pictur

256 Using femtosecond time-resolved two-photon photoelectron spectroscopy, we determine (i) the vertica

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

258 using ambient-pressure X-ray absorption and photoelectron spectroscopy, we proved that the dominant

259 nsient absorption spectroscopy and gas-phase photoelectron spectroscopy, we show that hexane, a commo

260 Applying angle-resolved photoelectron spectroscopy, we show that the silicon sur

261 layer on the surface, as determined by X-ray photoelectron spectroscopy, which likely prevented furth

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

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

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

265 confirmed using elemental analysis and X-ray photoelectron spectroscopy.

266 potential of -0.75 V, as observed from X-ray photoelectron spectroscopy.

267 ements, optical/solvent exposures, and X-ray photoelectron spectroscopy.

268 n between Au and ZnO was manifested by X-ray photoelectron spectroscopy.

269 namely X-ray magnetic circular dichroism and photoelectron spectroscopy.

270 lk water, using either optical absorption or photoelectron spectroscopy.

271 determined using X-ray diffraction and X-ray photoelectron spectroscopy.

272 ized by contact angle measurements and X-ray photoelectron spectroscopy.

273 temperature-programmed desorption, and X-ray photoelectron spectroscopy.

274 red by quite different methods such as X-ray photoelectron spectroscopy.

275 ce, which was probed by angle-resolved X-ray photoelectron spectroscopy.

276 OCCO) was observed and investigated by anion photoelectron spectroscopy.

277 y transmission electron microscopy and X-ray photoelectron spectroscopy.

278 s-pyridinyltetrazine, as determined by X-ray photoelectron spectroscopy.

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

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

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

282 have been investigated by using negative ion photoelectron spectroscopy.

283 elative to more traditional methods based on photoelectron spectroscopy.

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

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

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

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

288 computational and experimental study of the photoelectron spectrum of a simple aqueous solution of N

289 The photoelectron spectrum of the m-quinonimide anion shows

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

291 acterization includes its electron affinity, photoelectron spectrum, and the previously reported stru

292 Monte Carlo simulations of X-ray photoelectron trajectories suggest the formation of subs

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

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

295 approximately 3-4 nm) of the XPS and NEXAFS photoelectrons used for analysis at 413 K.

296 ponding cryogenically cooled anions via slow photoelectron velocity-map imaging (cryo-SEVI).

297 Slow photoelectron velocity-map imaging (SEVI) spectroscopy h

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

299 ppearance of Br photoelectron peaks in X-ray photoelectron (XP) spectra.

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