ライフサイエンスコーパス: photoemission

1 tates in (Pb,Sn)Te, (Pb,Sn)Se and SnTe using photoemission.

2 )Sr(2)CaCu(2)O(8+delta) using angle-resolved photoemission.

3 istortions and the absence of edge states in photoemission.

4 genides ReS(2) and ReSe(2) by angle resolved photoemission.

5 version, hot-carrier extraction and electron photoemission.

6 om measured data using angular resolution in photoemission.

7 l characterization, angle-resolved and X-ray photoemission analysis, and temperature-dependent four-p

8 Using near-ambient pressure X-ray photoemission and a curved Pt(111) crystal we probe the

9 Angle-resolved photoemission and bulk transport measurements reveal tha

10 Using high-resolution angle-resolved photoemission and core-level spectroscopy, it is shown c

11 High-resolution photoemission and density functional calculations on rea

12 Using angle-resolved photoemission and density-functional theory, we show how

13 The valence photoemission and DFT results point to a new type of "st

14 ample, 2H-NbSe2, by spin- and angle-resolved photoemission and first-principles theory.

15 uent dynamics using time- and angle-resolved photoemission and infrared reflectivity probes.

16 The combination of photoemission and photoelectron diffraction techniques b

17 ions of free-electron generation by particle photoemission and photoionization of the surrounding wat

18 in crystalline hexacene using time-resolved photoemission and transient absorption spectroscopies.

19 se effects by studying exciton satellites in photoemission and tunneling spectroscopy, which present

20 These surface states can be probed by photoemission and tunnelling experiments.

21 tes have been comprehensively imaged by both photoemission and tunnelling spectroscopies.

22 e was studied in situ using ambient-pressure photoemission and X-ray absorption spectroscopy techniqu

23 or conversion, sunlight harvesting, electron photoemission, and advanced imaging and sensing.

24 canning tunneling microscopy, angle-resolved photoemission, and density functional theory study of Mn

25 Morphological, photoemission, and modelling studies show that boundarie

26 Electrical measurements, photoemission, and Raman spectroscopy are used to study

27 oscopy, synchrotron X-ray and angle-resolved photoemission, and X-ray absorption, direct spectroscopi

28 gas phase using a unique infrared desorption/photoemission anion source.

29 This effect, revealed by resonant X-ray photoemission, arises from interfacial hybridization bet

30 Here, we report angle-resolved photoemission (ARPES) evidence of FS reconstruction in o

31 We report on an angle resolved photoemission (ARPES) study of bulk electron-doped perov

32 Using angle-resolved photoemission (ARPES), we show here that doping electron

33 thereby rotating the tip-aligned directional photoemission as observed with angle-resolved 2D velocit

34 initiation process, photoelectron ejection (photoemission), as a facile way of initiating photochemi

35 ed wavelength regime provides quasi-singular photoemission at the (8,7) SWNTs.

36 DW from diffraction, scanning tunnelling and photoemission based probes suggests an unconventional an

37 The proposed photoemission-based devices benefit from the advantages

38 These states have been imaged by photoemission, but little information on their transport

39 mation and fully relativistic one-step-model photoemission calculations including matrix-element effe

40 Here we demonstrate that angle-resolved photoemission can directly image the quasiparticle dynam

41 as analyzed using parallel X-ray and optical photoemission channels to collect X-ray absorption near-

42 Here, we report angle-resolved photoemission characterization revealing a monotonic inc

43 The lack of angle-resolved photoemission data for every cuprate family precludes an

44 LaAlO3/SrTiO3 interface, our angle-resolved photoemission data show replica bands separated by 100 m

45 ..H-O hydrogen bonds, by combining our X-ray photoemission data with the local density-of-state image

46 imately 3 h thanks to a new multidimensional photoemission data-recording technique (combining full-f

47 nt in sensitivity, compared with traditional photoemission decay experiments and the ability to measu

48 er light absorbance and a factor of 2 larger photoemission during spin pumping.

49 to simple Neel wall structures, imaged using photoemission electron and Lorentz transmission electron

50 Photoemission electron microscopy (PEEM) and imaging X-r

51 Until recently, use of photoemission electron microscopy (PEEM) for such purpos

52 Ultrafast photoemission electron microscopy (PEEM) has demonstrate

53 X-ray photoemission electron microscopy (XPEEM), with its exce

54 ay transmission microscopy and time-resolved photoemission electron microscopy after applying nanosec

55 ll-shaped Permalloy nanowires obtained using photoemission electron microscopy combined with x-ray ma

56 sing X-ray magnetic circular dichroism-based photoemission electron microscopy coupled with macroscop

57 ng electron microscopy, as well as the first photoemission electron microscopy experiments, both acce

58 Here we use photoemission electron microscopy to image the trap dist

59 Using X-ray photoemission electron microscopy we show that the colle

60 When coupled with imaging methods like photoemission electron microscopy, it enables chemical i

61 Using photoemission electron microscopy, we image the nanoscal

62 ond pump-probe techniques with spectroscopic photoemission electron microscopy, we imaged the motion

63 Using X-ray photoemission electron microscopy, we show that the ferr

64 a novel method using low-energy electron and photoemission electron microscopy.

65 eling microscopy and spectroscopy (STM/STS), photoemission electron microscopy/spectroscopy (PEEM) an

66 Here we provide-using angle-resolved photoemission electron spectroscopy-the band structure o

67 l catalysts have been examined using valence photoemission experiments and density functional theory

68 results and the analysis of angular-resolved photoemission experiments on a cuprate superconductor.

69 e of Alq3 on Co and, by combining two-photon photoemission experiments with electronic structure theo

70 By combining time-resolved two-photon photoemission experiments with state-of-the-art numerica

71 ications of broken time-reversal symmetry in photoemission experiments, recent polarized neutron diff

72 rt materials simulation techniques and X-ray photoemission experiments, that a type-II, staggered, ba

73 mimetals, and recently confirmed to be so by photoemission experiments.

74 sport experiments agrees with angle-resolved photoemission experiments.

75 ensional hot electron gas through two-photon photoemission from a copper surface in vacuum.

76 experimental momentum maps of angle-resolved photoemission from molecular orbitals can be transformed

77 mentum-space characterization of multiphoton photoemission from plasmonic gold nanostars and demonstr

78 nic bands in a metal by exciting four-photon photoemission from the Cu(111) surface involving a three

79 Using hard X-ray angle-resolved photoemission (HARPES) at 3.2 keV, we investigate the bu

80 mojunction interfacial workfunction internal photoemission (HIWIP)-detector-LED up-converter and sili

81 Through such photoemission images we probe a characteristic elastic s

82 cathode luminescence imaging and two-photon photoemission imaging have subwavelength resolution, the

83 ide one of the first observations of delayed photoemission in a small cold molecular radical anion, a

84 Photoemission in materials research is commonly acknowle

85 s based on modulation of the carbon nanotube photoemission in the near-infrared, as we show by tracki

86 urface including electrons at the antinodes, photoemission indicates a solely nodal density-of-states

87 We examine the quantum confinement in the photoemission ionization energy in air and optical band

88 Internal photoemission (IPE), a process involving optical excitat

89 Our results indicate that photoemission is an effective way of initiating grafting

90 grafting because the irreversible nature of photoemission leaves the sample with a net excess of hol

91 Our angle-resolved photoemission measurements of the band structure as a fu

92 With further input from UV photoemission measurements on Au-protein systems, these

93 gated device architecture for angle-resolved photoemission measurements with a nano-focused light spo

94 Our transport data, corroborated by photoemission measurements, first-principles calculation

95 Our detailed angle-resolved photoemission measurements, first-principles simulations

96 ing tunnelling microscopy and angle resolved photoemission measurements.

97 ice motion at a single phonon frequency, and photoemission monitors the subsequent coherent changes i

98 aviolet source a powerful tool for ultrafast photoemission, nanoscale imaging and other applications.

99 takes place, and to compare with UV-mediated photoemission on Si(111)-H, a series of electron accepto

100 n state, which we observed by angle-resolved photoemission, paves the way for studying a range of top

101 The photoemission results indicate that at 150 K O(2) adsorb

102 high-symmetry (111) direction and carry out photoemission scans on top.

103 Finally, by generating time-resolved photoemission sequences of the photo-excited carrier tra

104 Angle-resolved photoemission spectra and DFT calculations show that a d

105 aN(0001) surface by recording the core-level photoemission spectra and obtained the electronic and ch

106 In particular, satellites in photoemission spectra are pure many-body effects, and th

107 ystals can be determined from angle-resolved photoemission spectra of a trilayer structure with one a

108 sition of alkali-metal atoms, angle-resolved photoemission spectra of Sr2IrO4 display disconnected se

109 The electron photoemission spectra of the films of synthesized materi

110 cted surprising linear magnetic dichroism in photoemission spectra of the split-off band.

111 tio many-body calculations of angle-resolved photoemission spectra of titanium dioxide, we show that

112 Core-level photoemission spectra show that the gating reversibly mo

113 Circular dichroism photoemission spectra suggest that these in-gap states p

114 ltrahigh vacuum catalytic experiments, X-ray photoemission spectra, and accurate density functional t

115 rough X-ray absorption fine structure, X-ray photoemission spectra, transport measurement and theoret

116 Using a combination of vibrational and photoemission spectroscopies, bonding of the two peptide

117 Here, using high-resolution angle-resolved photoemission spectroscopy (ARPES) along with first-prin

118 magnetic BaCr2As2 by means of angle-resolved photoemission spectroscopy (ARPES) and first-principles

119 ed (Bi, Sb)2Te3 thin films by angle-resolved photoemission spectroscopy (ARPES) and show unambiguousl

120 a systematic high-resolution angle-resolved photoemission spectroscopy (ARPES) and spin-resolved ARP

121 ere, we present evidence from angle-resolved photoemission spectroscopy (ARPES) for negative electron

122 FeSe on SrTiO3 (STO)(001) by angle-resolved photoemission spectroscopy (ARPES) has led to the conjec

123 omentum-space discrimination, angle-resolved photoemission spectroscopy (ARPES) is ideally suited for

124 tional ultraviolet/soft X-ray angle-resolved photoemission spectroscopy (ARPES) may in some cases be

125 nducting gaps observed in the angle-resolved photoemission spectroscopy (ARPES) measurement.

126 Detailed comparison between angle-resolved photoemission spectroscopy (ARPES) measurements and dens

127 Angle-resolved photoemission spectroscopy (ARPES) measurements combined

128 Here, by performing angle-resolved photoemission spectroscopy (ARPES) on NbP and TaP, we di

129 Here, we report angle-resolved photoemission spectroscopy (ARPES) results from Rb dosed

130 his dichotomy of the observed angle-resolved photoemission spectroscopy (ARPES) spectra is similarly

131 A series of angle-resolved photoemission spectroscopy (ARPES) studies were performe

132 Here we present an angle-resolved photoemission spectroscopy (ARPES) study of the Kondo la

133 Here we present an angle-resolved photoemission spectroscopy (ARPES) study of the trilayer

134 In this work, we use angle-resolved photoemission spectroscopy (ARPES) to investigate the in

135 pulses can be used to perform angle-resolved photoemission spectroscopy (ARPES) to map the electronic

136 l has been investigated using angle-resolved photoemission spectroscopy (ARPES) to reveal a single Di

137 Here we use angle-resolved photoemission spectroscopy (ARPES) to study FeSb(2), a c

138 0.60) have been determined by angle-resolved photoemission spectroscopy (ARPES) using synchrotron rad

139 mapping near the X-point via angle resolved photoemission spectroscopy (ARPES) with a Dirac nodal li

140 oy optical spectroscopy (OS), angle-resolved photoemission spectroscopy (ARPES), ab initio band-struc

141 Using angle-resolved photoemission spectroscopy (ARPES), we observe a quantum

142 Using angle-resolved photoemission spectroscopy (ARPES), we show that lithium

143 tropic Eliashberg theory, and angle-resolved photoemission spectroscopy (ARPES), we show that surface

144 Using angle-resolved photoemission spectroscopy (ARPES), we unravel the uniqu

145 gy and polarization dependent angle-resolved photoemission spectroscopy (ARPES).

146 ormula: see text] measured by angle-resolved photoemission spectroscopy (ARPES).

147 inaccessible to conventional angle-resolved photoemission spectroscopy (ARPES).

148 ction (LEED), high resolution angle-resolved photoemission spectroscopy (HR-ARPES), and scanning tunn

149 We use pump-probe angle-resolved photoemission spectroscopy (pump-probe ARPES) to directl

150 By using synchrotron radiation photoemission spectroscopy (SRPES), extended X-ray absor

151 time domain, using time- and angle-resolved photoemission spectroscopy (TR-ARPES).

152 rt herein a time-resolved and angle-resolved photoemission spectroscopy (TRARPES) study of WSe2, a la

153 of the photoelectrons emitted in ultraviolet photoemission spectroscopy (UPS) to determine the electr

154 By using ultraviolet photoemission spectroscopy (UPS), we show here that expo

155 on near-edge structure (XANES), valence-band photoemission spectroscopy (VB-PES), X-ray emission spec

156 d reaction (TPR) mass spectrometry and X-ray photoemission spectroscopy (XPS) following exposure to O

157 By carrying out angle-resolved photoemission spectroscopy and ab initio calculations on

158 ated kagome metal CoSn, using angle-resolved photoemission spectroscopy and band structure calculatio

159 In this work, by using angle-resolved photoemission spectroscopy and conductivity measurement,

160 Ultraviolet photoemission spectroscopy and contact potential differe

161 Here we utilized angle-resolved photoemission spectroscopy and density functional theory

162 combination of studies involving ultraviolet photoemission spectroscopy and density functional theory

163 ture of Bi(2)Se(3) employing high resolution photoemission spectroscopy and discover the dependence o

164 tries, using a combination of angle-resolved photoemission spectroscopy and first-principles calculat

165 Using in situ photoemission spectroscopy and online product analysis,

166 f a DSM that can be tested by angle-resolved photoemission spectroscopy and quantum oscillation exper

167 i/2) of the Brillouin zone by angle-resolved photoemission spectroscopy and quantum oscillation measu

168 In this study, we use photoemission spectroscopy and quantum transport to eluc

169 isted graphene confirmed by angular resolved photoemission spectroscopy and Raman analysis.

170 Using angle-resolved photoemission spectroscopy and scanning tunneling micros

171 In this work, through angle-resolved photoemission spectroscopy and scanning tunneling micros

172 ted LaNiO3 (LNO) films, using angle-resolved photoemission spectroscopy and the dynamical mean-field

173 Our angle-resolved photoemission spectroscopy and theoretical results show

174 We performed angle-resolved photoemission spectroscopy and tight binding calculation

175 Moreover, angle-resolved photoemission spectroscopy and tight-binding calculation

176 Through X-ray photoemission spectroscopy and X-ray absorption measurem

177 (3-alpha)Fgamma films, as confirmed by X-ray photoemission spectroscopy and X-ray absorption spectros

178 By photoemission spectroscopy below the Curie temperature,

179 Pump-probe photoemission spectroscopy can track these states by mea

180 measured in UV photoelectron and two-photon photoemission spectroscopy experiments can be assigned t

181 However, theoretical investigations and photoemission spectroscopy experiments indicate that in

182 g tunnelling spectroscopy and angle-resolved photoemission spectroscopy experiments that the recently

183 Here, femtosecond time-resolved two-photon photoemission spectroscopy has been used to probe the el

184 1) heterointerface using soft and hard x-ray photoemission spectroscopy in conjunction with detailed

185 on spectroscopy, analogous to angle-resolved photoemission spectroscopy in the solid state.

186 Standing-wave ambient-pressure photoemission spectroscopy is thus a very promising tech

187 Femtosecond two-photon photoemission spectroscopy is used to inject an electron

188 Our angle-resolved photoemission spectroscopy measurements and first-princi

189 In ZrSiS, angle-resolved photoemission spectroscopy measurements have shown an un

190 X-ray photoemission spectroscopy measurements indicate a shift

191 Using angle resolved photoemission spectroscopy measurements of Bi(2)Sr(2)CaC

192 Subsequent angle-resolved photoemission spectroscopy measurements of the FeSe/STO

193 Angle-resolved photoemission spectroscopy measurements on cleaved Bi(2)

194 Our angle-resolved photoemission spectroscopy measurements performed on the

195 Angle-resolved photoemission spectroscopy measurements reveal a small a

196 Subsequent angle-resolved photoemission spectroscopy measurements reveal an unusua

197 In situ transport and angle-resolved photoemission spectroscopy measurements reveal the metal

198 theoretical calculations and angle-resolved photoemission spectroscopy measurements.

199 iques of carrier kinetics and densities, air photoemission spectroscopy of material energetics, Kelvi

200 Here we report angle- and spin-resolved photoemission spectroscopy of WTe2 single crystals, thro

201 Here, using angle-resolved photoemission spectroscopy on detwinned underdoped Ba(1-

202 in monolayer samples by using angle-resolved photoemission spectroscopy on high-quality thin films of

203 re, we report high-resolution angle-resolved photoemission spectroscopy on MoSe2 single crystals and

204 We use nanoscale angle-resolved photoemission spectroscopy on single nanowires (nano-ARP

205 photoelectron spectroscopy and standing-wave photoemission spectroscopy provides the spatial arrangem

206 ere we report high-resolution angle-resolved photoemission spectroscopy results that reveal an unexpe

207 Photoemission spectroscopy revealed that ZnTPP-P-Ipa par

208 Angle-resolved photoemission spectroscopy shows the characteristic Dira

209 We present angle-resolved photoemission spectroscopy studies of Bi[Formula: see te

210 e we report a high-resolution angle-resolved photoemission spectroscopy study on LiFe(1-x)CoxAs.

211 an and sp(3) bonding characteristic in X-ray photoemission spectroscopy suggests the existence of int

212 de molecular-beam epitaxy and angle-resolved photoemission spectroscopy system to synthesize and inve

213 Here we show by angle-resolved photoemission spectroscopy that paramagnetic EuRh(2)Si(2

214 Here we show using angle resolved photoemission spectroscopy that twin-grain boundaries in

215 We used angle-resolved photoemission spectroscopy to experimentally observe a p

216 Here we use photoemission spectroscopy to image the formation of pro

217 Here, we use angle-resolved photoemission spectroscopy to measure three representati

218 We use angle-resolved photoemission spectroscopy to show that the two-gap beha

219 e core-hole clock implementation of resonant photoemission spectroscopy to study the femtosecond char

220 Here, we use time- and angle-resolved photoemission spectroscopy to study the initial rise of

221 Here we apply time-resolved photoemission spectroscopy to the tetracene/C(60) interf

222 Here we perform angle-resolved photoemission spectroscopy to try to find an electron do

223 Here, we use angle-resolved photoemission spectroscopy to uncover an abrupt destruct

224 Applying in situ photoemission spectroscopy under oxygen ambient, ionic a

225 ular beam epitaxy and in situ angle-resolved photoemission spectroscopy we show that valence fluctuat

226 tron microscopy, x-ray diffraction and x-ray photoemission spectroscopy were utilised to perform a st

227 Here, combining angle-resolved photoemission spectroscopy with density functional theor

228 ere, we employed state-of-the-art hard x-ray photoemission spectroscopy with judiciously chosen exper

229 Here, by using spin-resolved photoemission spectroscopy with p-polarized light in top

230 In this work, using angle-resolved photoemission spectroscopy with sub-micrometer spatial r

231 e show that micrometre-scale, angle-resolved photoemission spectroscopy(1-3) (microARPES) applied to

232 graphitic carbon support (accessed via C 1s photoemission spectroscopy).

233 e is essentially based on the angle resolved photoemission spectroscopy, a highly surface sensitive t

234 he gas are performed using momentum-resolved photoemission spectroscopy, analogous to angle-resolved

235 e[Formula: see text] band offset using X-ray photoemission spectroscopy, and chart the elemental comp

236 oss analysis using optical characterization, photoemission spectroscopy, and device modeling, directi

237 Spin- and angle-resolved photoemission spectroscopy, complemented by theoretical

238 Using angle-resolved photoemission spectroscopy, crossing points formed by th

239 By combining x-ray photoemission spectroscopy, density functional theory, a

240 absorption spectroscopy combined with X-ray photoemission spectroscopy, electrical transport and the

241 f indium selenide by means of angle-resolved photoemission spectroscopy, electron energy loss spectro

242 ing tunnelling microscopy and angle-resolved photoemission spectroscopy, in combination with first-pr

243 Here, using high-resolution angle-resolved photoemission spectroscopy, magnetotransport, and parall

244 Using angle-resolved photoemission spectroscopy, modelling, density functiona

245 g three different techniques (angle-resolved photoemission spectroscopy, polar Kerr effect, and time-

246 We characterize Sn-BSTS via angle-resolved photoemission spectroscopy, scanning tunnelling microsco

247 bdenum trioxide (MoO3), is studied combining photoemission spectroscopy, sheet resistance measurement

248 combination of magnetometry, spin-polarized photoemission spectroscopy, symmetry arguments and first

249 ity functional theory calculations and X-ray photoemission spectroscopy, the surface-assisted reactio

250 , using femtosecond time- and angle-resolved photoemission spectroscopy, we demonstrate a tendency to

251 Using spin- and angle-resolved photoemission spectroscopy, we demonstrate that such a s

252 ronic structure of Na3Bi with angle-resolved photoemission spectroscopy, we detected 3D Dirac fermion

253 Here, by performing angle-resolved photoemission spectroscopy, we directly observe a pair o

254 Using photoemission spectroscopy, we directly observe Fermi ar

255 With angle-resolved photoemission spectroscopy, we directly observed almost

256 By using time- and angle-resolved photoemission spectroscopy, we investigate the ultrafast

257 simultaneous spin, time, and angle-resolved photoemission spectroscopy, we map the spin-polarized un

258 Here, using high-resolution angle-resolved photoemission spectroscopy, we performed systematic elec

259 Here, by using spin- and angle-resolved photoemission spectroscopy, we report the observation of

260 oxide-semiconductor interface via hard x-ray photoemission spectroscopy, we show how to systematicall

261 Using time- and angle-resolved photoemission spectroscopy, we show that an intense ultr

262 si-freestanding graphene with angle-resolved photoemission spectroscopy, we showed that at finite dop

263 In this work, using angle-resolved photoemission spectroscopy, we visualized the electronic

264 ulk ReSe2 by direct nanoscale angle-resolved photoemission spectroscopy.

265 evealed by spatially resolved angle-resolved photoemission spectroscopy.

266 can be tested via laser-based angle-resolved photoemission spectroscopy.

267 s of Sr0.06Bi2Se3 (Tc ~ 2.5 K) by performing photoemission spectroscopy.

268 utional diffusion and in-situ angle-resolved photoemission spectroscopy.

269 icroscopy in conjunction with angle-resolved photoemission spectroscopy.

270 nd reduction were studied with high pressure photoemission spectroscopy.

271 mal state, investigated using angle-resolved photoemission spectroscopy.

272 ir spectral function using momentum-resolved photoemission spectroscopy.

273 hene by using high-resolution angle-resolved photoemission spectroscopy.

274 " We studied this state using angle-resolved photoemission spectroscopy.

275 y synchrotron and laser-based angle-resolved photoemission spectroscopy.

276 challenge is overcome by using time-resolved photoemission spectroscopy.

277 be the overall lineshape of the experimental photoemission spectrum.

278 we report on low-temperature angle-resolved photoemission studies of the valence band in this model

279 Detailed electrical and photoemission studies were carried out to probe the chem

280 l transport, X-ray magnetic diffraction, and photoemission studies with band structure calculations t

281 ty for the time-, spin- and momentum-resolve photoemission technique.

282 t laser and synchrotron-based angle-resolved photoemission techniques.

283 probe experiments, or in reciprocal space by photoemission, the phase information of the orbital is l

284 onic field simulations combined with quantum photoemission theory elucidate the role of surface-media

285 el calculations and to more precise one-step photoemission theory including matrix element effects.

286 ing, film thickness variations and a coupled photoemission-thermodynamic analysis of space-charge eff

287 Here we use time- and angle-resolved photoemission to directly measure the ultrafast response

288 two mechanisms of photoactivation (internal photoemission versus interband photoexcitation followed

289 a low-power infrared laser can cause enough photoemission via electron tunnelling to implement feasi

290 y extracting the time delays associated with photoemission we show that the lifetime of photoelectron

291 Using angle-resolved photoemission, we directly observe two pairs of Weyl poi

292 tions together with spin- and angle-resolved photoemission, we find that these generically host a co-

293 e explanation for this phenomenon is inverse photoemission, where the injection of highly energetic h

294 e, the photocurrent is dominated by internal photoemission, which exhibits energy thresholds correspo

295 ergy and momentum space using angle-resolved photoemission with a spatial resolution on the order of

296 Here we investigate, using photoemission, X-ray scattering and scanning tunnelling

297 mple electric self-detection of the integral photoemission yield and Fourier data analysis permit ext

298 X-ray induced photoemission yield contains structural information comp

299 we show that the integral hard-X-ray-induced photoemission yield is modulated by the Fresnel reflecti

300 Temperature-dependent photoemission-yield measurements from GaN show strong ev