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 ectronic band structure using angle-resolved photoemission.

5 ence band edge as observed by angle-resolved photoemission.

6 irs xi(0) closely tracks the gap measured by photoemission.

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

8 Angle-resolved photoemission and bulk transport measurements reveal tha

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

10 High-resolution photoemission and density functional calculations on rea

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

12 Synchrotron-based high-resolution photoemission and first-principles density-functional (D

13 Synchrotron-based high-resolution photoemission and first-principles density-functional sl

14 Photoemission and first-principles DF calculations were

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

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

17 The combination of photoemission and photoelectron diffraction techniques b

18 Using angle-resolved photoemission and scanning tunneling microscopy, we dete

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

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

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

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

23 These techniques, such as photoemission and tunnelling, yield measurements of the

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

25 Here, scanning tunneling microscopy, photoemission, and density-functional calculations are u

26 e unoccupied states that are inaccessible to photoemission, and find strong similarities to the struc

27 ay absorption fine structure (NEXAFS/EXAFS), photoemission, and first-principles density-functional (

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

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

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

31 ly rich data obtained both by angle-resolved photoemission (ARPES) and high-resolution, large-area sc

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

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

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

35 e Fermi level was measured by spin-polarized photoemission at room temperature for a thin film on Au(

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

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

38 The proposed photoemission-based devices benefit from the advantages

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

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

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

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

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

44 ation states and multivalence--such as X-ray photoemission core-level shifts, ionic radii and variati

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

46 We report angle-resolved photoemission data on the band dispersion for an alkali-

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

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

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

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

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

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

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

54 using piezo force microscopy, whereas X-ray photoemission electron microscopy as well as its tempera

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

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

60 Using photoemission electron microscopy, we image the nanoscal

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

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

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

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

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

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

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

68 urements on YBCO and of circularly polarized photoemission experiments on Bi(2)Sr(2)CaCu(2)O(8+delta)

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

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

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

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

73 sport experiments agrees with angle-resolved photoemission experiments.

74 agnitude smaller than the effect observed in photoemission experiments.

75 rmi-surface and energy gap in agreement with photoemission experiments.

76 le remains surprisingly well screened in the photoemission final state.

77 We found monochromatic electron photoemission from large-area self-assembled monolayers

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

79 There is generally good agreement between photoemission from vapor-deposited thin films of the C24

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

81 Ultrafast two-photon photoemission has been used to study electron solvation

82 Through such photoemission images we probe a characteristic elastic s

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

84 es to demonstrate controlled quenching of QD photoemission in a multiplexed format.

85 Photoemission in materials research is commonly acknowle

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

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

88 urface as measured by the Au(3+)/Au(0) X-ray photoemission intensities.

89 The photoemission intensity in the mesoporous intermetallic

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

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

92 emphasized in the tunneling measurements and photoemission is most sensitive to excitations near the

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

94 Angle-resolved photoemission measurements in the superconducting state

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

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

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

98 with the adsorption of OH comes from ex-situ photoemission measurements, which indicate that the Sn a

99 ing tunnelling microscopy and angle resolved photoemission measurements.

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

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

102 pulate the direction and polarization of the photoemission of CdSe nanoparticles via assembly into 2D

103 nts show that the grafting reaction involves photoemission of electrons into the liquid.

104 face process since there is no evidence from photoemission of sulfate adsorption, and the same surfac

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

106 ion with charged quasi-particles observed by photoemission, optical conductivity, and tunnelling sugg

107 cy can be controlled either by tuning the QD photoemission or by adjusting the number of dye-labeled

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

109 excitonic behavior upon photoexcitation and photoemission processes.

110 The photoemission results and comparison with the correspond

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

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

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

114 s and the electron-phonon interaction in the photoemission spectra of La(2 - x)Sr(x)CuO4.

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

116 The electron photoemission spectra of the films of synthesized materi

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

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

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

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

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

122 Using a photoemission spectroscometer that operates close to amb

123 lysis in combination with infrared and X-ray photoemission spectroscopies has shown the anatase nanoc

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

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

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

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

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

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

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

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

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

133 Angle-resolved photoemission spectroscopy (ARPES) measurements combined

134 Here we report angle-resolved photoemission spectroscopy (ARPES) of LaOFeP (supercondu

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

150 ident-photon-energy-modulated angle-resolved photoemission spectroscopy (IPEM-ARPES), we report the d

151 edge X-ray absorption spectroscopy (NEXAFS), photoemission spectroscopy (PES), X-ray diffraction (XRD

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

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

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

155 Ultraviolet photoemission spectroscopy (UPS) indicates that the decr

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

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

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

159 nergy electron diffraction (LEED), and X-ray photoemission spectroscopy (XPS).

160 tates that have distinct signatures in X-ray photoemission spectroscopy and 'ionic radii' which vary

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

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

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

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

165 terface by means of time-resolved two-photon photoemission spectroscopy and electronic structure theo

166 layered metallic systems with angle-resolved photoemission spectroscopy and electronic transport meas

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

168 Using in situ photoemission spectroscopy and online product analysis,

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

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

171 Using 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 We used angle-resolved photoemission spectroscopy applied to deeply underdoped

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

180 Comparison of the dispersions with photoemission spectroscopy data indicates that quasipart

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

182 Angle-resolved photoemission spectroscopy experiments have revealed a k

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

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

185 We report angle-resolved photoemission spectroscopy experiments which probe the 4

186 As in photoemission spectroscopy for electronic materials, our

187 ue can provide an analogue of angle-resolved photoemission spectroscopy for probing anisotropic syste

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

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

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

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

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

193 X-ray photoemission spectroscopy measurements indicate a shift

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

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

196 Our angle-resolved photoemission spectroscopy measurements performed on the

197 Angle-resolved photoemission spectroscopy measurements reveal a small a

198 Subsequent angle-resolved photoemission spectroscopy measurements reveal an unusua

199 theoretical calculations and angle-resolved photoemission spectroscopy measurements.

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

201 ave been quantitatively measured using X-ray photoemission spectroscopy on a 15 microm aqueous liquid

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

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

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

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

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

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

208 X-ray photoemission spectroscopy revealed that the Pd 3d bindi

209 scopy, spectroscopic ellipsometry, and X-ray photoemission spectroscopy shows that the films assemble

210 Angle-resolved photoemission spectroscopy shows the characteristic Dira

211 iolet photoelectron spectroscopy and inverse photoemission spectroscopy studies have been performed t

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

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

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

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

216 Here we use photoemission spectroscopy to directly probe the element

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

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

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

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

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

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

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

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

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

226 g tunnelling spectroscopy and angle-resolved photoemission spectroscopy to visualize the gapless surf

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

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

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

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

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

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

236 raviolet photoelectron spectroscopy, inverse photoemission spectroscopy, and Kelvin probe techniques.

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

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

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

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

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

242 nity of the compound, determined via inverse photoemission spectroscopy, is 5.6 eV, which is 0.4 eV l

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

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

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

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

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

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

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

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

251 surface state of Bi2Te3 with angle-resolved photoemission spectroscopy, we demonstrate that the surf

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 icroscopy in conjunction with angle-resolved photoemission spectroscopy.

264 nd reduction were studied with high pressure photoemission spectroscopy.

265 ir spectral function using momentum-resolved photoemission spectroscopy.

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

267 of two spectral weights using angle-resolved photoemission spectroscopy.

268 troscopy using CO as a probe and ultraviolet photoemission spectroscopy.

269 ion scattering spectroscopy, and ultraviolet photoemission spectroscopy.

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

271 ferent oxygen isotopes, using angle-resolved photoemission spectroscopy.

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

273 evealed by spatially resolved angle-resolved photoemission spectroscopy.

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

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

276 be the overall lineshape of the experimental photoemission spectrum.

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

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

279 Here we report a photoemission study of the underdoped copper oxide Bi(2)

280 combined theoretical and experimental (STM, photoemission) study of the molecular-scale factors invo

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

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

283 find an unusually sharp, reversible decay in photoemission that occurs as such filaments are cycled f

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

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 used synchrotron radiation-based soft x-ray photoemission to show that monolayer films of Pt, Pd, on

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

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

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

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 ent blue (15 A) or green (25-40 A) band-edge photoemission with luminescence quantum yields up to 23%

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