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1  graphitic carbon support (accessed via C 1s photoemission spectroscopy).
2 mal state, investigated using angle-resolved photoemission spectroscopy.
3 icroscopy in conjunction with angle-resolved photoemission spectroscopy.
4 nd reduction were studied with high pressure photoemission spectroscopy.
5 ir spectral function using momentum-resolved photoemission spectroscopy.
6 hene by using high-resolution angle-resolved photoemission spectroscopy.
7 of two spectral weights using angle-resolved photoemission spectroscopy.
8 troscopy using CO as a probe and ultraviolet photoemission spectroscopy.
9 ion scattering spectroscopy, and ultraviolet photoemission spectroscopy.
10 ferent oxygen isotopes, using angle-resolved photoemission spectroscopy.
11 r parameter by means of very high resolution photoemission spectroscopy.
12 tosecond time- and angle-resolved two-photon photoemission spectroscopy.
13 e material, using laser-based angle-resolved photoemission spectroscopy.
14 " We studied this state using angle-resolved photoemission spectroscopy.
15 ic evolution with x, by using angle resolved photoemission spectroscopy.
16 e at the Y point is proven by angle-resolved photoemission spectroscopy.
17 s with ~0.2 eV at point using angle-resolved photoemission spectroscopy.
18 ctronic structure measured by angle-resolved photoemission spectroscopy.
19  spin-integrated soft X-ray angular resolved photoemission spectroscopy.
20 y synchrotron and laser-based angle-resolved photoemission spectroscopy.
21 challenge is overcome by using time-resolved photoemission spectroscopy.
22 ulk ReSe2 by direct nanoscale angle-resolved photoemission spectroscopy.
23 evealed by spatially resolved angle-resolved photoemission spectroscopy.
24 can be tested via laser-based angle-resolved photoemission spectroscopy.
25 utional diffusion and in-situ angle-resolved photoemission spectroscopy.
26 s of Sr0.06Bi2Se3 (Tc ~ 2.5 K) by performing photoemission spectroscopy.
27 e show that micrometre-scale, angle-resolved photoemission spectroscopy(1-3) (microARPES) applied to
28 e is essentially based on the angle resolved photoemission spectroscopy, a highly surface sensitive t
29 he gas are performed using momentum-resolved photoemission spectroscopy, analogous to angle-resolved
30 tates that have distinct signatures in X-ray photoemission spectroscopy and 'ionic radii' which vary
31           Here, using tunnelling microscopy, photoemission spectroscopy and a theoretical analysis, w
32               By carrying out angle-resolved photoemission spectroscopy and ab initio calculations on
33       Here we provide the confirmation using photoemission spectroscopy and ab initio calculations.
34 3)Sb(5) using high-resolution angle-resolved photoemission spectroscopy and ab-initio calculations.
35 ated kagome metal CoSn, using angle-resolved photoemission spectroscopy and band structure calculatio
36        In this work, by using angle-resolved photoemission spectroscopy and conductivity measurement,
37                                  Ultraviolet photoemission spectroscopy and contact potential differe
38 nd 2H-TaSe(2) complemented by angle-resolved photoemission spectroscopy and density functional pertur
39 combination of studies involving ultraviolet photoemission spectroscopy and density functional theory
40                  Here, we use angle-resolved photoemission spectroscopy and density functional theory
41              Here we utilized angle-resolved photoemission spectroscopy and density functional theory
42 ture of Bi(2)Se(3) employing high resolution photoemission spectroscopy and discover the dependence o
43 terface by means of time-resolved two-photon photoemission spectroscopy and electronic structure theo
44 layered metallic systems with angle-resolved photoemission spectroscopy and electronic transport meas
45  Here, using 7-eV laser-based angle-resolved photoemission spectroscopy and Eliashberg function analy
46 canning tunneling microscopy, angle-resolved photoemission spectroscopy and first-principles calculat
47                         Using angle-resolved photoemission spectroscopy and first-principles calculat
48 tries, using a combination of angle-resolved photoemission spectroscopy and first-principles calculat
49 n, which we cross-validate by applying X-ray photoemission spectroscopy and Hall effect measurements
50 ome these limitations, we use angle-resolved photoemission spectroscopy and molecular beam epitaxy to
51                   Here, using angle-resolved photoemission spectroscopy and numerical simulations, we
52                                Using in situ photoemission spectroscopy and online product analysis,
53 f a DSM that can be tested by angle-resolved photoemission spectroscopy and quantum oscillation exper
54 i/2) of the Brillouin zone by angle-resolved photoemission spectroscopy and quantum oscillation measu
55  Here, using a combination of angle-resolved photoemission spectroscopy and quantum oscillation measu
56                        In this study, we use photoemission spectroscopy and quantum transport to eluc
57  layer of Sr(2)RuO(4) against angle-resolved photoemission spectroscopy and quasiparticle interferenc
58 isted graphene confirmed by angular resolved photoemission spectroscopy and Raman analysis.
59         In this work, through angle-resolved photoemission spectroscopy and scanning tunneling micros
60      In this work, we combine angle-resolved photoemission spectroscopy and scanning tunneling micros
61                         Using angle-resolved photoemission spectroscopy and scanning tunneling micros
62    Utilizing state-of-the-art angle-resolved photoemission spectroscopy and self-consistent ab-initio
63 ted LaNiO3 (LNO) films, using angle-resolved photoemission spectroscopy and the dynamical mean-field
64                           Our angle-resolved photoemission spectroscopy and theoretical results show
65                  We performed angle-resolved photoemission spectroscopy and tight binding calculation
66                     Moreover, angle-resolved photoemission spectroscopy and tight-binding calculation
67               Using time- and angle-resolved photoemission spectroscopy and time-resolved X-ray diffr
68                                Through X-ray photoemission spectroscopy and X-ray absorption measurem
69 (3-alpha)Fgamma films, as confirmed by X-ray photoemission spectroscopy and X-ray absorption spectros
70 e[Formula: see text] band offset using X-ray photoemission spectroscopy, and chart the elemental comp
71 canning tunneling microscopy, angle-resolved photoemission spectroscopy, and density functional theor
72 oss analysis using optical characterization, photoemission spectroscopy, and device modeling, directi
73 raviolet photoelectron spectroscopy, inverse photoemission spectroscopy, and Kelvin probe techniques.
74       By comparing ambient pressure resonant photoemission spectroscopy (AP-ResPES) measurements with
75                       We used angle-resolved photoemission spectroscopy applied to deeply underdoped
76   Here, using high-resolution angle-resolved photoemission spectroscopy (ARPES) along with first-prin
77 rconductor RbFe(2)As(2) using angle-resolved photoemission spectroscopy (ARPES) and dynamical mean fi
78        By performing in-vacuo angle-resolved photoemission spectroscopy (ARPES) and ex-situ electrica
79 magnetic BaCr2As2 by means of angle-resolved photoemission spectroscopy (ARPES) and first-principles
80           In this work, using angle-resolved photoemission spectroscopy (ARPES) and high-resolution s
81 plementary momentum-sensitive angle-resolved photoemission spectroscopy (ARPES) and low-energy electr
82 he extremely low disorder, by angle-resolved photoemission spectroscopy (ARPES) and quantum oscillati
83 e(2) and its investigation by angle-resolved photoemission spectroscopy (ARPES) and scanning tunnelin
84  we study this question using angle-resolved photoemission spectroscopy (ARPES) and scanning tunnelin
85                     Here, via angle-resolved photoemission spectroscopy (ARPES) and scanning tunnelli
86 ed (Bi, Sb)2Te3 thin films by angle-resolved photoemission spectroscopy (ARPES) and show unambiguousl
87  a systematic high-resolution angle-resolved photoemission spectroscopy (ARPES) and spin-resolved ARP
88                  By combining angle-resolved photoemission spectroscopy (ARPES) and x-ray absorption
89 ere, we present evidence from angle-resolved photoemission spectroscopy (ARPES) for negative electron
90  FeSe on SrTiO3 (STO)(001) by angle-resolved photoemission spectroscopy (ARPES) has led to the conjec
91                               Angle-resolved photoemission spectroscopy (ARPES) has played a key role
92 omentum-space discrimination, angle-resolved photoemission spectroscopy (ARPES) is ideally suited for
93 tional ultraviolet/soft X-ray angle-resolved photoemission spectroscopy (ARPES) may in some cases be
94 nducting gaps observed in the angle-resolved photoemission spectroscopy (ARPES) measurement.
95 s and performed comprehensive angle-resolved photoemission spectroscopy (ARPES) measurements and band
96   Detailed comparison between angle-resolved photoemission spectroscopy (ARPES) measurements and dens
97                               Angle-resolved photoemission spectroscopy (ARPES) measurements combined
98 ), we present high-resolution angle-resolved photoemission spectroscopy (ARPES) measurements of the B
99 es calculations combined with angle-resolved photoemission spectroscopy (ARPES) measurements show tha
100 by performing high-resolution angle-resolved photoemission spectroscopy (ARPES) measurements with sub
101 single-layer ZrTe(2) based on angle-resolved photoemission spectroscopy (ARPES) measurements.
102                Here we report angle-resolved photoemission spectroscopy (ARPES) of LaOFeP (supercondu
103           Here, by performing angle-resolved photoemission spectroscopy (ARPES) on NbP and TaP, we di
104   Conventional probes such as angle-resolved photoemission spectroscopy (ARPES) or scanning tunneling
105               Here, we report angle-resolved photoemission spectroscopy (ARPES) results from Rb dosed
106 his dichotomy of the observed angle-resolved photoemission spectroscopy (ARPES) spectra is similarly
107                   A series of angle-resolved photoemission spectroscopy (ARPES) studies were performe
108 carried out a high-resolution angle-resolved photoemission spectroscopy (ARPES) study of a CDW materi
109            Here we present an angle-resolved photoemission spectroscopy (ARPES) study of the Kondo la
110           Here, we present an angle-resolved photoemission spectroscopy (ARPES) study of the trilayer
111            Here we present an angle-resolved photoemission spectroscopy (ARPES) study of the trilayer
112  puzzle with a high-precision angle-resolved photoemission spectroscopy (ARPES) study on overdoped (B
113 ns using Raman scattering and angle-resolved photoemission spectroscopy (ARPES) to examine the phonon
114          In this work, we use angle-resolved photoemission spectroscopy (ARPES) to investigate the in
115 pulses can be used to perform angle-resolved photoemission spectroscopy (ARPES) to map the electronic
116 l has been investigated using angle-resolved photoemission spectroscopy (ARPES) to reveal a single Di
117                   Here we use angle-resolved photoemission spectroscopy (ARPES) to study FeSb(2), a c
118 0.60) have been determined by angle-resolved photoemission spectroscopy (ARPES) using synchrotron rad
119  mapping near the X-point via angle resolved photoemission spectroscopy (ARPES) with a Dirac nodal li
120 oy optical spectroscopy (OS), angle-resolved photoemission spectroscopy (ARPES), ab initio band-struc
121           Here we show, using angle-resolved photoemission spectroscopy (ARPES), that in V(2)O(3), th
122                         Using angle-resolved photoemission spectroscopy (ARPES), we observe a quantum
123                         Using angle-resolved photoemission spectroscopy (ARPES), we show that lithium
124 tropic Eliashberg theory, and angle-resolved photoemission spectroscopy (ARPES), we show that surface
125                         Using angle-resolved photoemission spectroscopy (ARPES), we unravel the uniqu
126 suring magnetic domains using angle-resolved photoemission spectroscopy (ARPES).
127 ectron diffraction (LEED) and angle-resolved photoemission spectroscopy (ARPES).
128 ormula: see text] measured by angle-resolved photoemission spectroscopy (ARPES).
129  inaccessible to conventional angle-resolved photoemission spectroscopy (ARPES).
130 gy and polarization dependent angle-resolved photoemission spectroscopy (ARPES).
131 candidate ZrTe(5) by spin and angle-resolved photoemission spectroscopy (ARPES): a quasi-1D band with
132 EED), low-energy electron microscopy (LEEM), photoemission spectroscopy as well as density functional
133                                           By photoemission spectroscopy below the Curie temperature,
134       Using a combination of vibrational and photoemission spectroscopies, bonding of the two peptide
135                                   Pump-probe photoemission spectroscopy can track these states by mea
136 ed that circular dichroism in angle-resolved photoemission spectroscopy (CD-ARPES) can be used to obs
137                     Spin- and angle-resolved photoemission spectroscopy, complemented by theoretical
138                         Using angle-resolved photoemission spectroscopy, crossing points formed by th
139           Comparison of the dispersions with photoemission spectroscopy data indicates that quasipart
140 tunneling microscopy, ambient-pressure X-ray photoemission spectroscopy, density functional calculati
141 udy, through state-of-the-art angle-resolved photoemission spectroscopy, density functional theory, a
142                           By combining x-ray photoemission spectroscopy, density functional theory, a
143        By using micro-focused angle-resolved photoemission spectroscopy during in situ doping of the
144 FeCoNi alloy using resonant and valence band photoemission spectroscopy, electrical resistivity, and
145  absorption spectroscopy combined with X-ray photoemission spectroscopy, electrical transport and the
146 f indium selenide by means of angle-resolved photoemission spectroscopy, electron energy loss spectro
147  measured in UV photoelectron and two-photon photoemission spectroscopy experiments can be assigned t
148                               Angle-resolved photoemission spectroscopy experiments have revealed a k
149      However, theoretical investigations and photoemission spectroscopy experiments indicate that in
150 g tunnelling spectroscopy and angle-resolved photoemission spectroscopy experiments that the recently
151                     We report angle-resolved photoemission spectroscopy experiments which probe the 4
152                                        As in photoemission spectroscopy for electronic materials, our
153 ue can provide an analogue of angle-resolved photoemission spectroscopy for probing anisotropic syste
154 lysis in combination with infrared and X-ray photoemission spectroscopies has shown the anatase nanoc
155   Here, femtosecond time-resolved two-photon photoemission spectroscopy has been used to probe the el
156 ction (LEED), high resolution angle-resolved photoemission spectroscopy (HR-ARPES), and scanning tunn
157 t-principles calculations and angle-resolved photoemission spectroscopy identify van Hove singulariti
158 the electronic structure with angle-resolved photoemission spectroscopy in a kagome magnet thin film
159 1) heterointerface using soft and hard x-ray photoemission spectroscopy in conjunction with detailed
160 on spectroscopy, analogous to angle-resolved photoemission spectroscopy in the solid state.
161 ing tunnelling microscopy and angle-resolved photoemission spectroscopy, in combination with first-pr
162 ident-photon-energy-modulated angle-resolved photoemission spectroscopy (IPEM-ARPES), we report the d
163               Standing-wave ambient-pressure photoemission spectroscopy is thus a very promising tech
164                       Femtosecond two-photon photoemission spectroscopy is used to inject an electron
165 nity of the compound, determined via inverse photoemission spectroscopy, is 5.6 eV, which is 0.4 eV l
166                                   Liquid-jet photoemission spectroscopy (LJ-PES) allows for a direct
167   Here, using high-resolution angle-resolved photoemission spectroscopy, magnetotransport, and parall
168 he polarization dependence of angle-resolved photoemission spectroscopy measurement.
169 eutron scattering, soft x-ray angle-resolved photoemission spectroscopy measurements and ab-initio la
170                           Our angle-resolved photoemission spectroscopy measurements and first-princi
171                     In ZrSiS, angle-resolved photoemission spectroscopy measurements have shown an un
172                                        X-ray photoemission spectroscopy measurements indicate a shift
173                         Using angle resolved photoemission spectroscopy measurements of Bi(2)Sr(2)CaC
174                    Subsequent angle-resolved photoemission spectroscopy measurements of the FeSe/STO
175                Here we report angle-resolved photoemission spectroscopy measurements on a cuprate par
176                               Angle-resolved photoemission spectroscopy measurements on cleaved Bi(2)
177      In this work, we conduct angle-resolved photoemission spectroscopy measurements on monolayer FeS
178                           Our angle-resolved photoemission spectroscopy measurements performed on the
179                               Angle-resolved photoemission spectroscopy measurements reveal a small a
180                    Subsequent angle-resolved photoemission spectroscopy measurements reveal an unusua
181         In situ transport and angle-resolved photoemission spectroscopy measurements reveal the metal
182 at agrees quantitatively with angle-resolved photoemission spectroscopy measurements(7) and reveals a
183 tes splitting observed by our angle-resolved photoemission spectroscopy measurements.
184 and effective model analyses, angle-resolved photoemission spectroscopy measurements.
185  theoretical calculations and angle-resolved photoemission spectroscopy measurements.
186                         Using angle-resolved photoemission spectroscopy, modelling, density functiona
187 n state-specific near-ambient pressure X-ray photoemission spectroscopy (NAP-XPS) to probe charge tra
188 rs using dynamic near-ambient pressure X-ray photoemission spectroscopy (NAP-XPS).
189 iques of carrier kinetics and densities, air photoemission spectroscopy of material energetics, Kelvi
190   In this work, we report the angle-resolved photoemission spectroscopy of superconducting La(0.8)Sr(
191      Here we report angle- and spin-resolved photoemission spectroscopy of WTe2 single crystals, thro
192 ave been quantitatively measured using X-ray photoemission spectroscopy on a 15 microm aqueous liquid
193                   Here, using angle-resolved photoemission spectroscopy on detwinned underdoped Ba(1-
194 in monolayer samples by using angle-resolved photoemission spectroscopy on high-quality thin films of
195 re, we report high-resolution angle-resolved photoemission spectroscopy on MoSe2 single crystals and
196              We use nanoscale angle-resolved photoemission spectroscopy on single nanowires (nano-ARP
197                                        Using photoemission spectroscopy (PES), we have systematically
198 edge X-ray absorption spectroscopy (NEXAFS), photoemission spectroscopy (PES), X-ray diffraction (XRD
199 g three different techniques (angle-resolved photoemission spectroscopy, polar Kerr effect, and time-
200 photoelectron spectroscopy and standing-wave photoemission spectroscopy provides the spatial arrangem
201             We use pump-probe angle-resolved photoemission spectroscopy (pump-probe ARPES) to directl
202 e, we combine high-resolution angle-resolved photoemission spectroscopy, Raman scattering and density
203                         Using angle-resolved photoemission spectroscopy, resonant inelastic X-ray sca
204                                     Resonant photoemission spectroscopy (ResPES) revealed the unique
205                                              Photoemission spectroscopy results show that films of N
206 ere we report high-resolution angle-resolved photoemission spectroscopy results that reveal an unexpe
207                                        X-ray photoemission spectroscopy revealed that the Pd 3d bindi
208                                              Photoemission spectroscopy revealed that ZnTPP-P-Ipa par
209 rometric time- and angle-resolved two-photon photoemission spectroscopy reveals dark exciton dynamics
210 onic structure by synergistic angle-resolved photoemission spectroscopy, scanning tunneling microscop
211 erromagnetic metal, FeTe, via angle-resolved photoemission spectroscopy, scanning tunneling spectrosc
212   We characterize Sn-BSTS via angle-resolved photoemission spectroscopy, scanning tunnelling microsco
213 bdenum trioxide (MoO3), is studied combining photoemission spectroscopy, sheet resistance measurement
214 scopy, spectroscopic ellipsometry, and X-ray photoemission spectroscopy shows that the films assemble
215                               Angle-resolved photoemission spectroscopy shows the characteristic Dira
216               By using synchrotron radiation photoemission spectroscopy (SRPES), extended X-ray absor
217 iolet photoelectron spectroscopy and inverse photoemission spectroscopy studies have been performed t
218                    We present angle-resolved photoemission spectroscopy studies of Bi[Formula: see te
219                  We performed angle-resolved photoemission spectroscopy studies on the triple-layer B
220 e we report a high-resolution angle-resolved photoemission spectroscopy study on LiFe(1-x)CoxAs.
221 an and sp(3) bonding characteristic in X-ray photoemission spectroscopy suggests the existence of int
222  combination of magnetometry, spin-polarized photoemission spectroscopy, symmetry arguments and first
223 de molecular-beam epitaxy and angle-resolved photoemission spectroscopy system to synthesize and inve
224               Here we show by angle-resolved photoemission spectroscopy that paramagnetic EuRh(2)Si(2
225            Here we show using angle resolved photoemission spectroscopy that twin-grain boundaries in
226 ity functional theory calculations and X-ray photoemission spectroscopy, the surface-assisted reactio
227                                  Here we use photoemission spectroscopy to directly probe the element
228        Here, we use spin- and angle-resolved photoemission spectroscopy to evidence Weyl spin-momentu
229                       We used angle-resolved photoemission spectroscopy to experimentally observe a p
230                                  Here we use photoemission spectroscopy to image the formation of pro
231                  Here, we use angle-resolved photoemission spectroscopy to measure three representati
232                   Here we use angle-resolved photoemission spectroscopy to probe electron dynamics-ve
233       We used high-resolution angle-resolved photoemission spectroscopy to reveal the Fermi surface a
234                        We use angle-resolved photoemission spectroscopy to show that the two-gap beha
235 e core-hole clock implementation of resonant photoemission spectroscopy to study the femtosecond char
236        Here, we use time- and angle-resolved photoemission spectroscopy to study the initial rise of
237                  Here we apply time-resolved photoemission spectroscopy to the tetracene/C(60) interf
238               Here we perform angle-resolved photoemission spectroscopy to try to find an electron do
239                  Here, we use angle-resolved photoemission spectroscopy to uncover an abrupt destruct
240 g tunnelling spectroscopy and angle-resolved photoemission spectroscopy to visualize the gapless surf
241                Time-resolved, angle-resolved photoemission spectroscopy (TR-ARPES) is a one-particle
242 s and complementary time- and angle-resolved photoemission spectroscopy (tr-ARPES).
243  time domain, using time- and angle-resolved photoemission spectroscopy (TR-ARPES).
244 s studied by femtosecond time-resolved X-ray photoemission spectroscopy (TR-XPS) at the free-electron
245 rt herein a time-resolved and angle-resolved photoemission spectroscopy (TRARPES) study of WSe2, a la
246                             Applying in situ photoemission spectroscopy under oxygen ambient, ionic a
247 a(IB), in ultraviolet and low-energy inverse photoemission spectroscopy (UPS and LEIPS, respectively)
248                                  Ultraviolet photoemission spectroscopy (UPS) indicates that the decr
249 of the photoelectrons emitted in ultraviolet photoemission spectroscopy (UPS) to determine the electr
250                         By using ultraviolet photoemission spectroscopy (UPS), we show here that expo
251 on near-edge structure (XANES), valence-band photoemission spectroscopy (VB-PES), X-ray emission spec
252                               Angle-resolved photoemission spectroscopy was carried out on (La(1.28)N
253 ular beam epitaxy and in situ angle-resolved photoemission spectroscopy we show that valence fluctuat
254 , using femtosecond time- and angle-resolved photoemission spectroscopy, we demonstrate a tendency to
255               Using spin- and angle-resolved photoemission spectroscopy, we demonstrate that such a s
256  surface state of Bi2Te3 with angle-resolved photoemission spectroscopy, we demonstrate that the surf
257 ronic structure of Na3Bi with angle-resolved photoemission spectroscopy, we detected 3D Dirac fermion
258     By using time-, spin- and angle-resolved photoemission spectroscopy, we directly follow the forma
259           Here, by performing angle-resolved photoemission spectroscopy, we directly observe a pair o
260                                        Using photoemission spectroscopy, we directly observe Fermi ar
261                          With angle-resolved photoemission spectroscopy, we directly observed almost
262        By using micro-focused angle-resolved photoemission spectroscopy, we discovered contrasting su
263                         Using angle-resolved photoemission spectroscopy, we identify two Dirac surfac
264         Here, using time- and angle-resolved photoemission spectroscopy, we investigate the ultrafast
265            By using time- and angle-resolved photoemission spectroscopy, we investigate the ultrafast
266 t synchrotron and laser-based angle-resolved photoemission spectroscopy, we investigated a stoichiome
267  simultaneous spin, time, and angle-resolved photoemission spectroscopy, we map the spin-polarized un
268                         Using angle-resolved photoemission spectroscopy, we observe a band with vanis
269                         Using angle-resolved photoemission spectroscopy, we observe an anomalous ener
270         Here, using time- and angle-resolved photoemission spectroscopy, we obtain a holistic view of
271   Here, using high-resolution angle-resolved photoemission spectroscopy, we performed systematic elec
272                 Here, using multidimensional photoemission spectroscopy, we provide a layer- and mome
273                   Here, using angle-resolved photoemission spectroscopy, we provide an example of thi
274        In this study, through angle-resolved photoemission spectroscopy, we provide comprehensive spe
275      Here, by using spin- and angle-resolved photoemission spectroscopy, we report the observation of
276 ng hard X-ray diffraction and angle-resolved photoemission spectroscopy, we reveal unusual 2D ferro-r
277                       Through angle-resolved photoemission spectroscopy, we show for the first time m
278 oxide-semiconductor interface via hard x-ray photoemission spectroscopy, we show how to systematicall
279               Using time- and angle-resolved photoemission spectroscopy, we show that an intense ultr
280            By using time- and angle-resolved photoemission spectroscopy, we show that intense optical
281 si-freestanding graphene with angle-resolved photoemission spectroscopy, we showed that at finite dop
282           In this work, using angle-resolved photoemission spectroscopy, we visualized the electronic
283 tron microscopy, x-ray diffraction and x-ray photoemission spectroscopy were utilised to perform a st
284 uch as in time-resolved X-ray absorption and photoemission spectroscopy, where improved measurement o
285               Here, combining angle-resolved photoemission spectroscopy with density functional theor
286 ombine polarization-dependent angle-resolved photoemission spectroscopy with density functional theor
287 ombine polarization-dependent angle-resolved photoemission spectroscopy with functional renormalizati
288 ere, we employed state-of-the-art hard x-ray photoemission spectroscopy with judiciously chosen exper
289            Here, by utilizing angle-resolved photoemission spectroscopy with micrometre spatial resol
290  combining spatially resolved angle-resolved photoemission spectroscopy with optical spectroscopy, we
291                 Here, by using spin-resolved photoemission spectroscopy with p-polarized light in top
292      We provide evidence from angle-resolved photoemission spectroscopy with spin resolution, angle-d
293     Combining time-resolved multidimensional photoemission spectroscopy with state-of-the-art TDDFT+U
294           In this work, using angle-resolved photoemission spectroscopy with sub-micrometer spatial r
295                  Here, we use angle-resolved photoemission spectroscopy with submicron spatial resolu
296               Here, we combine time-resolved photoemission spectroscopy with time-resolved magneto-op
297                                        X-ray Photoemission Spectroscopy (XPS) confirmed the formation
298 d reaction (TPR) mass spectrometry and X-ray photoemission spectroscopy (XPS) following exposure to O
299 en these cell components, we carry out X-ray photoemission spectroscopy (XPS) measurements during lit
300 nergy electron diffraction (LEED), and X-ray photoemission spectroscopy (XPS).

 
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