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1  graphitic carbon support (accessed via C 1s photoemission spectroscopy).
2 nd reduction were studied with high pressure photoemission spectroscopy.
3 ir spectral function using momentum-resolved photoemission spectroscopy.
4 hene by using high-resolution angle-resolved photoemission spectroscopy.
5 of two spectral weights using angle-resolved photoemission spectroscopy.
6 challenge is overcome by using time-resolved photoemission spectroscopy.
7 troscopy using CO as a probe and ultraviolet photoemission spectroscopy.
8 ion scattering spectroscopy, and ultraviolet photoemission spectroscopy.
9 ferent oxygen isotopes, using angle-resolved photoemission spectroscopy.
10 r parameter by means of very high resolution photoemission spectroscopy.
11 tosecond time- and angle-resolved two-photon photoemission spectroscopy.
12 ulk ReSe2 by direct nanoscale angle-resolved photoemission spectroscopy.
13 evealed by spatially resolved angle-resolved photoemission spectroscopy.
14 can be tested via laser-based angle-resolved photoemission spectroscopy.
15 s of Sr0.06Bi2Se3 (Tc ~ 2.5 K) by performing photoemission spectroscopy.
16 icroscopy in conjunction with angle-resolved photoemission spectroscopy.
17 e is essentially based on the angle resolved photoemission spectroscopy, a highly surface sensitive t
18 he gas are performed using momentum-resolved photoemission spectroscopy, analogous to angle-resolved
19 tates that have distinct signatures in X-ray photoemission spectroscopy and 'ionic radii' which vary
20               By carrying out angle-resolved photoemission spectroscopy and ab initio calculations on
21 combination of studies involving ultraviolet photoemission spectroscopy and density functional theory
22              Here we utilized angle-resolved photoemission spectroscopy and density functional theory
23 ture of Bi(2)Se(3) employing high resolution photoemission spectroscopy and discover the dependence o
24 terface by means of time-resolved two-photon photoemission spectroscopy and electronic structure theo
25 layered metallic systems with angle-resolved photoemission spectroscopy and electronic transport meas
26 tries, using a combination of angle-resolved photoemission spectroscopy and first-principles calculat
27                                Using in situ photoemission spectroscopy and online product analysis,
28 f a DSM that can be tested by angle-resolved photoemission spectroscopy and quantum oscillation exper
29 isted graphene confirmed by angular resolved photoemission spectroscopy and Raman analysis.
30                         Using angle-resolved photoemission spectroscopy and scanning tunneling micros
31 ted LaNiO3 (LNO) films, using angle-resolved photoemission spectroscopy and the dynamical mean-field
32                           Our angle-resolved photoemission spectroscopy and theoretical results show
33                  We performed angle-resolved photoemission spectroscopy and tight binding calculation
34                     Moreover, angle-resolved photoemission spectroscopy and tight-binding calculation
35                                Through X-ray photoemission spectroscopy and X-ray absorption measurem
36 (3-alpha)Fgamma films, as confirmed by X-ray photoemission spectroscopy and X-ray absorption spectros
37 oss analysis using optical characterization, photoemission spectroscopy, and device modeling, directi
38 raviolet photoelectron spectroscopy, inverse photoemission spectroscopy, and Kelvin probe techniques.
39                       We used angle-resolved photoemission spectroscopy applied to deeply underdoped
40 magnetic BaCr2As2 by means of angle-resolved photoemission spectroscopy (ARPES) and first-principles
41 ed (Bi, Sb)2Te3 thin films by angle-resolved photoemission spectroscopy (ARPES) and show unambiguousl
42  a systematic high-resolution angle-resolved photoemission spectroscopy (ARPES) and spin-resolved ARP
43 ere, we present evidence from angle-resolved photoemission spectroscopy (ARPES) for negative electron
44  FeSe on SrTiO3 (STO)(001) by angle-resolved photoemission spectroscopy (ARPES) has led to the conjec
45 omentum-space discrimination, angle-resolved photoemission spectroscopy (ARPES) is ideally suited for
46 tional ultraviolet/soft X-ray angle-resolved photoemission spectroscopy (ARPES) may in some cases be
47 nducting gaps observed in the angle-resolved photoemission spectroscopy (ARPES) measurement.
48   Detailed comparison between angle-resolved photoemission spectroscopy (ARPES) measurements and dens
49                               Angle-resolved photoemission spectroscopy (ARPES) measurements combined
50                Here we report angle-resolved photoemission spectroscopy (ARPES) of LaOFeP (supercondu
51           Here, by performing angle-resolved photoemission spectroscopy (ARPES) on NbP and TaP, we di
52               Here, we report angle-resolved photoemission spectroscopy (ARPES) results from Rb dosed
53            Here we present an angle-resolved photoemission spectroscopy (ARPES) study of the Kondo la
54            Here we present an angle-resolved photoemission spectroscopy (ARPES) study of the trilayer
55          In this work, we use angle-resolved photoemission spectroscopy (ARPES) to investigate the in
56 l has been investigated using angle-resolved photoemission spectroscopy (ARPES) to reveal a single Di
57  mapping near the X-point via angle resolved photoemission spectroscopy (ARPES) with a Dirac nodal li
58 oy optical spectroscopy (OS), angle-resolved photoemission spectroscopy (ARPES), ab initio band-struc
59                         Using angle-resolved photoemission spectroscopy (ARPES), we observe a quantum
60                         Using angle-resolved photoemission spectroscopy (ARPES), we show that lithium
61 tropic Eliashberg theory, and angle-resolved photoemission spectroscopy (ARPES), we show that surface
62                         Using angle-resolved photoemission spectroscopy (ARPES), we unravel the uniqu
63  inaccessible to conventional angle-resolved photoemission spectroscopy (ARPES).
64 gy and polarization dependent angle-resolved photoemission spectroscopy (ARPES).
65                                   Pump-probe photoemission spectroscopy can track these states by mea
66                     Spin- and angle-resolved photoemission spectroscopy, complemented by theoretical
67           Comparison of the dispersions with photoemission spectroscopy data indicates that quasipart
68                           By combining x-ray photoemission spectroscopy, density functional theory, a
69  absorption spectroscopy combined with X-ray photoemission spectroscopy, electrical transport and the
70 f indium selenide by means of angle-resolved photoemission spectroscopy, electron energy loss spectro
71  measured in UV photoelectron and two-photon photoemission spectroscopy experiments can be assigned t
72                               Angle-resolved photoemission spectroscopy experiments have revealed a k
73      However, theoretical investigations and photoemission spectroscopy experiments indicate that in
74 g tunnelling spectroscopy and angle-resolved photoemission spectroscopy experiments that the recently
75                     We report angle-resolved photoemission spectroscopy experiments which probe the 4
76                                        As in photoemission spectroscopy for electronic materials, our
77 ue can provide an analogue of angle-resolved photoemission spectroscopy for probing anisotropic syste
78 lysis in combination with infrared and X-ray photoemission spectroscopies has shown the anatase nanoc
79 ction (LEED), high resolution angle-resolved photoemission spectroscopy (HR-ARPES), and scanning tunn
80 1) heterointerface using soft and hard x-ray photoemission spectroscopy in conjunction with detailed
81 on spectroscopy, analogous to angle-resolved photoemission spectroscopy in the solid state.
82 ing tunnelling microscopy and angle-resolved photoemission spectroscopy, in combination with first-pr
83 ident-photon-energy-modulated angle-resolved photoemission spectroscopy (IPEM-ARPES), we report the d
84               Standing-wave ambient-pressure photoemission spectroscopy is thus a very promising tech
85                       Femtosecond two-photon photoemission spectroscopy is used to inject an electron
86 nity of the compound, determined via inverse photoemission spectroscopy, is 5.6 eV, which is 0.4 eV l
87                     In ZrSiS, angle-resolved photoemission spectroscopy measurements have shown an un
88                                        X-ray photoemission spectroscopy measurements indicate a shift
89                    Subsequent angle-resolved photoemission spectroscopy measurements of the FeSe/STO
90                               Angle-resolved photoemission spectroscopy measurements on cleaved Bi(2)
91                           Our angle-resolved photoemission spectroscopy measurements performed on the
92                               Angle-resolved photoemission spectroscopy measurements reveal a small a
93                    Subsequent angle-resolved photoemission spectroscopy measurements reveal an unusua
94  theoretical calculations and angle-resolved photoemission spectroscopy measurements.
95                         Using angle-resolved photoemission spectroscopy, modelling, density functiona
96      Here we report angle- and spin-resolved photoemission spectroscopy of WTe2 single crystals, thro
97 ave been quantitatively measured using X-ray photoemission spectroscopy on a 15 microm aqueous liquid
98                   Here, using angle-resolved photoemission spectroscopy on detwinned underdoped Ba(1-
99 in monolayer samples by using angle-resolved photoemission spectroscopy on high-quality thin films of
100 re, we report high-resolution angle-resolved photoemission spectroscopy on MoSe2 single crystals and
101              We use nanoscale angle-resolved photoemission spectroscopy on single nanowires (nano-ARP
102 edge X-ray absorption spectroscopy (NEXAFS), photoemission spectroscopy (PES), X-ray diffraction (XRD
103 g three different techniques (angle-resolved photoemission spectroscopy, polar Kerr effect, and time-
104 photoelectron spectroscopy and standing-wave photoemission spectroscopy provides the spatial arrangem
105             We use pump-probe angle-resolved photoemission spectroscopy (pump-probe ARPES) to directl
106                                              Photoemission spectroscopy results show that films of N
107 ere we report high-resolution angle-resolved photoemission spectroscopy results that reveal an unexpe
108                                        X-ray photoemission spectroscopy revealed that the Pd 3d bindi
109   We characterize Sn-BSTS via angle-resolved photoemission spectroscopy, scanning tunnelling microsco
110 bdenum trioxide (MoO3), is studied combining photoemission spectroscopy, sheet resistance measurement
111 scopy, spectroscopic ellipsometry, and X-ray photoemission spectroscopy shows that the films assemble
112                               Angle-resolved photoemission spectroscopy shows the characteristic Dira
113               By using synchrotron radiation photoemission spectroscopy (SRPES), extended X-ray absor
114 iolet photoelectron spectroscopy and inverse photoemission spectroscopy studies have been performed t
115 e we report a high-resolution angle-resolved photoemission spectroscopy study on LiFe(1-x)CoxAs.
116 an and sp(3) bonding characteristic in X-ray photoemission spectroscopy suggests the existence of int
117  combination of magnetometry, spin-polarized photoemission spectroscopy, symmetry arguments and first
118 de molecular-beam epitaxy and angle-resolved photoemission spectroscopy system to synthesize and inve
119            Here we show using angle resolved photoemission spectroscopy that twin-grain boundaries in
120 ity functional theory calculations and X-ray photoemission spectroscopy, the surface-assisted reactio
121                                  Here we use photoemission spectroscopy to directly probe the element
122                       We used angle-resolved photoemission spectroscopy to experimentally observe a p
123                                  Here we use photoemission spectroscopy to image the formation of pro
124                  Here, we use angle-resolved photoemission spectroscopy to measure three representati
125                   Here we use angle-resolved photoemission spectroscopy to probe electron dynamics-ve
126       We used high-resolution angle-resolved photoemission spectroscopy to reveal the Fermi surface a
127                        We use angle-resolved photoemission spectroscopy to show that the two-gap beha
128 e core-hole clock implementation of resonant photoemission spectroscopy to study the femtosecond char
129        Here, we use time- and angle-resolved photoemission spectroscopy to study the initial rise of
130                  Here we apply time-resolved photoemission spectroscopy to the tetracene/C(60) interf
131               Here we perform angle-resolved photoemission spectroscopy to try to find an electron do
132                  Here, we use angle-resolved photoemission spectroscopy to uncover an abrupt destruct
133 g tunnelling spectroscopy and angle-resolved photoemission spectroscopy to visualize the gapless surf
134 rt herein a time-resolved and angle-resolved photoemission spectroscopy (TRARPES) study of WSe2, a la
135                                  Ultraviolet photoemission spectroscopy (UPS) indicates that the decr
136 of the photoelectrons emitted in ultraviolet photoemission spectroscopy (UPS) to determine the electr
137 on near-edge structure (XANES), valence-band photoemission spectroscopy (VB-PES), X-ray emission spec
138                               Angle-resolved photoemission spectroscopy was carried out on (La(1.28)N
139 ular beam epitaxy and in situ angle-resolved photoemission spectroscopy we show that valence fluctuat
140 , using femtosecond time- and angle-resolved photoemission spectroscopy, we demonstrate a tendency to
141               Using spin- and angle-resolved photoemission spectroscopy, we demonstrate that such a s
142  surface state of Bi2Te3 with angle-resolved photoemission spectroscopy, we demonstrate that the surf
143 ronic structure of Na3Bi with angle-resolved photoemission spectroscopy, we detected 3D Dirac fermion
144           Here, by performing angle-resolved photoemission spectroscopy, we directly observe a pair o
145                                        Using photoemission spectroscopy, we directly observe Fermi ar
146                          With angle-resolved photoemission spectroscopy, we directly observed almost
147            By using time- and angle-resolved photoemission spectroscopy, we investigate the ultrafast
148  simultaneous spin, time, and angle-resolved photoemission spectroscopy, we map the spin-polarized un
149   Here, using high-resolution angle-resolved photoemission spectroscopy, we performed systematic elec
150      Here, by using spin- and angle-resolved photoemission spectroscopy, we report the observation of
151 oxide-semiconductor interface via hard x-ray photoemission spectroscopy, we show how to systematicall
152               Using time- and angle-resolved photoemission spectroscopy, we show that an intense ultr
153 si-freestanding graphene with angle-resolved photoemission spectroscopy, we showed that at finite dop
154 tron microscopy, x-ray diffraction and x-ray photoemission spectroscopy were utilised to perform a st
155 ere, we employed state-of-the-art hard x-ray photoemission spectroscopy with judiciously chosen exper
156                 Here, by using spin-resolved photoemission spectroscopy with p-polarized light in top
157           In this work, using angle-resolved photoemission spectroscopy with sub-micrometer spatial r
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).

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