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1 he local density-of-state images obtained by scanning tunnelling microscopy.
2 ed using several advanced techniques such as scanning tunnelling microscopy.
3 ization) reactions in single molecules using scanning tunnelling microscopy.
4 dy nominally stoichiometric Bi(2)Se(3) using scanning tunnelling microscopy.
5 gle-atom depassivation can be achieved using scanning tunnelling microscopy.
6 gle-spin sensitivity, such as spin-polarized scanning tunnelling microscopy.
7 s (hole concentration of 0.12 to 0.22) using scanning tunnelling microscopy.
8 lectron spin on a surface was detected using scanning tunnelling microscopy.
9             Imaging at the atomic scale with scanning tunnelling microscopy allowed for direct charac
10 ymmetry positions in the atomically resolved scanning tunnelling microscopy allows the physical order
11 riodicity is given by kF/pi, consistent with scanning tunnelling microscopy and angle resolved photoe
12 atomic and electronic characterization using scanning tunnelling microscopy and angle-resolved photoe
13                                              Scanning tunnelling microscopy and atomic manipulation c
14                      Here, using time-lapsed scanning tunnelling microscopy and density functional th
15                                              Scanning tunnelling microscopy and density functional th
16                   Here we present a combined scanning tunnelling microscopy and first-principles theo
17                                              Scanning tunnelling microscopy and holograms comprised o
18 trate thermal mirror buckling of graphene by scanning tunnelling microscopy and large-scale molecular
19 wave states with broken symmetry observed in scanning tunnelling microscopy and soft X-ray measuremen
20 t temperatures as low as 260 degrees C using scanning tunnelling microscopy and spectroscopic techniq
21                Here we observe, by utilizing scanning tunnelling microscopy and spectroscopy down to
22                                  Here we use scanning tunnelling microscopy and spectroscopy to follo
23              Here we harness cross-sectional scanning tunnelling microscopy and spectroscopy together
24 we demonstrate that by using low-temperature scanning tunnelling microscopy and spectroscopy we can c
25 junctions at subnanometre length scales with scanning tunnelling microscopy and spectroscopy, and ide
26 ) d-wave superconductor and performing local scanning tunnelling microscopy and spectroscopy, here we
27 omains on Au(111), probed by low-temperature scanning tunnelling microscopy and spectroscopy, reveal
28                        Using low-temperature scanning tunnelling microscopy and spectroscopy, we embe
29                                        Using scanning tunnelling microscopy and spectroscopy, we foun
30                                        Using scanning tunnelling microscopy and spectroscopy, we obse
31 monolayer interface in MoSe2 and WSe2, using scanning tunnelling microscopy and spectroscopy.
32 n-doped graphitic superconductor, CaC(6), by scanning tunnelling microscopy and spectroscopy.
33 of tetramantane diamondoids on Au(111) using scanning tunnelling microscopy and spectroscopy.
34 aCu2O8+x, on the basis of observations using scanning tunnelling microscopy and spectroscopy.
35                          Here we show, using scanning tunnelling microscopy and supported by potentio
36                                              Scanning tunnelling microscopy and surface X-ray diffrac
37           The present combined experimental (scanning tunnelling microscopy) and theoretical (density
38 al ripple geometry was recently imaged using scanning tunnelling microscopy, but these measurements a
39                                              Scanning tunnelling microscopy can locally restore the r
40 allic glass Cu100-xHfx films and demonstrate scanning tunnelling microscopy control of aging at a met
41                   Atomic manipulation in the scanning tunnelling microscopy, conventionally a tool to
42 the development of hybrid techniques such as scanning tunnelling microscopy coupled to confocal scann
43  three different experimental configurations-scanning tunnelling microscopy, crossed-wire junction, a
44  determined through a detailed comparison of scanning tunnelling microscopy data and first-principles
45        Here we use numerical simulations and scanning tunnelling microscopy data to show that these r
46                          Here we show--using scanning tunnelling microscopy, electronic transport mea
47                                              Scanning tunnelling microscopy enables individual rotors
48 rs--through a combination of low-temperature scanning tunnelling microscopy experiments and first-pri
49 glue were therefore encouraged by the recent scanning tunnelling microscopy experiments on hole-doped
50                                     However, scanning tunnelling microscopy has limited applicability
51                                              Scanning tunnelling microscopy has long been used to ima
52                       Surface probes such as scanning tunnelling microscopy have detected complex ele
53                         Detailed analysis of scanning tunnelling microscopy images is used to reconst
54      Atomic-resolution characterization with scanning tunnelling microscopy is quantitatively compare
55                       A severe limitation in scanning tunnelling microscopy is the low temporal resol
56 atest advances in d2I/dV2 spectroscopy using scanning tunnelling microscopy, it has become possible t
57                               Here we report scanning tunnelling microscopy measurements at sub-kelvi
58                                              Scanning tunnelling microscopy measurements of step-edge
59               Here we report high-resolution scanning tunnelling microscopy measurements of the elect
60                               Here we report scanning tunnelling microscopy measurements showing that
61                               Here we report scanning tunnelling microscopy observations of the trans
62                                              Scanning tunnelling microscopy observations resolve the
63                                     Although scanning tunnelling microscopy observations under high v
64  study by scanning transmission electron and scanning tunnelling microscopies on a novel layered mate
65 haracterized at the single-molecule level by scanning tunnelling microscopy, reflection absorption in
66                                              Scanning tunnelling microscopy reveals that the yttria l
67            Here we use spectroscopic imaging scanning tunnelling microscopy (SI-STM) to image the evo
68                                        Using scanning tunnelling microscopy/spectroscopy and first-pr
69  surface of in situ cleaved IrTe(2) by using scanning tunnelling microscopy/spectroscopy, corroborate
70 crobeam X-ray photoelectron spectroscopy and scanning tunnelling microscopy/spectroscopy.
71         Here, electrical measurements by the scanning tunnelling microscopy (STM) break junction tech
72  to collect the required images in bulk, but scanning tunnelling microscopy (STM) could provide such
73 he -wave superconducting gap determined from scanning tunnelling microscopy (STM) for CeCoIn5, we con
74  and electronic properties at the nanoscale, scanning tunnelling microscopy (STM) has proven a very e
75 ablish a metrology combining low-temperature scanning tunnelling microscopy (STM) imaging and a compr
76                             In this study, a scanning tunnelling microscopy (STM) investigation with
77                                              Scanning tunnelling microscopy (STM) is an ideal techniq
78                     In this work, we present scanning tunnelling microscopy (STM) measurements of the
79                                              Scanning tunnelling microscopy (STM) measurements show t
80                                       We use scanning tunnelling microscopy (STM) to investigate a st
81                        Using low-temperature scanning tunnelling microscopy (STM) to measure an indiv
82  the high-resolution imaging capabilities of scanning tunnelling microscopy (STM).
83  universal cluster properties extracted from scanning tunnelling microscopy studies of cuprate superc
84    NEA+MP docking complexes are imaged using scanning tunnelling microscopy supplemented by density f
85                                              Scanning tunnelling microscopy, supported by electronic
86 ng the submolecular resolution capability of scanning tunnelling microscopy, supported by photoelectr
87                Here we show by spin-resolved scanning tunnelling microscopy that the spin direction a
88 e, using photoemission, X-ray scattering and scanning tunnelling microscopy, the canonical CDW compou
89 gstrom region of freestanding graphene using scanning tunnelling microscopy, thereby allowing measure
90 which we achieve by applying pressure with a scanning tunnelling microscopy tip.
91                                  Here we use scanning tunnelling microscopy to determine directly the
92 situ and measured them using high-resolution scanning tunnelling microscopy to determine picoscale ch
93                                  Here we use scanning tunnelling microscopy to determine the effects
94                                       We use scanning tunnelling microscopy to observe an orthorhombi
95 croscopy and molecular orbital imaging using scanning tunnelling microscopy to study more than 100 as
96                                  Here we use scanning tunnelling microscopy to study self-assembled m
97                                              Scanning tunnelling microscopy together with density fun
98 a angle-resolved photoemission spectroscopy, scanning tunnelling microscopy, transport studies, X-ray
99 ucture was characterized using bond-resolved scanning tunnelling microscopy, which enables chemical b
100 presents a fundamental advance in the use of scanning tunnelling microscopy, which together with the
101 gle crystal bcc Co30Fe70 nanoparticles using scanning tunnelling microscopy with a standard tungsten
102 u(n)O3(n+1) (n = 1, 2) using low-temperature scanning tunnelling microscopy, X-ray photoelectron spec
103          Here we show, through atom-resolved scanning tunnelling microscopy, X-ray spectroscopy and c

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