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1 rogenating borophene with atomic hydrogen in ultrahigh vacuum.
2 111) homoepitaxial growth and ion erosion in ultrahigh vacuum.
3 tless X-ray photoelectron spectroscopy under ultrahigh vacuum.
4 njugated covalent networks on surfaces under ultrahigh vacuum.
5 n etching of epitaxial graphene/SiC(0001) in ultrahigh vacuum.
6 on of monolayers from the gas phase under an ultrahigh vacuum.
7 ted Pt(n)(+) (n </= 11) on GCE substrates in ultrahigh vacuum.
8 ng epitaxial graphene using atomic oxygen in ultrahigh vacuum.
9 grow on SiC crystals at high temperatures in ultrahigh vacuum.
10 a film formed on a Mo(100) single crystal in ultrahigh vacuum.
11 h vapor deposition onto graphite surfaces in ultrahigh vacuum.
12  amorphous, polycrystalline or exist only in ultrahigh vacuum.
13 en a Co and Fe center, while cycling between ultrahigh vacuum and 2 mbar of water at constant tempera
14 ature-programmed desorption (TPD) both under ultrahigh vacuum and in situ from liquid solutions.
15  which restricts their operation pressure to ultrahigh vacuums and leads to a short lifetime and low
16 ion at the nano/atomic scale from ambient to ultrahigh-vacuum and electrochemical environments.
17 e science studies of crystalline surfaces in ultrahigh vacuum, and first-principles modeling using de
18 phyrins were first prepared on Au(111) under ultrahigh vacuum, and hydrogen atoms were then removed f
19 by X-ray photoelectron spectroscopy (XPS) in ultrahigh vacuum at room temperature.
20 roximately 1 muC.cm(-2), and is preserved in ultrahigh vacuum, but disappears upon heating to 100 deg
21 transform mass spectrometers operating under ultrahigh vacuum, but exceptional m/ z resolution and ac
22  epitaxial monolayer graphene was studied in ultrahigh vacuum by low-temperature scanning tunneling m
23 iation of surface phenoxides was measured in ultrahigh vacuum by X-ray photoelectron spectroscopy, as
24                              Here, combining ultrahigh vacuum catalytic experiments, X-ray photoemiss
25 e interferometer near a spherical mass in an ultrahigh-vacuum chamber, we reduced the screening mecha
26 dgap dielectric crystals, investigated under ultrahigh vacuum conditions at room temperature, is revi
27  in few A to 5 nm gap sizes, performed under ultrahigh vacuum conditions between a Au-coated probe fe
28                        Need of substrate and ultrahigh vacuum conditions for deposition of borophene
29 erface, which can be retrieved neither under ultrahigh vacuum conditions nor from interfaces immersed
30 n synthesized on a noble metal surface under ultrahigh vacuum conditions via a gas-mediated surface r
31 he (111) surfaces of copper and silver under ultrahigh vacuum conditions were studied by scanning tun
32 an azide can be performed under solvent-free ultrahigh vacuum conditions with reactants adsorbed on a
33 ented because the use of soft X-rays implies ultrahigh vacuum conditions.
34 olecular, nanoscale spatial resolution under ultrahigh vacuum conditions.
35 d by using a collimated molecular beam under ultrahigh vacuum conditions.
36 ingle-layer graphene crystals examined under ultrahigh vacuum conditions.
37                        Performing TERS under ultrahigh-vacuum conditions allows pristine and atomical
38  electron density when imaged with STM under ultrahigh-vacuum conditions at 77 K.
39 sis of actinide tetrapyrrole complexes under ultrahigh-vacuum conditions, on both a metallic support
40                                        Under ultrahigh-vacuum conditions, physical vapor deposition a
41 t is, deep within water's "no man's land" in ultrahigh-vacuum conditions.
42 s (i.e., borophene) on silver surfaces under ultrahigh-vacuum conditions.
43 ligomers directly on a Ag(111) support under ultrahigh-vacuum conditions.
44 is used to image these species at 77 K under ultrahigh-vacuum conditions.
45              This pathway, operational in an ultrahigh vacuum environment at moderate temperature is
46 y incompatibility of the liquid samples with ultrahigh vacuum environment of the electron optics and
47 dehydrogenative porphyrin homocoupling in an ultrahigh vacuum environment provides access to surface-
48 rves cell morphology, allows analysis in the ultrahigh vacuum environment, and reduces topographic ar
49 sorbed on several noble metal surfaces in an ultrahigh vacuum environment.
50 ponents self-assembly on solid surface in an ultrahigh vacuum environment.
51 in derivatives (2H-TPCN) with Co atoms in an ultrahigh vacuum environment.
52  work on size-selected supported clusters in ultrahigh-vacuum environments and under realistic reacti
53 ften ignored in theoretical and even in some ultrahigh vacuum experimental studies.
54 he PdO(101) surface as determined from model ultrahigh vacuum experiments and theoretical calculation
55                   The films are stable under ultrahigh vacuum for at least 17 h but show onset of dec
56                   The films are stable under ultrahigh vacuum for at least 60 h but show signs of dec
57       A lead nanocrystal was crystallized in ultrahigh vacuum from a droplet on a silica substrate an
58                  Various substrate-supported ultrahigh-vacuum growth techniques for borophene, such a
59          Analytic results and experiments in ultrahigh vacuum indicate that the static friction betwe
60                             Here, we combine ultrahigh-vacuum irradiation experiments with comprehens
61 ever the quality of the graphene produced in ultrahigh vacuum is poor due to the high sublimation rat
62                Surface Raman spectroscopy in ultrahigh vacuum is used to interrogate interfaces forme
63 ced by a controlled temperature annealing in ultrahigh vacuum, is presented.
64 tering, even though the instrument was under ultrahigh vacuum (&lt;5 x 10(-7) Pa).
65 nd electrical properties analyzed in situ by ultrahigh-vacuum, multiple mode atomic force microscopy
66  methane and carbon dioxide-water mixture in ultrahigh vacuum of the order of 10(-10) mbar for extend
67 of submonolayer quantities of corannulene in ultrahigh vacuum onto thick Cs films, deposited at 100 K
68                              In this manner, ultrahigh-vacuum oxidation overcomes the limitations of
69 d to density functional theory, showing that ultrahigh-vacuum oxidization results in uniform epoxy fu
70 in-film growth mechanisms of aluminum during ultrahigh vacuum physical vapor deposition, dense arrays
71 d to ionize neutral organic molecules in the ultrahigh-vacuum region of a Fourier transform ion cyclo
72 n is triggered by ultraviolet irradiation in ultrahigh vacuum, requiring no aid of the graphene Moire
73                                 Annealing in ultrahigh vacuum revealed a thermal stability limit of a
74                                     Using an ultrahigh vacuum scanning tunneling microscope (STM), we
75  is induced and investigated using cryogenic ultrahigh vacuum scanning tunneling microscopy (STM).
76 face and investigated using room temperature ultrahigh vacuum scanning tunneling microscopy.
77 semiconductor nanostructures with the use of ultrahigh-vacuum scanning thermoelectric microscopy.
78                                           An ultrahigh-vacuum scanning tunneling microscope was used
79 ce of gold was discovered with the use of an ultrahigh-vacuum scanning tunneling microscope.
80 ecisely controllable junction of a cryogenic ultrahigh-vacuum scanning tunnelling microscope(14-16),
81 density functional theory calculations in an ultrahigh vacuum setting show that, with the oxide coati
82 t preparation by infrared laser pumping, and ultrahigh vacuum surface analysis techniques make it pos
83                                        While ultrahigh vacuum surface science techniques have provide
84 aces that are not accessible in conventional ultrahigh-vacuum surface-science experiments.
85 ayers of quality similar to that obtained by ultrahigh vacuum techniques at elevated temperature.
86  sugars, such as glucose and fructose, using ultrahigh vacuum techniques.
87 ore sensitive to UV, ionizing radiation, and ultrahigh vacuum than wild-type spores, indicating that
88  borophene) can be identified and mapped via ultrahigh vacuum tip-enhanced Raman spectroscopy (UHV-TE
89 mical characterization of BL borophene using ultrahigh vacuum tip-enhanced Raman spectroscopy (UHV-TE
90                                              Ultrahigh vacuum tip-enhanced Raman spectroscopy (UHV-TE
91 angstrom-scale interfacial interactions with ultrahigh-vacuum tip-enhanced Raman spectroscopy (UHV-TE
92 us exposure of Cot molecules and Eu vapor in ultrahigh vacuum to an inert substrate, such as graphene
93  is thermally robust and is evaporated under ultrahigh vacuum to form thin films of intact diradicals
94             Triradical 3 is evaporated under ultrahigh vacuum to form thin films of intact triradical
95 on single crystalline surfaces of titania in ultrahigh vacuum to investigate the unusual size depende
96  microfabricated device, we conduct in situ, ultrahigh vacuum transmission electron microscope measur
97 ructures have been investigated in real-time ultrahigh vacuum transmission electron microscopy (UHV-T
98  gas-phase, research with model catalysts in ultrahigh vacuum (UHV) and so-called high-pressure cell
99  tens of nanometer large nanoparticles under ultrahigh vacuum (UHV) as well as high vacuum (HV) condi
100 However, room temperature (RT) combined with ultrahigh vacuum (UHV) can induce major SEI evolution fr
101 he ion source from impacting the surface, an ultrahigh vacuum (UHV) chamber for ion deposition by sof
102 gle-crystal surfaces was characterized under ultrahigh vacuum (UHV) conditions by using temperature p
103 e that 2D core-shell surfaces prepared under ultrahigh vacuum (UHV) conditions constitute excellent m
104 nanometer-thin films on insulators and under ultrahigh vacuum (UHV) conditions from photocoupled brom
105 on induced decomposition of adsorbed 1 under ultrahigh vacuum (UHV) conditions proceeds through initi
106 curs on Au(111) upon thermal annealing under ultrahigh vacuum (UHV) conditions.
107 ee-base TPP layer on a Ag(100) surface under ultrahigh vacuum (UHV) conditions.
108 ecular beam reactive scattering (MBRS) under ultrahigh vacuum (UHV) conditions.
109                Radical 1 is evaporated under ultrahigh vacuum (UHV) forming assemblies of intact radi
110 stem used for the deposition of molecules in ultrahigh vacuum (UHV) is presented, along with encourag
111 er absorbed on a rutile TiO2(110) surface in ultrahigh vacuum (UHV) is studied with spin-polarized de
112  the FAIMS stage complicates maintaining the ultrahigh vacuum (UHV) needed for Orbitrap operation.
113 ocyanine (CuPc) monolayers is observed using ultrahigh vacuum (UHV) scanning tunneling microscopy (ST
114                                        Using ultrahigh vacuum (UHV) scanning tunneling microscopy (ST
115 tial surface characterization was done in an ultrahigh vacuum (UHV) system, and depending on preparat
116                                           In ultrahigh vacuum (UHV) the clean-annealed surface produc
117                                           In ultrahigh vacuum (UHV), TERS can be performed in pristin
118 nt were previously observed in dry DNA under ultrahigh vacuum (UHV), while hydrated electrons were fo
119 om those found at room temperature and under ultrahigh vacuum (UHV).
120 bly of 10,12-pentacosadiynoic acid (PCDA) in ultrahigh vacuum (UHV).
121 aces accessed through sample delamination in ultrahigh vacuum (UHV).
122  were deposited on clean Pt(111) surfaces in ultrahigh vacuum (UHV).
123 alternative to cryogenics for SIMS and other ultrahigh-vacuum (UHV) analyses of biological species.
124 d single-crystalline supports prepared in an ultrahigh-vacuum (UHV) environment.
125 clusters are fairly stable upon annealing in ultrahigh vacuum up to 600 K, increasing the temperature
126 om solution onto a Au(111) substrate held in ultrahigh vacuum using electrospray deposition (UHV-ESD)
127 3)2]5 and Ti[N(CH3)2]4 have been examined in ultrahigh vacuum using X-ray photoelectron spectroscopy.
128 re resistance to UV, ionizing radiation, and ultrahigh vacuum was studied in wild-type and DNA repair
129 onal Pt monolayer grown by Pt evaporation in ultrahigh vacuum, we observe a significant destabilizati
130 dine films are reacted with Ca at 30 K under ultrahigh vacuum with the reaction progress monitored by

 
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