ライフサイエンスコーパス: adatom

1 omplex involves two PhS species and one gold adatom.

2 nd formation and partial oxidation of the Bi adatom.

3 anine molecules coordinating to a central Cu-adatom.

4 ites and dosed CO is found to bind to the Au adatom.

5 mble into surface-bonded complexes with gold adatoms.

6 structures is observed from the light-driven adatoms.

7 nts observe only the product associated with adatoms.

8 reatly shortening the diffusion distance for adatoms.

9 depending on the presence or absence of gold adatoms.

10 ecules connected by coordination bonds to Ag adatoms.

11 templated by the twofold coordination to Ag adatoms.

12 nced by specific substrates, intercalants or adatoms.

13 thus, their surfaces are covered with oxygen adatoms.

14 s water at rt, leaving a surface devoid of O adatoms.

15 e paramagnetic centres such as vacancies and adatoms.

16 e capping agent and the surface diffusion of adatoms.

17 uctures, comprising two molecules and six Au adatoms.

18 followed by galvanic displacement of the Cu adatoms.

19 solid/vapor and the solid/water interface, H adatom addition involves neutral H atom transfer hence t

20 be established on the basis of the nitrogen adatom adsorption energy (Delta E(N*)).

21 By imaging more than 70,000 single adatom adsorption sites, we compare the site preference

22 We directly image such individual adatoms, along with carbon chains and vacancies, and inv

23 An oxygen adatom and a vicinal Co-atom form a metal-oxygen site-pa

24 the bulk band gap are localised at specific (adatom and rest atom) sites on the reconstructed surface

25 ith an ensemble effect via the synergy of Co adatom and S of the D-1T MoS(2) support by tuning hydrog

26 cale changes, i.e. the creation of nanosized adatom and vacancy clusters.

27 ert substrates (e.g. alumina) are limited to adatoms and cations of Pt, Pd, and Ru.

28 in of the Majorana zero modes, from magnetic adatoms and external magnetic field, provides a new sing

29 atoms into metastable states, generating Cu adatoms and nanoclusters at mild cathodic potentials, wh

30 surface is lateral (surface) diffusion of O-adatoms and oxygen surface vacancies.

31 We consider specifically rings of adatoms and show that they allow for the creation, annih

32 how CO exposure affects the stability of Pt adatoms and subnano clusters at the Fe3O4(001) surface,

33 tude stronger compared with that between the adatoms and the hBN substrate.

34 drogenation, unveiling the catalytic role of adatoms and their effect on regioselectivity.

35 The formation energies of vacancies, adatoms and topological defects are discussed.

36 ents involving in situ deposition of surface adatoms, and complimentary modeling, we examine the elec

37 H atoms and, below a threshold potential, Cu adatoms are formed on the surface in a (4x4) superstruct

38 The Au adatoms are found to cap the under-coordinated oxygen si

39 Notably, residual O adatoms are not required for photochemical production of

40 These adatoms are observed using scanning tunneling microscopy

41 ect on the CO oxidation reaction when oxygen adatoms are preadsorbed.

42 At the lower coverage, only sulfur adatoms are present.

43 y intriguing properties; for example iridium adatoms are proposed to induce a substantial topological

44 Such adatoms are shown to be storable in ambient conditions f

45 k above the Fermi level is observed after Gd adatoms are trapped inside Fe corrals, while two peaks a

46 ine electronic waves by carefully positioned adatoms at clean metallic surfaces, we demonstrate an ap

47 been possible to determine which has faster adatom attachment kinetics.

48 ed strain field is generated that alters the adatom binding energy and, in turn, leads to a kinetic i

49 chiral domains even when R is achiral, while adatom binding leads to rectangular plane groups that su

50 ts the pitting intrinsically associated with adatom binding, desirably producing more regularly struc

51 provides information about the energetics of adatom binding, localized conduction channels, molecular

52 migration, vacancy-adatom recombination and adatom bistability.

53 d be assigned to the presence of single gold adatoms bonded by a coordination bond underneath the mol

54 he headgroup itself, whether it takes on the adatom-bound motif RS(*)Au(0)S(*)R or involves direct bi

55 tively on this surface leading to reactive O adatoms, but not on Au(111) or HOPG .

56 een carbon monoxide and a neighboring oxygen adatom by the tip.

57 Here, we image the potential over adatoms, chains, and clusters of Ag and Au atoms assembl

58 ols on the Au(111) surface is driven by gold adatom chemistry, which has recently been found to be th

59 By placing, with atomic precision, a copper adatom close to a porphycene molecule, we found that the

60 u-CO complex formation and diffusion, and Au adatom cluster formation on both elbows and step edges o

61 We also show that as the oxygen adatom coverage increases, the rate of CO oxidation decr

62 etric shell, and Al(14)I(y)(-), which has an adatom-decorated core.

63 he Majorana zero mode induced by magnetic Fe adatoms deposited on the surface.

64 these step-cation interactions via selective adatom deposition at the steps and by choosing an optima

65 cing the compound to be a dynamic process of adatom desorption and replacement.

66 th occurs on flat surfaces as a result of Cu adatoms detaching from steps and diffusing across terrac

67 led kinetically limited adatom funneling, as adatoms diffused asymmetrically along the vicinal facets

68 Adatom diffusion along steps is via hopping mechanism, a

69 et evolution in comparison with extracted Ga adatom diffusion lengths directly influences the vertica

70 Adatom diffusion on surface [Formula: see text] is high

71 These mechanisms include adatom diffusion on terraces, along steps, and around is

72 electric field can change normal stochastic adatom diffusion to biased diffusion, leading to selecti

73 ation, facilitated {100}-to-vicinal-to-{111} adatom diffusion.

74 first-principles calculations, including the adatom-diversified geometric structures, the Si- and C-d

75 es insight into role of support structure in adatom energetics, film nucleation, early-stage SEI morp

76 3 H2) depending on the nature of the present adatoms (Fe, Co, Ni or Cu).

77 oval shows that there is one additional gold adatom for every two octanethiol molecules on the surfac

78 ation, whereby numerous atomic vacancies and adatoms form.

79 that lead to cluster formation and show how adatom formation energies enable efficient screening of

80 atom-substrate exchange barriers separate Cu adatoms from a Cu-Au mixture, leaving behind a fluid pha

81 ll above 400 K are necessary to remove the O adatoms from the TiC(001) substrate by direct reaction w

82 tron microscopy revealed kinetically limited adatom funneling, as adatoms diffused asymmetrically alo

83 ed coordination centers were supplied by the adatom gas of the Cu(111) surface.

84 erials, such as gold, platinum, metal alloys/adatom, graphene, composites and glucose-specific organi

85 tive adsorption between nitrate and hydrogen adatoms (H*).

86 Starting from single adatoms hosting deep Shiba states, we use the highly ani

87 es adsorbed methyl (CH(3,ad)) plus an iodine adatom (I(ad)).

88 n of protecting groups or the elimination of adatoms in a gold-pentadecacene complex.

89 he site preference and dynamic motion of the adatoms in both a fully hydrated and a vacuum state.

90 Here we show that the magnetism of adatoms in graphene is itinerant and can be controlled b

91 detailed understanding of the role of metal adatoms in surface-molecule bonding and anchoring and of

92 istribution and higher diffusivities for the adatoms in the liquid phase compared with those in vacuu

93 on reaction forming water and surface oxygen adatoms, in line with experimental observations.

94 tructures through bond rotations and surface adatom incorporation.

95 ion barriers, because the basicity of oxygen adatoms increases with coverage and they become more eff

96 Although experiments have shown an adatom-induced enhancement of the electron-phonon coupli

97 ntation of assemblies with point defects and adatoms introduced at predetermined locations, and using

98 ol on Pt(111) to form methoxy and a hydrogen adatom is found to be uphill by +57 kJ/mol.

99 des modified by the incorporation of bismuth adatoms is revealed.

100 The spacing between Bi adatoms is such that peroxide association with two Bi ca

101 rences in the spatial distribution of oxygen adatoms; isolated adatoms lead to epoxidation, while isl

102 on rates, we demonstrate that on Cu(111) the adatom kinetics plays a decisive role in the expression

103 ial distribution of oxygen adatoms; isolated adatoms lead to epoxidation, while islands of "oxidic" o

104 )I(3)(-) the I induces an active site on the adatom, making the cluster reactive, explaining ligand-p

105 pon deposition, however, the adsorbed atoms (adatoms) may not stay at the same sites where the deposi

106 FT input regarding site binding energies and adatom migration barriers.

107 all bcc CuZn phase is more stable against Cu adatom migration than the fcc CuZn phase with the abilit

108 lso reveal defect dynamics, including oxygen adatom migration, vacancy-adatom recombination and adato

109 We established that the adatom mobility due to the heavy ion W(+) irradiation (i

110 yed resistive heating, to provide sufficient adatom mobility, in order to obtain high-quality dense f

111 se "picocavity" SERS spectra show that while adatom movement is significantly slower under low light

112 transport through the SEIs and fast lithium adatom movement on the substrate are essential for achie

113 ading to selective reduction of the nitrogen adatom (N*) to ammonium.

114 spectra from an optically generated metallic adatom near a molecule of interest can be inverted into

115 , we reveal that the primary factors are the adatom nucleation energies and the geometry of growth is

116 gaps, where they rapidly create ("write") an adatom on one facet surface.

117 ,10-dicyanoanthracene (DCA) molecules and Au adatoms on a Ag(111) surface at room temperature (RT).

118 Here we show that single oxygen adatoms on a boron monolayer (i.e., borophene) can be id

119 r to explore their ability to trap single Au adatoms on an Au(111) surface.

120 ns extremely small 'PdFe' clusters and metal adatoms on defective iron oxide to give the required met

121 ynamic equilibrium, where condensation of Ge adatoms on SiO2 is disfavored due to the extremely short

122 perations within their coherence time, while adatoms on surfaces probed by a scanning tunneling micro

123 The local effects of isolated magnetic adatoms on the electronic properties of the surface of a

124 atomic resolution, the dynamics of platinum adatoms on the monolayer in an aqueous salt solution.

125 ropose a set-up, based on chains of magnetic adatoms on the surface of a thin-film superconductor, in

126 , with alkanethiol molecules binding to gold adatoms on the surface.

127 X-ray photoelectron spectra show that Ti adatoms on the SWNT surface oxidize even under ultra-hig

128 s to systematically study the role of oxygen adatoms on the thermal transport in graphene oxide.

129 using a framework developed for friction of adatoms on various surfaces.

130 hydrogenation via interaction with an oxygen adatom or surface hydroxyl species to generate acrolein.

131 cohol is readily abstracted by either oxygen adatoms or adsorbed hydroxyl species on the gold surface

132 e transfer from a triboelectric probe to the adatom-organic coating complex.

133 dominated by surface diffusion of precursor adatoms over the nanowire walls, planar growth is domina

134 nding on the molecule, these light-extracted adatoms persist for minutes under ambient conditions.

135 partial redispersion and recovery of the Pt adatom phase.

136 phase CO molecules react readily with oxygen adatoms preadsorbed on Au/TiO(2)(110) to produce CO(2) e

137 ing induces considerable inward diffusion of adatoms, producing a distinct oxide morphology.

138 cally inert AFM tips terminated by an oxygen adatom provide excellent resolution of both the adsorbed

139 All O adatoms react thermally with methanol to form methoxy an

140 Differences between the adatom reactivities on copper and silver and the resulti

141 , including oxygen adatom migration, vacancy-adatom recombination and adatom bistability.

142 dation state for understanding molecular and adatom reconfiguration in optical nanocavities in respon

143 actions is undisputed, but the role of metal adatoms remains, to a large extent, unanswered, particul

144 ygen vacancies, cation vacancies, and cation adatoms, respectively.

145 les strongly indicates that the diffusion of adatoms results in a near thermodynamic equilibrium grow

146 of methyl- and phenylthiolate with the gold-adatom (RS-Au-SR, with R as the hydrocarbon group) under

147 th a stoichiometric CdSe core and surface Cd adatoms serving as binding sites for terminal S atoms of

148 raction energy between the ESR sensor and an adatom shows an inverse-cube distance dependence (r(-3.0

149 urface and bulk, with atomic steps acting as adatom sinks during heating and sources during cooling.

150 eduction conditions creates highly active Cu adatom sites not present on Cu(111).

151 s the Bi coverage becomes greater and the Bi adatom spacing becomes smaller, peroxide can adsorb on B

152 ocess is dictated by the inherent asymmetric adatom-substrate exchange barriers for separating dissim

153 We show that the disparity in the adatom-substrate exchange barriers separate Cu adatoms f

154 s three-dimensional clusters because of weak adatom-substrate interactions.

155 gh the decoration of graphene with an alkali adatom superlattice.

156 zing superconducting graphene by creating an adatom superlattice.

157 eps on Pt[410] help to stabilize the N and O adatoms that form upon dissociation and the transition s

158 ves, we are able to distinguish the fluorine adatoms that have bonded ionically to the graphite surfa

159 eaving behind a fluid phase enriched with Au adatoms that subsequently aggregate into supported clust

160 he NHC complex is added to the surface as an adatom, thereby precluding the need for reorganization o

161 In contrast, Ca adatoms thermally diffuse from such sites quickly, to se

162 t induces mobility among otherwise stable Pt adatoms through the formation of Pt carbonyls (Pt1-CO),

163 the much greater tendency for a diffusing Li adatom to remain locked in place once it reaches a terra

164 The thermal energy activates adatoms to aggregate resulting in the formation of self-

165 ng the substrate surface, which still enable adatoms to follow the atomic motif of the underlying sub

166 The insertion of atoms below the adatoms to form a dumbbell configuration involves extra

167 fer hence the reaction barriers for adding H adatoms to phenol are lowered by only 10-20 kJ/mol, due

168 he addition of the first and second hydrogen adatoms to three, ring carbon positions (ortho, meta, an

169 ereas the asymmetric interfacet diffusion of adatoms to {111} end-facets mediated longitudinal growth

170 ating the surface energetics and surface ion/adatom transport characteristics of the interphases form

171 ugh coadsorption of cyclic dialanine with Cu-adatoms under Ultra-High Vacuum (UHV) conditions.

172 scrambling between water and adsorbed oxygen adatoms upon heating the surface.

173 el that elucidates the need for fast lithium adatom velocity along the substrate that outpaces the cr

174 ingle-bond sensitivity of UHV-TERS to oxygen adatoms, we demonstrate the enhanced chemical stability

175 es recombine to generate water and an oxygen adatom, which subsequently dehydrogenates allyloxide.

176 this task because of its weak binding with H adatoms, which increases the selectivity and production

177 ped via coordination of homo- or heterometal adatoms, which may also play a role in the molecular tra

178 tional theory calculations to establish that adatoms will experience remote epitaxial registry with a

179 Here, by precisely positioning magnetic adatoms with a scanning tunneling microscope (STM), we d

180 free Yu-Shiba-Rusinov bound states at the Fe adatoms with a weaker coupling to the substrate, and dis

181 determine the magnetic moments of individual adatoms with high accuracy.