ライフサイエンスコーパス: adatom

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

2 omplex involves two PhS species and one gold adatom.

3 nd formation and partial oxidation of the Bi adatom.

4 ecules connected by coordination bonds to Ag adatoms.

5 templated by the twofold coordination to Ag adatoms.

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

7 e paramagnetic centres such as vacancies and adatoms.

8 e capping agent and the surface diffusion of adatoms.

9 uctures, comprising two molecules and six Au adatoms.

10 followed by galvanic displacement of the Cu adatoms.

11 nced by specific substrates, intercalants or adatoms.

12 mble into surface-bonded complexes with gold adatoms.

13 thus, their surfaces are covered with oxygen adatoms.

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

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

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

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

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

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

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

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

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

23 These adatoms are observed using scanning tunneling microscopy

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

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

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

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

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

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

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

31 migration, vacancy-adatom recombination and adatom bistability.

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

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

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

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

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

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

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

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

40 Adatom diffusion along steps is via hopping mechanism, a

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

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

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

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

45 3 H2) depending on the nature of the present adatoms (Fe, Co, Ni or Cu).

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

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

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

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

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

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

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

53 tructures through bond rotations and surface adatom incorporation.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

81 partial redispersion and recovery of the Pt adatom phase.

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

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

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

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

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

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

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

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

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

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

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

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

94 zing superconducting graphene by creating an adatom superlattice.

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

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

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

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

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

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

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

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

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

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

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

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

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