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“…The absence of the RuO 2 peaks (expected 0.65 eV higher relatively to the position of the Ru3d 5/2 peak 26 ) in XPS data is in agreement with the XRD spectra (Fig. 4) that are devoid of any RuO 2 phase (in agreement to the XRD data published by Leick et al 2 ). The C1s peak position due to the residual carbon was deconvoluted in the 284-285 eV range, to account for CO and CH x species that constitute the Ru precursor.…”
Section: B Composition and Thicknesssupporting
confidence: 91%
“…Substituting the values of w p and C d from Table I in Eqs. (2) and 3, the Drude-derived resistivity of the Ru islands can be calculated. Using these data along with the fraction f 1 of the Ruthenium phase (f Ru top ; tabulated in Table II) as an input into the Landauer model Eq.…”
Section: Sheet Resistancementioning
confidence: 99%
“…ALD deposition of Ru had been recently explored using a variety of precursors and reactants. [1][2][3] The interest in Ru deposition arises from its high work function, low bulk resistivity, and ability to form stable conductive oxides. In this manuscript, we investigate the electrical characteristics (conductivity) of ultra-thin Ru films on H-passivated Si surfaces as a function of the number of Ru ALD cycles.…”
The sheet resistance measured by a four-probe technique is compared to the resistivity data derived from the optical response of thin ruthenium films grown on hydrogen-passivated Si(111) surfaces by atomic-layer deposition using cyclopentadienyl ethylruthenium dicarbonyl, Ru(Cp)(CO) 2 Et and O 2 as gas reactant. The Drude-Landauer theory is applied to evaluate the spectroscopic ellipsometry response and the DC resistivity evaluated by 4-point probe measurements. Results indicate that thin Ru films (below $5 nm) deposited on Si exhibit a higher sheet resistance than similarly grown Ru films on TiN. This is explained by an island-growth mechanism at the initial stages of Ru deposition that greatly diminishes the film conductivity before the formation of a continuous film. V
“…The absence of the RuO 2 peaks (expected 0.65 eV higher relatively to the position of the Ru3d 5/2 peak 26 ) in XPS data is in agreement with the XRD spectra (Fig. 4) that are devoid of any RuO 2 phase (in agreement to the XRD data published by Leick et al 2 ). The C1s peak position due to the residual carbon was deconvoluted in the 284-285 eV range, to account for CO and CH x species that constitute the Ru precursor.…”
Section: B Composition and Thicknesssupporting
confidence: 91%
“…Substituting the values of w p and C d from Table I in Eqs. (2) and 3, the Drude-derived resistivity of the Ru islands can be calculated. Using these data along with the fraction f 1 of the Ruthenium phase (f Ru top ; tabulated in Table II) as an input into the Landauer model Eq.…”
Section: Sheet Resistancementioning
confidence: 99%
“…ALD deposition of Ru had been recently explored using a variety of precursors and reactants. [1][2][3] The interest in Ru deposition arises from its high work function, low bulk resistivity, and ability to form stable conductive oxides. In this manuscript, we investigate the electrical characteristics (conductivity) of ultra-thin Ru films on H-passivated Si surfaces as a function of the number of Ru ALD cycles.…”
The sheet resistance measured by a four-probe technique is compared to the resistivity data derived from the optical response of thin ruthenium films grown on hydrogen-passivated Si(111) surfaces by atomic-layer deposition using cyclopentadienyl ethylruthenium dicarbonyl, Ru(Cp)(CO) 2 Et and O 2 as gas reactant. The Drude-Landauer theory is applied to evaluate the spectroscopic ellipsometry response and the DC resistivity evaluated by 4-point probe measurements. Results indicate that thin Ru films (below $5 nm) deposited on Si exhibit a higher sheet resistance than similarly grown Ru films on TiN. This is explained by an island-growth mechanism at the initial stages of Ru deposition that greatly diminishes the film conductivity before the formation of a continuous film. V
“…4 Other Ru precursors such as Ru(EtCp)2 and CpRu(CO)2Et have also been developed. 34,35 Generally, the deposition temperature is above 200 °C for these metal organic precursors. 36,37 As pointed out earlier, oxygen can oxidize metal surface and use of N-plasma is therefore important for the deposition of metals.…”
<div>In the atomic layer deposition (ALD) of Cobalt (Co) and Ruthenium (Ru) metal using nitrogen plasma, the structure and composition of the post N-plasma NHx terminated (x = 1 or 2) metal surfaces are not well known but are important in the subsequent metal containing pulse. In this paper, we use the low-index (001) and (100) surfaces of Co and Ru as models of the metal polycrystalline thin films. The (001) surface with a hexagonal surface structure is the most stable surface and the (100) surface with a zigzag structure is the least stable surface but has high reactivity. We investigate the stability of NH and NH2 terminations on these surfaces to determine the saturation coverage of NHx on Co and Ru. NH is most stable in the hollow hcp site on (001) surface and the bridge site on the (100) surface, while NH2 prefers the bridge site on both (001) and (100) surfaces. The differential energy is calculated to find the saturation coverage of NH and NH2. We also present results on mixed NH/NH2-terminations. The results are analyzed by thermodynamics using Gibbs free energies (ΔG) to reveal temperature effects on the stability of NH and NH2 terminations. Ultra-high vacuum (UHV) and standard ALD</div><div>operating conditions are considered. Under typical ALD operating conditions we find that the most stable NHx terminated metal surfaces are 1 ML NH on Ru (001) surface (350K-550K), 5/9 ML NH on Co (001) surface (400K-650K) and a mixture of NH and NH2 on both Ru (100) and Co (100) surfaces.</div>
“…Initially, the reaction mechanisms were mainly studied by identifying the reaction products formed during the process. By using mass spectrometry, Aaltonen et al established for Ru and Pt that CO 2 and H 2 O are formed during both ALD half-reactions as the main reactions products, implying that combustion-like reactions play a dominant role (13). By gas-phase infrared spectroscopy, and later also by mass-spectrometry (15,19), it was observed for Pt ALD that CH 4 is also formed during the MeCpPtMe 3 pulse (14), which revealed a concurrent reaction pathway in addition to ligand combustion.…”
Atomic layer deposition (ALD) of noble metals has attracted much attention in recent years for the deposition of thin metal films, as well as for the synthesis of supported metallic nanoparticles. Noble metal surfaces and nanoparticles possess catalytic activity for dissociation of metalorganic precursor and O 2 molecules, which has important consequences for the reaction mechanisms of ALD. In this work, a case study is presented with respect to the importance of catalytic surface reactions during the nucleation and growth of Pt ALD, which serves as a model system for the growth of other noble metals by ALD. It is illustrated that atomic level understanding of these processes is vital for the development of novel nanopatterning and nanoparticle synthesis approaches.
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