81 research outputs found

    Resolution in Focused Electron- and Ion-Beam Induced Chemical Vapor Deposition

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    The key physical processes governing resolution of focused electron-beam and ion-beam-assisted chemical vapor deposition are analyzed via an adsorption rate model. We quantify for the first time how the balance of molecule depletion and replenishment determines the resolution inside the locally irradiated area. Scaling laws are derived relating the resolution of the deposits to molecule dissociation, surface diffusion, adsorption, and desorption. Supporting results from deposition experiments with a copper metalorganic precursor gas on a silicon substrate are presented and discussed.Comment: 4 pages, 4 figures, 1 tabl

    Tailoring thin-film mechanical fragmentation properties of hybrid atomic/molecular-layer-deposited materials

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    Molecular layer deposition (MLD) as the little sister of atomic layer deposition is a strongly emerging thin-film technique for deposition of ultra-thin inorganic–organic hybrid (“metalcone”) coatings directly from the gas phase, even on complex three-dimensional surfaces. Employing tensile testing coupled with in situ optical microscopy, we found [1] that using inorganic metal oxide ALD alone could increase the crack onset strain via nanolaminating amorphous and nanocrystalline film layers, see fig. 1a. This behavior can be attributed to changing residual strains [2] in the overall Al2O3/Y2O3 nanolaminate film and shifted the crack onset strain from 0.67% to 1.1% (and decreased the crack density by a factor 2). However, introducing organic carbon backbones into the inorganic oxide material allows increasing the crack onset strain by an order of magnitude. Please click Download on the upper right corner to see the full abstract

    A novel copper precursor for electron beam induced deposition

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    A fluorine free copper precursor, Cu(tbaoac)2 with the chemical sum formula CuC16O6H26 is introduced for focused electron beam induced deposition (FEBID). FEBID with 15 keV and 7 nA results in deposits with an atomic composition of Cu:O:C of approximately 1:1:2. Transmission electron microscopy proved that pure copper nanocrystals with sizes of up to around 15 nm were dispersed inside the carbonaceous matrix. Raman investigations revealed a high degree of amorphization of the carbonaceous matrix and showed hints for partial copper oxidation taking place selectively on the surfaces of the deposits. Optical transmission/reflection measurements of deposited pads showed a dielectric behavior of the material in the optical spectral range. The general behavior of the permittivity could be described by applying the Maxwell–Garnett mixing model to amorphous carbon and copper. The dielectric function measured from deposited pads was used to simulate the optical response of tip arrays fabricated out of the same precursor and showed good agreement with measurements. This paves the way for future plasmonic applications with copper-FEBID

    Nano-Hall sensors with granular Co-C

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    We analyzed the performance of Hall sensors with different Co-C ratios, deposited directly in nano-structured form, using Co2(CO)8Co_2(CO)_8 gas molecules, by focused electron or ion beam induced deposition. Due to the enhanced inter-grain scattering in these granular wires, the Extraordinary Hall Effect can be increased by two orders of magnitude with respect to pure Co, up to a current sensitivity of 1Ω/T1 \Omega/T. We show that the best magnetic field resolution at room temperature is obtained for Co ratios between 60% and 70% and is better than 1ÎŒT/Hz1/21 \mu T/Hz^{1/2}. For an active area of the sensor of 200×200nm2200 \times 200 nm^2, the room temperature magnetic flux resolution is ϕmin=2×10−5ϕ0\phi_{min} = 2\times10^{-5}\phi_0, in the thermal noise frequency range, i.e. above 100 kHz.Comment: 5 pages, 4 figure

    Lateral resolution in focused electron beam-induced deposition: scaling laws for pulsed and static exposure

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    In this work, we review the single-adsorbate time-dependent continuum model for focused electron beam-induced deposition (FEBID). The differential equation for the adsorption rate will be expressed by dimensionless parameters describing the contributions of adsorption, desorption, dissociation, and the surface diffusion of the precursor adsorbates. The contributions are individually presented in order to elucidate their influence during variations in the electron beam exposure time. The findings are condensed into three new scaling laws for pulsed exposure FEBID (or FEB-induced etching) relating the lateral resolution of deposits or etch pits to surface diffusion and electron beam exposure dwell time for a given adsorbate depletion state
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