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  • 1
    In: Journal of Vacuum Science & Technology A: Vacuum, Surfaces, and Films, American Vacuum Society, Vol. 38, No. 3 ( 2020-05-01)
    Abstract: Experimentally measured resistivity of Co(0001) and Ru(0001) single crystal thin films, grown on c-plane sapphire substrates, as a function of thickness is modeled using the semiclassical model of Fuchs–Sondheimer. The model fits show that the resistivity of Ru would cross below that for Co at a thickness of approximately 20 nm. For Ru films with thicknesses above 20 nm, transmission electron microscopy evidences threading and misfit dislocations, stacking faults, and deformation twins. Exposure of Co films to ambient air and the deposition of oxide layers of SiO2, MgO, Al2O3, and Cr2O3 on Ru degrade the surface specularity of the metallic layer. However, for the Ru films, annealing in a reducing ambient restores the surface specularity. Epitaxial electrochemical deposition of Co on epitaxially deposited Ru layers is used as an example to demonstrate the feasibility of generating epitaxial interconnects for back-end-of-line structures. An electron transport model based on a tight-binding approach is described, with Ru interconnects used as an example. The model allows conductivity to be computed for structures comprising large ensembles of atoms (105–106), scales linearly with system size, and can also incorporate defects.
    Type of Medium: Online Resource
    ISSN: 0734-2101 , 1520-8559
    RVK:
    Language: English
    Publisher: American Vacuum Society
    Publication Date: 2020
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    detail.hit.zdb_id: 797704-9
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  • 2
    Online Resource
    Online Resource
    Institute of Electrical and Electronics Engineers (IEEE) ; 2021
    In:  IEEE Transactions on Electron Devices Vol. 68, No. 1 ( 2021-1), p. 257-263
    In: IEEE Transactions on Electron Devices, Institute of Electrical and Electronics Engineers (IEEE), Vol. 68, No. 1 ( 2021-1), p. 257-263
    Type of Medium: Online Resource
    ISSN: 0018-9383 , 1557-9646
    Language: Unknown
    Publisher: Institute of Electrical and Electronics Engineers (IEEE)
    Publication Date: 2021
    detail.hit.zdb_id: 2028088-9
    detail.hit.zdb_id: 241634-7
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  • 3
    Online Resource
    Online Resource
    Institute of Electrical and Electronics Engineers (IEEE) ; 2022
    In:  IEEE Transactions on Electron Devices Vol. 69, No. 7 ( 2022-7), p. 3854-3860
    In: IEEE Transactions on Electron Devices, Institute of Electrical and Electronics Engineers (IEEE), Vol. 69, No. 7 ( 2022-7), p. 3854-3860
    Type of Medium: Online Resource
    ISSN: 0018-9383 , 1557-9646
    Language: Unknown
    Publisher: Institute of Electrical and Electronics Engineers (IEEE)
    Publication Date: 2022
    detail.hit.zdb_id: 2028088-9
    detail.hit.zdb_id: 241634-7
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  • 4
    In: Advanced Functional Materials, Wiley, Vol. 32, No. 45 ( 2022-11)
    Abstract: High aspect ratio metal nanostructures are commonly found in a broad range of applications such as electronic compute structures and sensing. The self‐heating and elevated temperatures in these structures, however, pose a significant bottleneck to both the reliability and clock frequencies of modern electronic devices. Any notable progress in energy efficiency and speed requires fundamental and tunable thermal transport mechanisms in nanostructured metals. In this work, time‐domain thermoreflectance is used to expose cross‐plane quasi‐ballistic transport in epitaxially grown metallic Ir(001) interposed between Al and MgO(001). Thermal conductivities ranges from roughly 65 (96 in‐plane) to 119 (122 in‐plane) W m −1 K −1 for 25.5–133.0 nm films, respectively. Further, low defects afforded by epitaxial growth are suspected to allow the observation of electron–phonon coupling effects in sub‐20 nm metals with traditionally electron‐mediated thermal transport. Via combined electro‐thermal measurements and phenomenological modeling, the transition is revealed between three modes of cross‐plane heat conduction across different thicknesses and an interplay among them: electron dominant, phonon dominant, and electron–phonon energy conversion dominant. The results substantiate unexplored modes of heat transport in nanostructured metals, the insights of which can be used to develop electro‐thermal solutions for a host of modern microelectronic devices and sensing structures.
    Type of Medium: Online Resource
    ISSN: 1616-301X , 1616-3028
    URL: Issue
    Language: English
    Publisher: Wiley
    Publication Date: 2022
    detail.hit.zdb_id: 2029061-5
    detail.hit.zdb_id: 2039420-2
    SSG: 11
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  • 5
    Online Resource
    Online Resource
    MDPI AG ; 2023
    In:  Nanomaterials Vol. 13, No. 6 ( 2023-03-07), p. 957-
    In: Nanomaterials, MDPI AG, Vol. 13, No. 6 ( 2023-03-07), p. 957-
    Abstract: Mo(001) and Mo(011) layers with thickness d = 4–400 nm are sputter-deposited onto MgO(001) and α-Al2O3(112¯0) substrates and their resistivity is measured in situ and ex situ at room temperature and 77 K in order to quantify the resistivity size effect. Both Mo(001) and Mo(011) layers are epitaxial single crystals and exhibit a resistivity increase with decreasing d due to electron surface scattering that is well described by the classical Fuchs and Sondheimer model. Data fitting yields room temperature effective electron mean free paths λ*= 14.4 ± 0.3 and 11.7 ± 0.3 nm, respectively, indicating an anisotropy with a smaller resistivity size effect for the Mo(011) orientation. This is attributed to a smaller average Fermi velocity component perpendicular to (011) surfaces, causing less surface scattering and a suppressed resistivity size effect. First-principles electronic structure calculations in combination with Boltzmann transport simulations predict an orientation dependent transport with a more pronounced resistivity increase for Mo(001) than Mo(011). This is in agreement with the measurements, confirming the effect of the Fermi surface shape on the thin-film resistivity. The predicted anisotropy λ001*/λ011* = 1.57 is in reasonable agreement with 1.66 and 1.23 measured at 77 and 295 K. The overall results indicate that the resistivity size effect in Mo is relatively small, with a measured product of the bulk resistivity times the effective electron mean free path ρoλ* = (7.7 ± 0.3) and (6.2 ± 0.2) × 10−16 Ωm2 for Mo(001) and Mo(011) layers. The latter value is in excellent agreement with the first-principles-predicted ρoλ = 5.99 × 10−16 Ωm2 and is 10% and 40% smaller than the reported measured ρoλ for Cu and W, respectively, indicating the promise of Mo as an alternate conductor for narrow interconnects.
    Type of Medium: Online Resource
    ISSN: 2079-4991
    Language: English
    Publisher: MDPI AG
    Publication Date: 2023
    detail.hit.zdb_id: 2662255-5
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  • 6
    Online Resource
    Online Resource
    American Physical Society (APS) ; 2018
    In:  Physical Review Letters Vol. 121, No. 23 ( 2018-12-7)
    In: Physical Review Letters, American Physical Society (APS), Vol. 121, No. 23 ( 2018-12-7)
    Type of Medium: Online Resource
    ISSN: 0031-9007 , 1079-7114
    RVK:
    RVK:
    Language: English
    Publisher: American Physical Society (APS)
    Publication Date: 2018
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    detail.hit.zdb_id: 208853-8
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  • 7
    Online Resource
    Online Resource
    AIP Publishing ; 2022
    In:  Applied Physics Letters Vol. 120, No. 4 ( 2022-01-24)
    In: Applied Physics Letters, AIP Publishing, Vol. 120, No. 4 ( 2022-01-24)
    Abstract: In situ transport measurements on 10-nm-thick epitaxial Cu(001), Co(001), and Rh(001) layers exhibit a characteristic increase in the sheet resistance ΔRs/Ro = 43%, 10%, and 4% when adding 4.0, 13.0, and 13.0 monolayers of Ti, respectively. Similarly, exposing these layers to 0.6 Torr O2 results in a 26%, 22%, and & lt;5% increase in Rs. This suggests that adatoms on Cu and Co surfaces considerably disturb the surface potential, leading to diffuse electron scattering and a resulting resistance increase while these effects are negligible for Rh. A similarly small resistivity increase Δρ/ρ & lt; 7% is measured during air exposure of 10-nm-thick epitaxial layers of electronegative metals including Ru, Rh, Ir, W, and Mo, while Δρ/ρ increases to 11%–36% for more electropositive metals including Cu, Ag, Co, Ni, and Nb. The Δρ for Ni, Co, and Nb is larger than what is expected for a complete transition from specular to diffuse surface scattering, indicating a breakdown of the semiclassical Fuchs–Sondheimer model, which needs to be replaced by a two-dimensional conductor description. The measured inverse correlation between electronegativity and Δρ/ρ suggests that the magnitude of the surface potential perturbation is the primary parameter affecting electron surface scattering in thin metal layers. More specifically, the charge transfer from electropositive metal surfaces to adatoms perturbs the surface potential and causes electron surface scattering and a resistance increase. Conversely, electronegative metals facilitate smooth surface potentials with specular electron reflection and a minimized resistance increase. They are, therefore, promising as conductors for highly scaled interconnect lines.
    Type of Medium: Online Resource
    ISSN: 0003-6951 , 1077-3118
    RVK:
    Language: English
    Publisher: AIP Publishing
    Publication Date: 2022
    detail.hit.zdb_id: 211245-0
    detail.hit.zdb_id: 1469436-0
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  • 8
    Online Resource
    Online Resource
    AIP Publishing ; 2022
    In:  Applied Physics Letters Vol. 120, No. 24 ( 2022-06-13)
    In: Applied Physics Letters, AIP Publishing, Vol. 120, No. 24 ( 2022-06-13)
    Abstract: The electron reflection probability r at symmetric twin boundaries Σ3, Σ5, Σ9, and Σ11 is predicted from first principles for the eight most conductive face-centered cubic (fcc) metals. r increases with decreasing interplanar distance of atomic planes parallel to the boundary. This provides the basis for an extrapolation scheme to estimate the reflection probability rr at random grain boundaries, which is relatively small, rr = 0.28–0.39, for Cu, Ag, and Au due to their nearly spherical Fermi surfaces, but approximately two times higher for Al, Ca, Ni, Rh, and Ir with a predicted rr = 0.61–0.72. The metal resistivity in the limit of small randomly oriented grains with fixed average size is expected to be proportional to the materials benchmark quantity ρoλ × rr/(1 − rr), where ρo and λ are the bulk resistivity and bulk electron mean free path, respectively. Cu has the lowest value for this quantity, indicating that all other fcc metals have a higher resistivity in the limit of small randomly oriented grains. Thus, the conductivity benefit of replacement metals for narrow Cu interconnect lines can only be realized if the grains are larger than the linewidth or exhibit symmetric orientation relationships where r & lt; rr.
    Type of Medium: Online Resource
    ISSN: 0003-6951 , 1077-3118
    RVK:
    Language: English
    Publisher: AIP Publishing
    Publication Date: 2022
    detail.hit.zdb_id: 211245-0
    detail.hit.zdb_id: 1469436-0
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  • 9
    Online Resource
    Online Resource
    AIP Publishing ; 2021
    In:  Journal of Applied Physics Vol. 130, No. 11 ( 2021-09-21)
    In: Journal of Applied Physics, AIP Publishing, Vol. 130, No. 11 ( 2021-09-21)
    Abstract: The resistivity size effect in Ir is quantified with in situ and ex situ transport measurements at 295 and 77 K using epitaxial layers with thickness d = 5–140 nm deposited on MgO(001) and Al2O3(0001) substrates. Data fitting with the Fuchs–Sondheimer model of the measured resistivity ρ vs d for single-crystal Ir(001)/MgO(001) layers deposited at Ts = 1000 °C yield an effective electron mean free path λeff = 7.4 ± 1.2 nm at 295 K, a room-temperature bulk resistivity ρo = 5.2 μΩ cm, and a temperature-independent product ρoλeff = (3.8 ± 0.6)×10−16 Ω m2, which is in good agreement with first-principles predictions. Layers deposited at Ts = 700 °C and stepwise annealed to 1000 °C exhibit a unique polycrystalline multi-domain microstructure with smooth renucleated 111-oriented grains that are & gt;10 μm wide for d = 10 nm, resulting in a 26% lower ρoλeff. Ir(111)/Al2O3(0001) layers exhibit two 60°-rotated epitaxial domains with an average lateral grain size of 88 nm. The grain boundaries cause a thickness-independent resistivity contribution Δρgb = 0.86 ± 0.19 and 0.84 ± 0.12 μΩ cm at 295 and 77 K, indicating an electron reflection coefficient R = 0.52 ± 0.02 for this boundary characterized by a 60° rotation about the ⟨111⟩ axis. The overall results indicate that microstructural features including strain fields from misfit dislocations and/or atomic-level roughness strongly affect the resistivity size effect in Ir. The measured ρoλeff for Ir is smaller than for any other elemental metal and 69%, 43%, and 25% below reported ρoλ products for Co, Cu, and Ru, respectively, indicating that Ir is a promising alternate metal for narrow high-conductivity interconnects.
    Type of Medium: Online Resource
    ISSN: 0021-8979 , 1089-7550
    Language: English
    Publisher: AIP Publishing
    Publication Date: 2021
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    detail.hit.zdb_id: 3112-4
    detail.hit.zdb_id: 1476463-5
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  • 10
    Online Resource
    Online Resource
    American Chemical Society (ACS) ; 2022
    In:  ACS Applied Electronic Materials Vol. 4, No. 12 ( 2022-12-27), p. 5775-5788
    In: ACS Applied Electronic Materials, American Chemical Society (ACS), Vol. 4, No. 12 ( 2022-12-27), p. 5775-5788
    Type of Medium: Online Resource
    ISSN: 2637-6113 , 2637-6113
    Language: English
    Publisher: American Chemical Society (ACS)
    Publication Date: 2022
    detail.hit.zdb_id: 2949097-2
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