4 research outputs found

    Defect-Free Erbium Silicide Formation Using an Ultrathin Ni Interlayer

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    An ultrathin Ni interlayer (∼1 nm) was introduced between a TaN-capped Er film and a Si substrate to prevent the formation of surface defects during thermal Er silicidation. A nickel silicide interfacial layer formed at low temperatures and incurred uniform nucleation and the growth of a subsequently formed erbium silicide film, effectively inhibiting the generation of recessed-type surface defects and improving the surface roughness. As a side effect, the complete transformation of Er to erbium silicide was somewhat delayed, and the electrical contact property at low annealing temperatures was dominated by the nickel silicide phase with a high Schottky barrier height. After high-temperature annealing, the early-formed interfacial layer interacted with the growing erbium silicide, presumably forming an erbium silicide-rich Er–Si–Ni mixture. As a result, the electrical contact property reverted to that of the low-resistive erbium silicide/Si contact case, which warrants a promising source/drain contact application for future high-performance metal–oxide–semiconductor field-effect transistors

    Al<sub>2</sub>O<sub>3</sub> Passivation Effect in HfO<sub>2</sub>·Al<sub>2</sub>O<sub>3</sub> Laminate Structures Grown on InP Substrates

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    The passivation effect of an Al<sub>2</sub>O<sub>3</sub> layer on the electrical properties was investigated in HfO<sub>2</sub>–Al<sub>2</sub>O<sub>3</sub> laminate structures grown on indium phosphide (InP) substrate by atomic-layer deposition. The chemical state obtained using high-resolution X-ray photoelectron spectroscopy showed that interfacial reactions were dependent on the presence of the Al<sub>2</sub>O<sub>3</sub> passivation layer and its sequence in the HfO<sub>2</sub>–Al<sub>2</sub>O<sub>3</sub> laminate structures. Because of the interfacial reaction, the Al<sub>2</sub>O<sub>3</sub>/HfO<sub>2</sub>/Al<sub>2</sub>O<sub>3</sub> structure showed the best electrical characteristics. The top Al<sub>2</sub>O<sub>3</sub> layer suppressed the interdiffusion of oxidizing species into the HfO<sub>2</sub> films, whereas the bottom Al<sub>2</sub>O<sub>3</sub> layer blocked the outdiffusion of In and P atoms. As a result, the formation of In–O bonds was more effectively suppressed in the Al<sub>2</sub>O<sub>3</sub>/HfO<sub>2</sub>/Al<sub>2</sub>O<sub>3</sub>/InP structure than that in the HfO<sub>2</sub>-on-InP system. Moreover, conductance data revealed that the Al<sub>2</sub>O<sub>3</sub> layer on InP reduces the midgap traps to 2.6 × 10<sup>12</sup> eV<sup>–1</sup> cm<sup>–2</sup> (compared to that of HfO<sub>2</sub>/InP, that is, 5.4 × 10<sup>12</sup> eV<sup>–1</sup> cm<sup>–2</sup>). The suppression of gap states caused by the outdiffusion of In atoms significantly controls the degradation of capacitors caused by leakage current through the stacked oxide layers

    Structural and Electrical Properties of EOT HfO<sub>2</sub> (<1 nm) Grown on InAs by Atomic Layer Deposition and Its Thermal Stability

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    We report on changes in the structural, interfacial, and electrical characteristics of sub-1 nm equivalent oxide thickness (EOT) HfO<sub>2</sub> grown on InAs by atomic layer deposition. When the HfO<sub>2</sub> film was deposited on an InAs substrate at a temperature of 300 °C, the HfO<sub>2</sub> was in an amorphous phase with an sharp interface, an EOT of 0.9 nm, and low preexisting interfacial defect states. During post deposition annealing (PDA) at 600 °C, the HfO<sub>2</sub> was transformed from an amorphous to a single crystalline orthorhombic phase, which minimizes the interfacial lattice mismatch below 0.8%. Accordingly, the HfO<sub>2</sub> dielectric after the PDA had a dielectric constant of ∼24 because of the permittivity of the well-ordered orthorhombic HfO<sub>2</sub> structure. Moreover, border traps were reduced by half than the as-grown sample due to a reduction in bulk defects in HfO<sub>2</sub> dielectric during the PDA. However, in terms of other electrical properties, the characteristics of the PDA-treated sample were degraded compared to the as-grown sample, with EOT values of 1.0 nm and larger interfacial defect states (D<sub>it</sub>) above 1 × 10<sup>14</sup> cm<sup>–2</sup> eV<sup>–1</sup>. X-ray photoelectron spectroscopy data indicated that the diffusion of In atoms from the InAs substrate into the HfO<sub>2</sub> dielectric during the PDA at 600 °C resulted in the development of substantial midgap states

    MoS<sub>2</sub>–InGaZnO Heterojunction Phototransistors with Broad Spectral Responsivity

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    We introduce an amorphous indium–gallium–zinc-oxide (<i>a</i>-IGZO) heterostructure phototransistor consisting of solution-based synthetic molybdenum disulfide (few-layered MoS<sub>2</sub>, with a band gap of ∼1.7 eV) and sputter-deposited <i>a</i>-IGZO (with a band gap of ∼3.0 eV) films as a novel sensing element with a broad spectral responsivity. The MoS<sub>2</sub> and <i>a</i>-IGZO films serve as a visible light-absorbing layer and a high mobility channel layer, respectively. Spectroscopic measurements reveal that appropriate band alignment at the heterojunction provides effective transfer of the visible light-induced electrons generated in the few-layered MoS<sub>2</sub> film to the underlying <i>a</i>-IGZO channel layer with a high carrier mobility. The photoresponse characteristics of the <i>a</i>-IGZO transistor are extended to cover most of the visible range by forming a heterojunction phototransistor that harnesses a visible light responding MoS<sub>2</sub> film with a small band gap prepared through a large-area synthetic route. The MoS<sub>2</sub>–IGZO heterojunction phototransistors exhibit a photoresponsivity of approximately 1.7 A/W at a wavelength of 520 nm (an optical power of 1 μW) with excellent time-dependent photoresponse dynamics
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