2 research outputs found

    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
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