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Probing the Dielectric Properties of Ultrathin Al/Al<sub>2</sub>O<sub>3</sub>/Al Trilayers Fabricated Using<i>in Situ</i>Sputtering and Atomic Layer Deposition

67

Citations

39

References

2018

Year

Abstract

Dielectric properties of ultrathin Al<sub>2</sub>O<sub>3</sub> (1.1-4.4 nm) in metal-insulator-metal (M-I-M) Al/Al<sub>2</sub>O<sub>3</sub>/Al trilayers fabricated in situ using an integrated sputtering and atomic layer deposition (ALD) system were investigated. An M-I interfacial layer (IL) formed during the pre-ALD sample transfer even under high vacuum has a profound effect on the dielectric properties of the Al<sub>2</sub>O<sub>3</sub> with a significantly reduced dielectric constant (ε<sub>r</sub>) of 0.5-3.3 as compared to the bulk ε<sub>r</sub> ∼ 9.2. Moreover, the observed soft-type electric breakdown suggests defects in both the M-I interface and the Al<sub>2</sub>O<sub>3</sub> film. By controlling the pre-ALD exposure to reduce the IL to a negligible level, a high ε<sub>r</sub> up to 8.9 was obtained on the ALD Al<sub>2</sub>O<sub>3</sub> films with thicknesses from 3.3 to 4.4 nm, corresponding to an effective oxide thickness (EOT) of ∼1.4-1.9 nm, respectively, which are comparable to the EOTs found in high-K dielectrics like HfO<sub>2</sub> at 3-4 nm in thickness and further suggest that the ultrathin ALD Al<sub>2</sub>O<sub>3</sub> produced in optimal conditions may provide a low-cost alternative gate dielectric for CMOS. While ε<sub>r</sub> decreases at a smaller Al<sub>2</sub>O<sub>3</sub> thickness, the hard-type dielectric breakdown at 32 MV/cm and in situ scanning tunneling spectroscopy revealed band gap ∼2.63 eV comparable to that of an epitaxial Al<sub>2</sub>O<sub>3</sub> film. This suggests that the IL is unlikely a dominant reason for the reduced ε<sub>r</sub> at the Al<sub>2</sub>O<sub>3</sub> thickness of 1.1-2.2 nm but rather a consequence of the electron tunneling as confirmed in the transport measurement. This result demonstrates the critical importance in controlling the IL to achieving high-performance ultrathin dielectric in MIM structures.

References

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