Nanofabrication Technology
for Quantum Effect Devices
S. W. Pang, K. K. Ko, and E. W.
Berg
University of Michigan, Ann Arbor, Michigan 48109-2122, USA
Low-dimensional quantum confined structures
such as quantum dots and quantum wires could provide improved performance for
electrical and optoelectronic devices because of the sharp 1-D density of
states and the enhanced oscillator strengths. Quantum dots and wires were fabricated
by electron beam lithography, dry etching, and epitaxial regrowth. Quantum dots
and wires consisted of AlGaAs/InGaAs multiple quantum wells with 25 nm width
were generated and etched in a Cl2/Ar plasma. The as-etched quantum
dots and wires have smooth surface morphology and vertical profile. Enhanced
electro-optic coefficient was observed on waveguides with quantum dots in the
active region. Microcavities in In0.20Ga0.80As/GaAs were
also fabricated. Significant improvement in the threshold current density has
been predicted for microcavity structures in which the width of the optical
cavity is reduced to 0.3 µm. 0.25 µm wide microcavities were etched to a depth
of 2.8 µm with vertical profile and smooth surface. (Figures 1 and 2)
The in-plane gated (IPG) quantum wire
transistor were fabricated using dry etching in a Cl2/Ar plasma
generated with the ECR source. The 2DEG in the side gates and the channel are
isolated by air gaps, with the 2DEG in the side gates providing electrostatic
modulation of the width of the channel. The electric field from the 2DEG in the
side gate is parallel to the 2DEG in the channel, resulting in a very efficient
coupling of the electric field into the channel. The air gaps between the gates
and the channel should provide negligible gate leakage current and small gate
capacitance for high frequency operation. Modulation of the 1-D channel width
with capacitive coupling using the in-plane gates has been demonstrated, and
good device characteristics were obtained. Gate leakage current <0.1 nA was
measured on IPG transistors with a gate isolation depth of 520 nm. (Figure 3)

Figure 1. Scanning electron micrograph of
quantum dots after dry etching using an ECR source. A Cl2/Ar plasma
generated with 50 W microwave power and 50 W rf power at 0.6 mTorr was used.

Figure 2. 0.25 µm wide microcavities in In0.20Ga0.80As/GaAs
etched down to 2.8 µm deep.

Figure 3. Scanning electron micrograph of a
in-plane gated quantum wire transistor. The in-plane gates were etched by a Cl2/Ar plasma
generated with 20% Cl2 using 50 W
microwave power and 100 W rf power at 0.5 mTorr.
References
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Pang, "Low Pressure Etching of Nanostructures and Via Holes Using an
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Pang, "Optical and Electrical Characteristics of InGaAs and GaAs
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M. J. Rooks, "Photoluminescence and Electro-Optic Properties of Small
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Pang, "Controllable Layer by Layer Etching of GaAs with an Electron
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Source", J. Electrochem. Soc. 140, 3620-3623 (1993).
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Pang, "Low Temperature Silicon Oxidation with Oxygen Plasma Generated
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Lithography", J. Vac. Sci. Technol. B 7, 1624-1628 (1989).
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"Submicrometer Structure Fabricated by Dry Etching and Masked Ion
Beam Lithography", J. Electrochem. Soc. 135, 1526-1529 (1988).
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895 (1988).
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Ehrlich, S. W. Pang, and J. N. Randall, "Cermet as an Inorganic
Resist for Ion Lithography", J. Vac. Sci. Technol. B 5, 379 (1987).
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Efremow, S. W. Pang, and A. C. Anderson, "Hot Jet Etching of Pb,
GaAs, and Si", J. Vac. Sci. Technol. B 5, 363 (1987).
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Pang, G. D. Johnson, D. K. Astolfi, and D. J. Ehrlich, "Nanometer
Scale Columns In GaAs Fabricated by Angled Ion Beam Assisted
Etching", Appl. Phys. Lett. 51, 1726-1728 (1987).
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Randall, and M. W. Geis, "Sub-100nm-wide, deep trenches defined by
reactive-ion etching", J. Vac. Sci. Technol. B 4, 341-344 (1986).
Last Updated: November 19, 2007
E-Mail: pang@eecs.umich.edu
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