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Thermally
Oxidized Al2O3 Thin-Films
in Metal-Insulator-Metal Structures.
Theodore Feldman, Comsewogue HS, Port Jeferson Station, NY; Elena Cimpoiasu,
Xuequing Liu, Nikita Simonian, and Konstantin K. Likharev, Condensed Matter
Research Group, Department of Physics and Astronomy, Stony Brook University.
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Electron tunneling
has long been used as a tool to investigate the properties of thin-film
materials. It is also the underlying phenomenon of a large range of electronic
devices, including applications in the semiconductor industry, particularly,
nonvolatile memory cells. This project investigates metal-insulator-metal
(MIM) structures with aluminum oxide as the dielectric layer. The purpose
of this investigation is to determine the parameters that are characteristic
of aluminum oxide grown as dielectric thin-films in view of the development
of the fabrication technology necessary to process crested tunnel barriers.
The crested tunnel barriers would have a trilayered structure with the
middle layer having the highest barrier height, while the side layers
would have a reduced barrier height. Such trilayer structure of the tunnel
barrier results in accelerated tunneling at higher voltages. This property
is what makes the crested barrier junctions a viable candidate for pertinent
applications, such as nonvolatile memory cells.
The sample barrier wafers examined were fabricated in situ using a cryopumped
vacuum system with a base pressure of 5E-08 Torr. The fabrication process
starts with the deposition of a 100 nm niobium base (Nb) electrode using
dc magnetron sputtering on a two-inch oxidized silicon wafer (Si02). Following
this procedure, the base electrode is blanketed with 100 nm of aluminum
film also using dc magnetron sputtering. The oxide is produced by exposure
of the aluminum to an oxygen atmosphere for a certain period of time.
The least oxidized of the samples, Cr02, was exposed to oxygen at 2.5
Torr for ten minutes, to an exposure of approximately 2E+05 Pa·s,
the moderately oxidized sample Cr05 had an exposure of 3E+07 Pa·s
after forty minutes in a 100 Torr oxygen environment, and the most oxidized
wafer, Cr12 had an exposure of 2E+10 Pa·s after forty hours in
a 100 Torr oxygen environment. These ranges are designed to efficiently
model every thickness of barrier from very thin barriers near the crossover
between resonant and direct tunneling, such as Cr02, to the maximum thickness
of unassisted oxide growth (Cr12).
Measurements were performed on several junctions with areas of 3*3µm2
or 30*30µm2 at liquid helium temperatures (4.2K) namely: ten, eleven,
and sixteen of Cr02, eight, nine, ten, eleven, and sixteen of Cr05, and
junctions seven, eight, eleven, sixteen, twelve, and fifteen (only junctions
twelve and fifteen have areas of 30*30µm2) of Cr12. These measurements
(current versus voltage curves) were performed using the universal testing
setup Octopux. This system uses a series of analog to digital converters
to provide dc current biasing, which is measured using the voltage drop
across a 2kO loading resistor connected in series with the barrier junction.
The measurements were then recorded using a high precision Keithley 2001
multimeter. Data acquisition and visualization were performed with Xlisp,
a built-in programming language. Using this data the experimental I-V
curves and the more sensitive experimental conductance (G) of the sample
versus voltage, which is calculated using the equation: dI/dV (the derivative
of the current with respect to voltage) were plotted. Also, the theoretical
current versus voltage curve and the theoretical conductance were calculated
using the transmission coefficient (the ratio of the electrons that tunnel
through the potential barrier to the electrons incident on the barrier)
found from the exact solution of the Schrödinger equation by a MATLab
computer code.
By comparing these electrical properties of the barrier relationships
between them can be made and by comparing these properties to the chemical
properties of a chip, the conductance and thus structure of the chip can
be optimized. Current results show that there is a direct relationship
between average barrier height and thickness. For our samples, the highest
barrier height was 1.64 eV. This is to be compared with the 3.5 4eV for
sapphire (Al2O3) reported in the literature. However, this disparity of
results is not surprising because the Al2O3 grown in this method is known
to have an amorphous structure rather than a crystalline structure. Therefore,
further optimization and testing of the samples are needed and ongoing.
The development of trilayer crested tunnel barriers may be a forerunner
of great improvements in commercial nonvolatile semiconductor memories
in which digital bits are stored as a minute electrical charge of a small
"floating gate." Equipped with crested barriers, such memory
cells would be able to combine a standard ten-year retention time with
sub-10 nanosecond write/erase times, which today requires one microsecond,
making current technology not applicable to bit-addressable applications.
Thus, the crested barrier memory cells may be used in fast bit-addressable
nonvolatile random access memories with increased scalability that could
decrease its size to the nanometer range, leading to memory devices in
the terabit range.
This research was supported by the Air Force Office of Scientific Research
and a Simons Fellowship.
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