Abstract:
Nitrides are a technologically important class of materials consisting
of well-known III(A)-nitrides, transition metal and rare-earth nitrides.
While conventional wurtzite nitride semiconductors, such as GaN, InN,
AlGaN, have significantly impacted lighting and high-frequency-highpower electronics, they are inadequate for effectively addressing contemporary challenges such as energy conversion, neuromorphic computing,
quantum computing, and data security.
In the quest for new materials with novel functionalities enabling it
to meet the current requirements, this thesis explores a relatively less
explored III(B)-transition metal nitride, scandium nitride (ScN). Unlike
conventional wurtzite III(A)- nitrides exhibiting direct optical bandgbap, ScN has a cubic rocksalt structure and an indirect bandgap. With
some resemblance (composition, doping, etc.) and with some contrast (structure, bandgap, mobility, etc.) to GaN, ScN provides high hope for
various current scenario applications. This thesis delves into the exploration of ScN films for applications in thermoelectrics, electronics, and
artificial optoelectronic synapses. The thesis comprises of six chapters,
and a brief summary on each is presented below.
In Chapter 1, the significance, evolution, and characteristics of the
emerging III(B)-nitride semiconductor, ScN, are presented. Additionally, a concise introduction to thermoelectricity, Schottky diodes, and
artificial synapses is provided, elucidating their fundamental concepts
and illustrating how ScN showing how ScN seamlessly fits well into each
area.
As ScN exhibit degenerate semiconducting properties and a low thermal conductivity among ambient-stable III-nitrides, it is a potential candidate for thermoelectric application. Chapter 2 explores the thermoelectric performance of MBE deposited thin film. In part-A of this chapter, MBE deposited epitaxial single-crystalline ScN thin film on MgO substrates is shown to have a high Seebeck co-efficient ( -175 µV/K
at 950K) and high thermoelectric power factor (∼2.3×10−3 W/m.K2
).
MBE growth and electronic transport properties are investigated in detail in this part. Previously, theoretical calculations have shown that
scandium and nitrogen vacancies in ScN lead to asymmetric density of
state peaks near the Fermi energy that should be useful for improving the Seebeck coefficient. In part B, we have introduced such defects in
ScN by lithium-ion implantation and investigate the thermoelectric performance. The defects increase the Seebeck coefficient and reduce the
thermal conductivity to half of the thermal conductivity in pristine ScN. A significant rectification of electrical current in the metal/ScN interface is necessary to realize the ScN-based Schottky diode and thermionic
emission in metal/ScN superlattices. Smooth and compact ScN thin
films with low carrier concentration are essential to achieve significant
current rectification. In part A of this chapter, the energy barrier for
various growth modes in ScN thin film deposition with DC reactive magnetron sputtering and its impact on film morphology are investigated.
It is found that a high substrate temperature (∼800 °C) is required to
obtain smooth and compact ScN films. In part B, the electron concentration in ScN is reduced with magnesium (hole) doping. Electrical
characterization of indium (In), silver (Ag), and gold (Au) contacts on
electron-compensated n-ScN reveals that the Indium forms an Ohmic
contact, while Ag and Au form Schottky contact with significant current
rectification. The barrier heights are measured to be 0.55 eV for Ag/ScN
and 0.53 eV for Au/ScN diodes. The von Neumann bottleneck in conventional computing systems can
be overcome by implementing biological neuron-like hardware having
both processing and memory in the same unit. In chapter 4, we show that the negative photoresponse in ScN and positive photoresponse in
Mg-doped ScN can be used as inhibitory and excitatory synapses, respectively, and the persistence in photo-response decay can be exploited
as memory. With these devices, we emulate some of the basic neural
functionalities, like the transition from short-term memory (STM) to
long-term memory (LTM), learning and forgetting curves, frequencydependent paired pulse facilitation (PPF) and paired pulse depression
(PPD), dynamic filtering, Hebbian learning, and logic gate operations. In chapter 5, we try to understand a drastic decrease in electrical
conductivity with increasing Mg compensation in ScN with the quasiclassical Anderson transition theory proposed by Efros and Shklovskii.
The resistivity of intentionally-undoped ScN increases by nine orders
on adding about 3% Mg due to the long-range potential fluctuation
created by the inhomogeneous distribution of the impurities. The carrier
droplets trapped in the potential wells must tunnel unless activated to
percolation level. This room-temperature metal-insulator transition in
heavily n-doped ScN on high compensation with Mg is accompanied
by peculiar phenomena like persistent photoconductivity and increasing
mobility with increasing temperature. Since the crystallinity of ScN
is maintained across the transition, ScN can now be used in epitaxial
single-crystalline devices with a wide range of resistivity The final chapter summarizes the comprehensive findings of the thesis. MBE deposition of ScN films and deliberately inducing defects to
enhance the thermoelectric performance adds a new materials engineering aspect to ScN. The demonstration of significant current rectification
in Ag/ScN and Au/ScN Schottky diodes marks a pivotal development.
The innovative application of ScN as an artificial optoelectronic synapse
introduces a promising avenue for practical implementations. The study
of the quasi-classical Anderson transition in ScN with hole doping not
only advances the understanding of ScN’s electronic compensation behaviour but also contributes to the broader comprehension of the electronic nature of narrow bandgap semiconductors. Altogether, this thesis
delves into the versatility of ScN, showcasing promising advancements
that set the stage for future developments and applications in the realm
of materials science.