2 research outputs found
HCl Flow-Induced Phase Change of α‑, β‑, and ε‑Ga<sub>2</sub>O<sub>3</sub> Films Grown by MOCVD
Precise
control of the heteroepitaxy on a low-cost foreign substrate
is often the key to drive the success of fabricating semiconductor
devices in scale when a large low-cost native substrate is not available.
Here, we successfully synthesized three different phases of Ga<sub>2</sub>O<sub>3</sub> (α, β, and ε) films on <i>c</i>-plane sapphire by only tuning the flow rate of HCl along
with other precursors in an MOCVD reactor. A 3-fold increase in the
growth rate of pure β-Ga<sub>2</sub>O<sub>3</sub> was achieved
by introducing only 5 sccm of HCl flow. With continuously increased
HCl flow, a mixture of β- and ε-Ga<sub>2</sub>O<sub>3</sub> was observed, until the Ga<sub>2</sub>O<sub>3</sub> film transformed
completely to a pure ε-Ga<sub>2</sub>O<sub>3</sub> with a smooth
surface and the highest growth rate (∼1 μm/h) at a flow
rate of 30 sccm. At 60 sccm, we found that the film tended to have
a mixture of α- and ε-Ga<sub>2</sub>O<sub>3</sub> with
a dominant α-Ga<sub>2</sub>O<sub>3</sub>, while the growth rate
dropped significantly (∼0.4 μm/h). The film became rough
as a result of the mixture phases since the growth rate of ε-Ga<sub>2</sub>O<sub>3</sub> is much higher than that of α-Ga<sub>2</sub>O<sub>3</sub>. In this HCl-enhanced MOCVD mode, the Cl impurity concentration
was almost identical among the investigated samples. On the basis
of our density functional theory calculation, we found that the relative
energy between β-, ε-, and α-Ga<sub>2</sub>O<sub>3</sub> became smaller, thus inducing the phase change by increasing
the HCl flow in the reactor. Thus, it is plausible that the HCl acted
as a catalyst during the phase transformation process. Furthermore,
we revealed the microstructure and the epitaxial relationship between
Ga<sub>2</sub>O<sub>3</sub> with different phases and the <i>c</i>-plane sapphire substrates. Our HCl-enhanced MOCVD approach
paves the way to achieving highly controllable heteroepitaxy of Ga<sub>2</sub>O<sub>3</sub> films with different phases for device applications
Highly efficient transverse-electric-dominant ultraviolet-c emission employing GaN multiple quantum disks in AlN nanowires matrix
Heavy reliance on extensively studied AlGaN based light emitting diodes (LEDs) to replace environmentally hazardous
mercury based ultraviolet (UV) lamps is inevitable. However, external quantum efficiency (EQE) for AlGaN based deep
UV emitters remains poor. Dislocation induced nonradiative recombination centers and poor electron-hole wavefunction
overlap due to the large polarization field induced quantum confined stark effect (QCSE) in “Al” rich AlGaN are some of
the key factors responsible for poor EQE. In addition, the transverse electric polarized light is extremely suppressed in
“Al”-rich AlGaN quantum wells (QWs) because of the undesired crossing over among the light hole (LH), heavy hole
(HH) and crystal-field split-off (SH) states. Here, optical and structural integrities of dislocation-free ultrathin GaN
quantum disk (QDisk) (~ 1.2 nm) embedded in AlN barrier (~ 3 nm) grown employing plasma-assisted molecular beam
epitaxy (PAMBE) are investigated considering it as a novel nanostructure to realize highly efficient TE polarized deep UV
emitters. The structural and chemical integrities of thus grown QDisks are investigated by high angle annular dark field
scanning transmission electron microscopy (HAADF-STEM). We, particularly, emphasize the polarization dependent
photoluminescence (PL) study of the GaN Disks to accomplish almost purely TE polarized UV (~ 260 nm) light. In
addition, we observed significantly high internal quantum efficiency (IQE) of ~ 80 %, which is attributed to the enhanced
overlap of the electron-hole wavefunction in extremely quantum confined ultrathin GaN QDisks, thereby presenting GaN
QDisks embedded in AlN nanowires as a practical pathway towards the efficient deep UV emitters