21 research outputs found
Special Issue for KSTP30 Years Anniversary: Recent Steel Research in Mechanics of Plastic Deformation and Materials Processing
Special Issue for KSTP30 Years Anniversary: Recent Steel Research in Mechanics of Plastic Deformation and Materials Processin
Robust Heteroepitaxial Growth of GaN Formulated on Porous TiN Buffer Layers
Gallium nitride (GaN) heteroepitaxial growth is widely
studied
as a semiconductor material due to its various benefits. Especially,
development of a buffer layer between GaN and the substrate verifies
to be an effective strategy to reduce high threading dislocation density.
However, the buffer layer often impedes strong adhesion between the
epilayer and foreign substrate because thermally induced residual
stress often causes delamination of the epilayer during fabrication.
Here, we developed a robust GaN heteroepitaxy employing a porous buffer
layer formulated by hydride vapor phase epitaxy. A sufficiently low
but completely coated thin Ti layer was deposited on the sapphire
substrate, which led to a rough and porous TiN layer after nitridation.
This porous structure enables the penetration of the GaN source into
the porous structure, allowing GaN epitaxy initiation throughout the
TiN layer. As a result, GaN crystal growth can fill the porous area
during the GaN heteroepitaxy. Integrated visualization demonstrated
that the voids were successfully removed by GaN infiltration, enabling
the heteroepitaxial structure to show little deformation, confirmed
by multiple indentations. Last, the void-free GaN heteroepitaxy with
the porous TiN buffer layer displayed robust adhesion after delamination
tests
Robust Heteroepitaxial Growth of GaN Formulated on Porous TiN Buffer Layers
Gallium nitride (GaN) heteroepitaxial growth is widely
studied
as a semiconductor material due to its various benefits. Especially,
development of a buffer layer between GaN and the substrate verifies
to be an effective strategy to reduce high threading dislocation density.
However, the buffer layer often impedes strong adhesion between the
epilayer and foreign substrate because thermally induced residual
stress often causes delamination of the epilayer during fabrication.
Here, we developed a robust GaN heteroepitaxy employing a porous buffer
layer formulated by hydride vapor phase epitaxy. A sufficiently low
but completely coated thin Ti layer was deposited on the sapphire
substrate, which led to a rough and porous TiN layer after nitridation.
This porous structure enables the penetration of the GaN source into
the porous structure, allowing GaN epitaxy initiation throughout the
TiN layer. As a result, GaN crystal growth can fill the porous area
during the GaN heteroepitaxy. Integrated visualization demonstrated
that the voids were successfully removed by GaN infiltration, enabling
the heteroepitaxial structure to show little deformation, confirmed
by multiple indentations. Last, the void-free GaN heteroepitaxy with
the porous TiN buffer layer displayed robust adhesion after delamination
tests
Hydrogen Back-Pressure Effects on the Dehydrogenation Reactions of Ca(BH<sub>4</sub>)<sub>2</sub>
The dehydrogenation reactions of Ca(BH<sub>4</sub>)<sub>2</sub> are investigated under different isobaric conditions using
in situ
synchrotron radiation powder X-ray diffraction and nuclear magnetic
resonance measurements. Ca(BH<sub>4</sub>)<sub>2</sub> dissociates
in multiple steps, and several intermediate phases, such as an amorphous
phase(s), CaB<sub>2</sub>H<sub><i>x</i></sub>, and CaB<sub>12</sub>H<sub>12</sub>, are observed during dehydrogenation. Among
the intermediate phases, it is known that CaB<sub>2</sub>H<sub><i>x</i></sub> is fully reversible, while the more stable CaB<sub>12</sub>H<sub>12</sub> with an icosahedral structure hinders reversible
reactions. Here, we try to control the dehydrogenation reaction pathway
of Ca(BH<sub>4</sub>)<sub>2</sub> by applying different hydrogen back-pressures.
The decomposition reaction of Ca(BH<sub>4</sub>)<sub>2</sub> in the
absence of a catalyst was found to be sensitive to the H<sub>2</sub> back-pressure. At <i>p</i>(H<sub>2</sub>) = 1 bar, Ca(BH<sub>4</sub>)<sub>2</sub> decomposes via two competitive dehydrogenation
reaction routes to form CaB<sub>2</sub>H<sub><i>x</i></sub> or CaB<sub>12</sub>H<sub>12</sub>. At <i>p</i>(H<sub>2</sub>) = 10 bar, the overall dehydrogenation reaction remains unchanged.
However, the formation of CaB<sub>2</sub>H<sub><i>x</i></sub> is reduced, and amorphous elemental boron is observed as a final
dehydrogenation product. At <i>p</i>(H<sub>2</sub>) = 20
bar, the elemental boron formation is significantly increased, and
the formation of the CaB<sub>2</sub>H<sub><i>x</i></sub> phase is suppressed. Possible routes to form CaH<sub>2</sub> and
elemental boron are discussed
Robust Heteroepitaxial Growth of GaN Formulated on Porous TiN Buffer Layers
Gallium nitride (GaN) heteroepitaxial growth is widely
studied
as a semiconductor material due to its various benefits. Especially,
development of a buffer layer between GaN and the substrate verifies
to be an effective strategy to reduce high threading dislocation density.
However, the buffer layer often impedes strong adhesion between the
epilayer and foreign substrate because thermally induced residual
stress often causes delamination of the epilayer during fabrication.
Here, we developed a robust GaN heteroepitaxy employing a porous buffer
layer formulated by hydride vapor phase epitaxy. A sufficiently low
but completely coated thin Ti layer was deposited on the sapphire
substrate, which led to a rough and porous TiN layer after nitridation.
This porous structure enables the penetration of the GaN source into
the porous structure, allowing GaN epitaxy initiation throughout the
TiN layer. As a result, GaN crystal growth can fill the porous area
during the GaN heteroepitaxy. Integrated visualization demonstrated
that the voids were successfully removed by GaN infiltration, enabling
the heteroepitaxial structure to show little deformation, confirmed
by multiple indentations. Last, the void-free GaN heteroepitaxy with
the porous TiN buffer layer displayed robust adhesion after delamination
tests
Robust Heteroepitaxial Growth of GaN Formulated on Porous TiN Buffer Layers
Gallium nitride (GaN) heteroepitaxial growth is widely
studied
as a semiconductor material due to its various benefits. Especially,
development of a buffer layer between GaN and the substrate verifies
to be an effective strategy to reduce high threading dislocation density.
However, the buffer layer often impedes strong adhesion between the
epilayer and foreign substrate because thermally induced residual
stress often causes delamination of the epilayer during fabrication.
Here, we developed a robust GaN heteroepitaxy employing a porous buffer
layer formulated by hydride vapor phase epitaxy. A sufficiently low
but completely coated thin Ti layer was deposited on the sapphire
substrate, which led to a rough and porous TiN layer after nitridation.
This porous structure enables the penetration of the GaN source into
the porous structure, allowing GaN epitaxy initiation throughout the
TiN layer. As a result, GaN crystal growth can fill the porous area
during the GaN heteroepitaxy. Integrated visualization demonstrated
that the voids were successfully removed by GaN infiltration, enabling
the heteroepitaxial structure to show little deformation, confirmed
by multiple indentations. Last, the void-free GaN heteroepitaxy with
the porous TiN buffer layer displayed robust adhesion after delamination
tests
Elastic modulus of steel at various temperatures [20].
<p>Elastic modulus of steel at various temperatures <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0035987#pone.0035987-Wray1" target="_blank">[20]</a>.</p
Densities of austenite and ferrite phase as a function of temperature and chemical composition [21].
<p>Densities of austenite and ferrite phase as a function of temperature and chemical composition <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0035987#pone.0035987-Miettinen1" target="_blank">[21]</a>.</p
Comparison between measured [<b>18</b>] and calculated transformation plastic strains according to externally applied stress.
<p>(Yield stress of ferrite: 160 MPa, Yield stress of austenite: 200 MPa).</p
Calculated distribution of von-Mises stress during austenite-to-ferrite transformation.
<p>Calculated distribution of von-Mises stress during austenite-to-ferrite transformation.</p
