31 research outputs found
Examining the Effect of Narrative Features and Thematic Music in an Audio-Based Exergame
Audio-based exergames are beneficial in that they allow users to exercise in an eyes-free and hands-free environment. In this study, we explored two audio-based exergame elements, narrative features and thematic music, that can impact exercise amount (step count and duration) and exercise enjoyment. We conducted a two-week long between-subjects study with 43 young adults and 43 middle-aged adults using SPORTIFY, an audio-based exergame. Our experimental results showed that (1) Using narrative features had a significant main effect on exercise amount and exercise enjoyment both for young adults and middle-aged adults. (2) Using thematic music had no significant main impact on exercise amount and exercise enjoyment both for young adults and middle-aged adults. (3) A significant interaction effect for exercise amount was observed in middle-aged adults, whereas a significant interaction effect for exercise enjoyment was observed in young adults.</p
Size Dependence of Excitation-Energy-Related Surface Trapping Dynamics in PbS Quantum Dots
Using ultrafast transient absorption
spectroscopy, we investigated
the surface carrier trapping dynamics in various sized PbS quantum
dots (QDs) when either a hot or cold exciton is photogenerated by
different pump-energy. We observed that hot carriers exhibit distinctly
different surface trapping dynamics from the cold exciton, in which
their corresponding transient absorption (TA) spectral evolutions
show clear differences in the long wavelength region (less than a
band gap energy, <i>E</i><sub>g</sub>). We observed a rapid
growth in the degree of surface trapping with an increase in the pump-energy.
On the other hand, the degree of surface trapping in terms of the
number of created excitons (āØ<i>N</i><sub><i>x</i></sub>ā©) shows negligible variation upon photoexcitation
at any given wavelength. The photoinduced electronāhole separation
followed by carrier trapping was characterized by ultrafast trapping
rate. The surface trapping rate was solely dependent on the PbS QD
size; the surface trapping rate becomes faster as the QD size increases.
Furthermore, we explain the dependence of QD size on the surface trapping
rate in terms of the size-dependent exciton binding energy (<i>E</i><sub>eb</sub>)
Effect of the Framework Flexibility on the Centricities in Centrosymmetric In<sub>2</sub>Zn(SeO<sub>3</sub>)<sub>4</sub> and Noncentrosymmetric Ga<sub>2</sub>Zn(TeO<sub>3</sub>)<sub>4</sub>
The solid-state syntheses, crystal structures, and characterization
of two stoichiometrically similar quaternary mixed metal selenite
and tellurite, In<sub>2</sub>ZnĀ(SeO<sub>3</sub>)<sub>4</sub> and Ga<sub>2</sub>ZnĀ(TeO<sub>3</sub>)<sub>4</sub>, respectively, are reported.
While In<sub>2</sub>ZnĀ(SeO<sub>3</sub>)<sub>4</sub> crystallizes in
the centrosymmetric monoclinic space group <i>P</i>2<sub>1</sub>/<i>n</i> (No. 14) with <i>a</i> = 8.4331(7)
Ć
, <i>b</i> = 4.7819(4) Ć
, <i>c</i> =
14.6583(13) Ć
, and Ī² = 101.684(6)Ā°, Ga<sub>2</sub>ZnĀ(TeO<sub>3</sub>)<sub>4</sub> crystallizes in the non-centrosymmetric
space group <i>I</i>-43<i>d</i> (No. 220) with <i>a</i> = <i>b</i> = <i>c</i> = 10.5794(8)
Ć
. In<sub>2</sub>ZnĀ(SeO<sub>3</sub>)<sub>4</sub> exhibits a two-dimensional
crystal structure consisting of distorted InO<sub>6</sub> octahedra,
ZnO<sub>6</sub> octahedra, and SeO<sub>3</sub> polyhedra. Ga<sub>2</sub>ZnĀ(TeO<sub>3</sub>)<sub>4</sub> shows a three-dimensional framework
structure that is composed of GaO<sub>4</sub> or ZnO<sub>4</sub> and
TeO<sub>3</sub> polyhedra. An effect of the framework flexibility
on the space group centricity is discussed. The SHG (second harmonic
generation) efficiency of noncentrosymmetric Ga<sub>2</sub>ZnĀ(TeO<sub>3</sub>)<sub>4</sub>, using 1064 nm radiation, is similar to that
of KH<sub>2</sub>PO<sub>4</sub> (KDP) and is not phase-matchable (Type
1). Complete characterizations including infrared spectroscopy and
thermal analyses for the reported materials are also presented, as
are dipole moment calculations
Selective Electrochemical Conversion of Carbon Dioxide to Formic Acid on Oxide-Derived Sn<sub><i>x</i></sub>Zn Bimetallic Catalysts
The
use of bimetallic catalysts for electrochemical CO2 reduction
is considered a promising strategy to enhance the catalytic
activity as well as the selectivity. Here, oxide-derived (OD) SnāZn
bimetallic electrocatalysts are developed for the exclusive conversion
of CO2 to HCOOH in an aqueous media. A pure Zn catalyst
promotes conversion of CO2 to CO with a high Faradaic efficiency
(FE) of 80%, whereas a Sn1Zn nanoporous catalyst drives
an efficient CO2-to-HCOOH pathway with a high FEHCOOH of 80% at a moderate overpotential of ā1.0 VRHE. The interaction between Sn and Zn plays an essential role in tuning
the selectivity and catalytic activity. SnāZn bimetallic catalysts
effectively localize electrons to metallic Sn, facilitating the selective
and stable conversion of CO2 to HCOOH. Additionally, the
catalyst maintains its initial efficiency even after a long-term (18
h) CO2 reduction reaction. This study experimentally demonstrates
that OD SnāZn bimetallic catalysts are efficient and stable
for reducing the CO2 gas to HCOOH
Thermoelectric Properties of Ultralong Silver Telluride Hollow Nanofibers
Ultralong
Ag<sub><i>x</i></sub>Te<sub><i>y</i></sub> nanofibers
were synthesized for the first time by galvanically
displacing electrospun Ni nanofibers. Control over the nanofiber morphology,
composition, and crystal structure was obtained by tuning the Ag<sup>+</sup> concentrations in the electrolytes. While Te-rich branched
p-type Ag<sub><i>x</i></sub>Te<sub><i>y</i></sub> nanofibers were synthesized at low Ag<sup>+</sup> concentrations,
Ag-rich nodular Ag<sub><i>x</i></sub>Te<sub><i>y</i></sub> nanofibers were obtained at high Ag<sup>+</sup> concentrations.
The Te-rich nanofibers consist of coexisting Te and Ag<sub>7</sub>Te<sub>4</sub> phases, and the Ag-rich fibers consist of coexisting
Ag and Ag<sub>2</sub>Te phases. The energy barrier height at the phase
interface is found to be a key factor affecting the thermoelectric
power factor of the fibers. A high barrier height increases the Seebeck
coefficient, <i>S</i>, but reduces the electrical conductivity,
Ļ, due to the energy filter effect. The Ag<sub>7</sub>Te<sub>4</sub>/Te system was not competitive with the Ag<sub>2</sub>Te/Ag
system due to its high barrier height where the increase in <i>S</i> could not overcome the severely diminished electrical
conductivity. The highest power factor was found in the Ag<sub>2</sub>Te/Ag-rich nanofibers with an energy barrier height of 0.054 eV
Galvanically Displaced Ultralong Pb<sub><i>x</i></sub>Se<sub><i>y</i></sub>Ni<sub><i>z</i></sub> Hollow Nanofibers with High Thermopower
A cost-effective
process that combines electrospinning and a galvanic
displacement reaction was utilized to synthesize ultralong hollow
Pb<sub><i>x</i></sub>Se<sub><i>y</i></sub>Ni<sub><i>z</i></sub> nanofibers with controlled dimensions, morphology,
composition, and crystal structure. Ni nanofibers were electrospun
with an average diameter of 150 nm and were used as the sacrificial
material for the galvanic displacement reaction. The composition and
morphology of the Pb<sub><i>x</i></sub>Se<sub><i>y</i></sub>Ni<sub><i>z</i></sub> nanofibers were controlled
during the reaction by tuning the concentration of HSeO<sub>2</sub><sup>+</sup> in the electrolytes. Hollow Pb<sub><i>x</i></sub>Se<sub><i>y</i></sub>Ni<sub><i>z</i></sub> nanofibers with smooth surfaces were obtained from the low-concentration
HSeO<sub>2</sub><sup>+</sup> solution (i.e., 0.01 and 0.05 mM), but
the hollow nanofibers synthesized from the high-concentration HSeO<sub>2</sub><sup>+</sup> solution (i.e., 1 mM) have rough outer surfaces
with nanocrystal protrusions. The Pb content of the nanofibersā
composition was varied from 3 to 42% by adjusting the HSeO<sub>2</sub><sup>+</sup> concentration. The thermoelectric properties of the
nanofiber mats were characterized, and the highest Seebeck coefficient
of approximately 449 Ī¼V/K at 300 K was found for the Pb<sub>37</sub>Se<sub>59</sub>Ni<sub>4</sub> nanofiber mat
Designing Novel LiDAR-Detectable Plate-Type Materials: Synthesis, Chemistry, and Practical Application for Autonomous Working Environment
Plate-type hollow black TiO2 (HL/BT) with
a high NIR
reflectance was fabricated for the first time as a LiDAR-detectable
black material. A TiO2 layer was formed on commercial-grade
glass by using the solāgel method to obtain a plate-type structure.
The glass template was then etched with hydrofluoric acid to form
a hollow structure, and blackness was further achieved through NaBH4 reduction, which altered the oxidation state of TiO2 to black TixO2xā1 or Ti4+ to Ti3+ and Ti2+. The blackness of the HL/BT material was maintained by a
novel approach that involved etching prior to reduction. The thickness
of the TiO2 layer was controlled to maximize the NIR reflectance
when applied as paint. The HL/BT material with a thickness of 140
nm (HL/BT140) showed a blackness (L*) of 13.3 and
high NIR reflectance of 23.6% at a wavelength of 905 nm. This is attributed
to the effective light reflection at the interface created by the
TiO2 layer and the hollow structure. Plate-type HL/BT140
provides excellent spreadability, durability, and thermal stability
in practical paint applications compared with sphere-type materials
due to the higher contacting area to the applied surface, making it
suitable for use as a LiDAR-detectable inorganic black pigment in
autonomous environments
Mitral Regurgitation Severity.
<p>P wave area in lead V1 (mean Ā± standard deviation) in relation to MR severity on cine-CMR (<b>3A</b>) and echo (<b>3B</b>). Note that P wave area increased stepwise in relation to MR severity as measured by both modalities, with greatest magnitude of increase at a threshold of moderate-severe MR (black bars).</p
Designing Novel LiDAR-Detectable Plate-Type Materials: Synthesis, Chemistry, and Practical Application for Autonomous Working Environment
Plate-type hollow black TiO2 (HL/BT) with
a high NIR
reflectance was fabricated for the first time as a LiDAR-detectable
black material. A TiO2 layer was formed on commercial-grade
glass by using the solāgel method to obtain a plate-type structure.
The glass template was then etched with hydrofluoric acid to form
a hollow structure, and blackness was further achieved through NaBH4 reduction, which altered the oxidation state of TiO2 to black TixO2xā1 or Ti4+ to Ti3+ and Ti2+. The blackness of the HL/BT material was maintained by a
novel approach that involved etching prior to reduction. The thickness
of the TiO2 layer was controlled to maximize the NIR reflectance
when applied as paint. The HL/BT material with a thickness of 140
nm (HL/BT140) showed a blackness (L*) of 13.3 and
high NIR reflectance of 23.6% at a wavelength of 905 nm. This is attributed
to the effective light reflection at the interface created by the
TiO2 layer and the hollow structure. Plate-type HL/BT140
provides excellent spreadability, durability, and thermal stability
in practical paint applications compared with sphere-type materials
due to the higher contacting area to the applied surface, making it
suitable for use as a LiDAR-detectable inorganic black pigment in
autonomous environments
Multivariate Models for Prediction of Increased P wave Area in Lead V1* in Overall CMR Population.
<p>Multivariate Models for Prediction of Increased P wave Area in Lead V1* in Overall CMR Population.</p