• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
• /
• 2008.11a
• /
• pp.141-142
• /
• 2008

Single crystal $ZnIn_2S_4$ layers were grown on thoroughly etched semi-insulating GaAs(100) substrate at $450^{\circ}C$ with hot wall epitaxy (HWE) system by evaporating $ZnIn_2S_4$ source at $610^{\circ}C$. The temperature dependence of the energy band gap of the $ZnIn_2S_4$ obtained from the absorption spectra was well described by the Varshni's relation, $E_g$(T) = 2.9514eV - ($7.24\times10^{-4}$ eV/K)$T^2$/(T + 489 K). After the as-grown $ZnIn_2S_4$ single crystal thin films was annealed in Zn-, S-, and In-atmospheres, the origin of point defects of $ZnIn_2S_4$ single crystal thin films has been investigated by the photoluminescence(PL) at 10 K. The native defects of $V_{Zn}$, $V_s$, $Zn_{int}$, and $S_{int}$, obtained by PL measurements were classified as a donors or acceptors type. And we concluded that the heat-treatment in the S-atmosphere converted $ZnIn_2S_4$ single crystal thin films to an optical p-type. Also, we confirmed that In in $ZnIn_2S_4$/GaAs did not form the native defects because In in $ZnIn_2S_4$ single crystal thin films existed in the form of stable bonds.

• Korean Journal of Materials Research
• /
• v.18 no.6
• /
• pp.318-325
• /
• 2008

Single crystal $ZnIn_2S_4$ layers were grown on thoroughly etched semi-insulating GaAs(100) substrate at $450^{\circ}C$ with hot wall epitaxy (HWE) system by evaporating $ZnIn_2S_4$ source at $610^{\circ}C$. The crystalline structure of the single crystal thin films was investigated by the photoluminescence (PL) and double crystal X-ray rocking curve (DCRC). The temperature dependence of the energy band gap of the $ZnIn_2S_4$ obtained from the absorption spectra was well described by the Varshni's relation, $E_g(T)=2.9514\;eV-(7.24{\times}10^{-4}\;eV/K)T^2/(T＋489\;K)$. After the as-grown $ZnIn_2S_4$ single crystal thin films were annealed in Zn-, S-, and In-atmospheres, the origin of point defects of $ZnIn_2S_4$ single crystal thin films has been investigated by the photoluminescence (PL) at 10 K. The native defects of $V_{Zn}$, $V_S$, $Zn_{int}$, and $S_{int}$ obtained by PL measurements were classified as a donors or acceptors type. And we concluded that the heat-treatment in the S-atmosphere converted $ZnIn_2S_4$ single crystal thin films to an optical p-type. Also, we confirmed that In in $ZnIn_2S_4$/GaAs did not form the native defects because In in $ZnIn_2S_4$ single crystal thin films existed in the form of stable bonds.

• Childhood Kidney Diseases
• /
• v.3 no.1
• /
• pp.27-34
• /
• 1999

Purpose: This study was designed to investigate the changes in soluble interleukin-2 receptor (sIL-2R) level in sera and urines of children with primary nephrotic syndrome, eliminating the confounding effects of age, proteinuria, and steroid treatment. Methods: Soluble IL-2R was measured by ELISA in sera and urines from patients with minimal change nephrotic syndrome or focal segmental glomerulosclerosis as well as from healthy controls. The serum levels and urinary sIL-2R/creatinine ratios were compared between control group and the 12 patient groups divided by their ages (0-1, 2-4, over 5 years), and presence or absence of proteinuria and/or steroid treatment (PU+Tx-, PU+Tx+, PU-Tx+, PU-Tx-). Results: Though the differences were not statistically significant probably because of the small numbers, serum sIL-2R levels seemed to be higher in younger age groups both in patients and control group. Nephrotic children did not show higher serum levels than normal children. Among the patients, proteinuric condition seemed to raise and steroid treatment tended to suppress the serum sIL-2R levels. Urinary sIL-2R/creatinine ratios were higher in younger age groups, more significantly in patients (P<0.001). Proteinuria and steroid treatment affected the urinary sIL-2R/creatinine ratios by the same way as the serum sIL-2R levels. Serum sIL-2R levels and urinary sIL-2R/creatinine ratios were not different between groups of different histologic findings or steroid responsiveness (P>0.05). Conclusion: Serum sIL-2R levels and the urinary sIL-2R/creatinine ratios were higher in younger age, and they were not higher in nephrotic patients compared to control group. The patients in relapse showed higher levels, while the levels were suppressed with steroid treatment. In proteinuric state, urinary sIL-2R/creatinine ratios reflected serum sIL-2R levels.

• Bulletin of the Korean Mathematical Society
• /
• v.32 no.2
• /
• pp.271-279
• /
• 1995

In 1986, Fabry, Mawhin and Nkashama [1] have considered periodic solutios for Lienard equation $$ (1_s) x" + f(x)x' + g(t,x) = s, $$ where s is a real parameter, f and g are continuous functions, and g is $2\pi$-periodic in t and have proved that if $$ (H) lim_{$\mid$x$\mid$\to\infty} g(t,x) = \infty uniformly in t \in [0,2\pi], $$ there exists $s_1 \in R$ such that $(1_s)$ has no $2\pi$periodic solution if $s< s_1$, and at least one $2\pi$-periodic solution if $s = s_1$, and at least two $2\pi$-periodic solutions if $s > s_1$.s_1$.

• Journal of Korean Society of Environmental Engineers
• /
• v.38 no.6
• /
• pp.317-322
• /
• 2016

While PFOS sodium salt ($C_8F_{17}SO_3Na$) was not degraded by microorganisms for 28 days, the 4 alternatives were biodegraded at the rates of 21.6% for $C_{25}F_{17}H_{32}S_3O_{13}Na_3$, 20.5% for $C_{15}F_9H_{21}S_2O_8Na_2$, 15.8% for $C_{23}F_{18}H_{28}S_2O_8Na_2$ and 6.4% for $C_{17}F_9H_{25}S_2O_8Na_2$, respectively. The acute toxicity test using Daphnia magna was conducted for 48 hours, the half effective concentration ($EC_{50}$) of PFOS sodium salt ($C_8F_{17}SO_3Na$) was evaluated in 54.5 mg/L. While the 4 alternatives did not show any effect at 500.0 mg/L. The surface tension of the PFOS salt ($C_8F_{17}SO_3Na$) is 46.2 mN/m at a concentration of 500.0 mg/L. While the surface tension of the 4 alternatives was found to be superior to PFOS sodium salt ($C_8F_{17}SO_3Na$). The surface tension of $C_{23}F_{18}H_{28}S_2O_8Na_2$ (20.9 mN/m) has the lowest, followed by $C_{15}F_9H_{21}S_2O_8Na_2$ (23.4 mN/m), $C_{17}F_9H_{25}S_2O_8Na_2$ (27.3 mN/m), $C_{25}F_{17}H_{32}S_3O_{13}Na_3$ (28.2 mN/m). The four kinds of alternatives ($C_{15}F_9H_{21}S_2O_8Na_2$, $C_{17}F_9H_{25}S_2O_8Na_2$, $C_{23}F_{18}H_{28}S_2O_8Na_2$, $C_{25}F_{17}H_{32}S_3O_{13}Na_3$) were found to be superior to PFOS sodium salt ($C_8F_{17}SO_3Na$) in terms of biodegradation, Daphnia sp. acute toxicity and surface tension, and thus they were considered applicable as PFOS alternatives. Especially biodegradation rate of $C_{15}F_9H_{21}S_2O_8Na_2$, $C_{23}F_{18}H_{28}S_2O_8Na_2$ and $C_{25}F_{17}H_{32}S_3O_{13}Na_3$ was relatively high as 15.8~21.6%, and Daphnia sp. acute toxicity and surface tension were considerably superior (surface tension 39~55%) to PFOS sodium salt. Therefore, these alternatives are considered to be available as an alternative of PFOS.

• Journal of the Korean Ceramic Society
• /
• v.22 no.2
• /
• pp.58-62
• /
• 1985

2.5~40$mu extrm{m}$ 영역에서 $As_2S_3$ 및 $GeS_{2.1}$ 유리의 적외선흡수에 관하여 연구했다. Lucovsky와 그의 연구팀이 제창훈 분자 모델에 의하면 8-20$\mu\textrm{m}$ 영역에서 위의 유리물질의 multiphonon 흡수대는 고립된 각 분자의 기본진동대의 overtone 및 combination과 같다. Lucovsky와 Galeener는 이이론에 입각하여 network 구조를 갖는 유리가 적외선 및 라만 스펙트럼에서 나타나는 multiphonon combination 과 overtone 진동수를 예언하는 실험적 선택룰을 제안했다 우리가 얻은 As2S3 및 GeS2.1 유리의 적외선 스펙트럼은 이 유리에 대해 적용한 위의 실험법칙과 잘 일치한다.

• Transactions of the Korean hydrogen and new energy society
• /
• v.4 no.2
• /
• pp.5-15
• /
• 1993

Hydrogen production in visible light with the following semiconductor systems, $CdS-WO_3$, $CdS-TiO_2$, have been investigated in the presence of redox catalyst (Pt, $RuO_2$). MeOH, EtOH, isopropanol, sulfide/sulfite mixture, lactic acid were used as sacrifical reagents. The optimal condition for $H_2$ evolution was found to be in qgueous lactic acid media for $CdS-WO_3/RuO_2$. The photochemical efficiency for this system was 1.05 % and the $H_2$ evolution rate was 26.5ml/min. at $6.07{\times}10^{-5}$ einstein/sec photon rate

• Bulletin of the Korean Chemical Society
• /
• v.14 no.6
• /
• pp.678-681
• /
• 1993

The new ternary phase $UP_2S_6$ has been prepared and structurally characterized. The compound is isostructural with $ZrP_2S_6$ and $ThP_2S_6$ but is different from $TiP_2S_6$. The structure has been determined by a single crystal X-ray diffraction technique. $UP_2S_6$ crystallizes in the the tetragonal system $({C^2}_{4h}-P4_2/m,\;a=6.797(7)\;{\AA},\;c=9.738(12)\;{\AA})$ with two formula units in the unit cell. The structure can be described in terms of $U^{4+}$ and ${P_2S_6}^{4-}$ ions. This hexathiohypodiphosphate anion $({P_2S_6}^{4-})$ has ideally staggered conformation. The $U^{4+}$ cation is coordinated by 8 sulfur atoms in a slightly distorted dodecahedral geometry (42m). The distribution of sulfur atoms is very well optimized for this geometry.

• Journal of Sensor Science and Technology
• /
• v.3 no.1
• /
• pp.78-82
• /
• 1994

Single-phase $CuInS_{2}$ thin film were prepared by E-beam deposition and the effects of its annealing were investigated. The S/In/Cu was stacked from S, In and Cu by EBE method and then, In the nitrogen atmosphere, the stacked layer were annealed to convert chalcopyrite $CuInS_{2}$ thin films. and that result we obtained p-type Chalcopyrite $CuInS_{2}$ thin films, Its resistivity was $0.03{\sim}0.007{\Omega}cm$, Hall mobility was $0.07{\sim}0.1cm^{2}V^{-1}S^{-1}$ and Hall concentration was $10^{20-21}cm^{-3}$, respectively.

• Journal of the Korean Mathematical Society
• /
• v.55 no.2
• /
• pp.373-390
• /
• 2018

In this paper we study the small-data scattering of the d dimensional fractional $Schr{\ddot{o}}dinger$ equations with d = 2, 3, $L{\acute{e}}vy$ index 1 < ${\alpha}$ < 2 and Hartree type nonlinearity $F(u)={\mu}({\mid}x{\mid}^{-{\gamma}}{\ast}{\mid}u{\mid}^2)u$ with max(${\alpha}$, ${\frac{2d}{2d-1}}$) < ${\gamma}{\leq}2$, ${\gamma}$ < d. This equation is scaling-critical in ${\dot{H}}^{s_c}$, $s_c={\frac{{\gamma}-{\alpha}}{2}}$. We show that the solution scatters in $H^{s,1}$ for any s > $s_c$, where $H^{s,1}$ is a space of Sobolev type taking in angular regularity with norm defined by ${\parallel}{\varphi}{\parallel}_{H^{s,1}}={\parallel}{\varphi}{\parallel}_{H^s}+{\parallel}{\nabla}_{{\mathbb{S}}{\varphi}}{\parallel}_{H^s}$. For this purpose we use the recently developed Strichartz estimate which is $L^2$-averaged on the unit sphere ${\mathbb{S}}^{d-1}$ and utilize $U^p-V^p$ space argument.