• Journal of Radiation Protection and Research
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• v.7 no.1
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• pp.23-33
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• 1982

The characteristic thermoluminescence responses of Teflon thermoluminescent dosimeters to radiations have been studied by the variation of radiation qualities as well as the high dose radiations. The change in the sensitivity of TLDs for different radiation qualities were studied through not only the photon energy dependence but also the change of supralinearity on the photon energy dependence, by exposing $^{60}Co$ gamma rays, the effective X-rays of 44keV, 69keV, 108keV, and thermal neutron of 0.04 eV. The results were as the following: The TL response of $T-CaSO_4$: Dy as a function of absorbed dose was linear up to about 5 Gy, and the response beyond 5Gy was supralinear for $^{60}Co$ gamma rays. The supralinearity of T-LiF-7 became noticeably apparent more than that of $T-CaSO_4$:Dy and also the lower the LET of radiation became the higher the supralinear effects were. No supralinearity appeared for the thermal neutron irradiations equivalent to 10Gy of $^{60}Co$ gamma rays. The relative sensitivities (Rs), which depended on the doses of $^{60}Co$ gamma rays to the TLDs of T-LiF-7 and T-$CaSO_4$:Dy could be, respectively, approximated to the following empirical formula fitted by the least square method: $$R_{LiF}=1.021-0.04581\;logD+0.402(logD)^2-0.405(logD)^3,\;\;5{\times}10^3{\geq}D{\geq}1(Gy)$$ $$R_{CaSO_4}=0.976-0.3241\;logD+0.262(logD)^2-0.298(logD)^3,\;5{\times}10^3{\geq}D{\geq}1(Gy)$$.

• Journal of the Korean Society of Radiology
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• v.8 no.4
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• pp.181-187
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• 2014

The purpose of this study were to analyze the characteristic of the glow curves in order to the glow temperature of the thermoluminescent dosimeters (TLDs) for the absorbed dose measurement of the radiation therapy. In this study, we was used the TLDs of the LiF:Mg${\cdot}$Ti, LiF:Mg${\cdot}$Cu${\cdot}$P, $CaF_2$:Dy, $CaF_2$:Mn (Thermo Fisher Scientific Inc., USA). The source-to-solid dry phantom (RW3 slab, IBA Dosmetry, Germany) surface distance was set at 100 cm, and the exposure dose of 100 MU (monitor unit) was used 6- and 15-MV X-rays, and 6- and 12-MeV electron beams in the reference depth, respectively. After the radiations exposure, we were to analyze the glow curves by using the TL reader (Hashaw 3500, Thermo Fisher Scientific Inc., USA) at the fixed heating rate of $15^{\circ}C/sec$ from $50^{\circ}C$ to $260^{\circ}C$. The glow peaks, the trapping level in the captured electrons and holes combined with the emitted light, were discovered the two or three peak. When the definite increasing the temperature of the TLDs, the maximum glow peak representing the glow temperature was follow as; $LiF:Mg{\cdot}Ti$: $185.5{\pm}1.3^{\circ}C$, $LiF:Mg{\cdot}Ti$: $135.0{\pm}5.1^{\circ}C$, $CaF_2$:Dy: $144.0{\pm}1.6^{\circ}C$, $CaF_2$:Mn: $294.3{\pm}3.8^{\circ}C$, respectively. Because the glow emission probability of the captured electrons depend on the heating temperature after the exposure radiation, TLDs by applying the fixed heating rate, the accuracy of measurement will be able to improve within the absorbed dose measurement of the radiation therapy.

• Journal of the Korean Chemical Society
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• v.32 no.1
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• pp.3-8
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• 1988

Nonstoichiometric solid solutions of the $Sr_{1+x}Dy_{1-x}FeO_{4-y}$ system (x = 0. 00, 0. 25, 0. 50, 0. 75 and 1. 00) with layered $K-2NiF_4$ type structure were prepared at 1200$^{\circ}$C under atmospheric pressure. X-ray powder diffraction spectra show that the crystallographic phases of the samples are tetragonal within the x range. Nonstoichiometric chemical formulas have been determined by Mohr salt analysis and it shows that the amount of $Fe^{4+}$ ion or ${\tau}$ value increases with increasing x. Electrical conductivities of the samples which were measured in the temperature range of $-100{\sim}200^{\circ}$C under atmospheric air pressure are varied within the semiconductivity range of $l0^{-8}{\sim}10^{-2}(ohm^{-1}{\cdot}cm^{-1}$) and the activation energies are also varied from 0.02 to 0.08 eV. Mixed valency state of $Fe^{3+}$ and $Fe^{4+}$ in the sample of $Sr_{1.00}Dy_{1.00}FeO_{4.04}$ was identified again by Mossbauer spectrum at 200K.

• Bulletin of the Korean Chemical Society
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• v.25 no.6
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• pp.852-858
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• 2004

Crystal structures of lanthanide complexes with NTA (NTA = nitrilotriacetate) are reported. The complexes of $[Ln(NTA)_2{\cdot}H_2O]^{3-}$ (Ln = Sm, Eu, Gd, Tb and Ho) crystallize in the orthorhombic space group Pccn. In the structures, the trivalent lanthanide ions are completely encapsulated via coordination to the two nitrogen atoms and the six carboxylate oxygen atoms of the two NTA ligands, and one water oxygen atoms. The complexes form a slightly distorted capped-square-antiprism polyhedron. Of the complexes, $[Eu(NTA)_2{\codt}H_2O]^{3-}$,\;[Tb(NTA)_2{\cdot}H_2O]^{3-}\;and\;[Dy(NTA)_2{\cdot}H_2O]^{3-}$ excited at the 325 He-Cd line produce very characteristic luminescence features, arising mostly from the f ${\to}$ f transitions. The absolute quantum yields of these complexes are determined at room temperature. Surprisingly, the $[Dy(NTA)_2{\cdot}H_2O]^{3-}$ complex is more luminescent than the $[Eu(NTA)_2{\cdot}H_2O]^{3-}\;and\;[Tb(NTA)_2{\cdot}H_2O]^{3-}$ complexes.

• Journal of the Korean Ceramic Society
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• v.18 no.2
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• pp.75-78
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• 1981

The electrical conductivity of $(M_2O_3)_x (BaTiO_3)_{1-x}$ has been measured over the temperature range of 30 to 27$0^{\circ}C$. The substitution of rare earth oxide such as $La_2O_3$, $Nd_2O_3$, or $Dy_2O_3$ can be represented by $M_2O_3$. The additional mole fraction of the rare earth oxide is ranged over 0.0015 to 0.0030. The electrical conductivity exhibits an anomalous decrease near the tetragonal to cubic transition about 12$0^{\circ}C$. The decrease in the electrical conductivity is observed at the higher impurity concentrations owing to space charge layer. The increase in the electrical conductivity is observed as the impurity ion is varied from $La^{+3}$$Nd^{+3}$ to $Dy^{+3}$, due to overlap of 4f electrons of the inner shell.

• Proceedings of the Korean Vacuum Society Conference
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• 2013.08a
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• pp.173-173
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• 2013

최근에 고효율의 형광체를 개발하고자 무기물 모체에 주입된 희토류 이온의 발광에 대한 연구가 급부상하고 있다. 형광체는 고휘도, 넓은 시청 각도와 저 비용으로 인하여 대형 평판 디스플레이 분야로 그 응용성을 확장하는 플라즈마 디스플레이 패널 제작에 있어서 매우 중요한 물질이다. 현재 적색 형광체로 널리 사용되고 있는 발광 물질은 YBO3:Eu3+ 혹은 (Y,Gd)BO3:Eu3+ 형광체이지만, Eu3+ 이온이 중심대칭의 자리에 위치하기 때문에, Eu3+ 이온의 5D07F1 전이에 의한 주황색의 발광 세기가 5D07F2 전이에 의한 적색의 세기보다 강하여 고품질의 색상을 구현하는데 상당한 어려움이 있다. 이러한 문제점을 해결하기 위하여 새로운 모체 격자를 갖는 적색, 녹색, 청색 형광체 개발에 많은 노력이 집중되고 있다. 본 연구에서는 형광체 합성시 중요한 변수의 하나인 소결 온도가 새로운 다양한 색을 방출하는 형광체 분말 CaSiO4:RE3+ (RE=Eu, Sm, Tb, Dy, Ce)의 특성에 미치는 영향을 조사하였다. CaSiO4:RE3+ (RE=Eu, Sm, Tb, Dy, Ce) 형광체 분말 시료는 초기 물질 CaO (99.99%), SiO2 (99.99%), Eu2O3 (99.99%), Sm2O3 (99.9%), Tb4O7 (99.9%), Dy2O3 (99.9%), CeO2 (99.9%)을 화학적량으로 준비하였다. 볼밀, 건조 작업을 한 후에, 시료를 막자사발에 넣고 분쇄하여 3시간의 하소 공정과 5시간의 소결 공정을 수행하였다. 이때 소결 온도를 변수로 선택하여 각각 $800^{\circ}C$, $900^{\circ}C$, $1,000^{\circ}C$, $1,100^{\circ}C$에서 소결 작업을 수행하여 합성 분말의 구조, 표면, 광학적 특성을 측정하여 소결 온도가 미치는 영향을 조사하였다. Eu3+가 도핑된 CaSiO4 형광체 분말의 경우에, 발광 스펙트럼은 597, 618, 655, 707 nm에서 관측되었으며, 소결 온도가 $800^{\circ}C$에서 $1,100^{\circ}C$로 증가함에 따라 모든 발광 스펙트럼의 세기는 순차적으로 증가함을 나타내었다. Tb3+가 도핑된 CaSiO4 형광체 분말의 경우에 관측된 발광 스펙트럼은 주 피크인 549 nm를 중심으로 하여 세기가 상대적으로 작은 493, 592, 626 nm의 피크들이 관측되었으며, 소결 온도가 증가함에 따라 전반적으로 발광 세기들이 증가하는 경향을 나타내었다. Sm3+가 도핑된 CaSiO4 형광체의 경우에, 발광 스펙트럼은 전형적인 Sm3+이온에 의한 전이 신호들이 605, 570, 653 nm에서 나타났다. 발광 스펙트럼의 세기는 소결 온도에 비례하여 증가하였다. Ce3+가 도핑된 경우에 발광 스펙트럼은 소결 온도에 관계없이 401 nm에서 관측되었으며, 소결 온도에 따라 발광 세기의 변화가 나타났다. 이 실험 결과로 부터, 합성시 적절한 소결 온도의 선택이 고발광 효율의 형광체를 제작하는데 있어서 매우 중요한 요소가 됨을 확인할 수 있었다.

• Proceedings of the Korean Magnestics Society Conference
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• 2012.11a
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• pp.16-17
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• 2012

• Proceedings of the Korean Magnestics Society Conference
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• 2016.11a
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• pp.136-137
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• 2016

• Journal of the Korean Magnetics Society
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• v.3 no.2
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• pp.143-148
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• 1993

$Bi_{x}Dy_{3-x}Al_{1}Fe_{4}O_{12}$(x=1, 1.2, 1.5) magnetic garnet films were fabricated on the glass substrates by pyrolysis method. As the Bi content was increased, the saturation magnetization increased from 5 emu/cc to 11 emu/cc and all the films showed perpendicular magnetic anisotropy. As the content of Bi was increased, Faraday rotation angle (${\theta}_F$) at 780 nm of the films increased from $0.11^{\circ}/\mu\textrm{m}$ to $0.20^{\circ}/\mu\textrm{m}$ and the garnet crystallization temperature decreased from $660^{\circ}C$ to $630^{\circ}C$. Also, the coercivity ($H_{c}$) decreased from 1200 Oe to 600 Oe and the grain sizes increased. $H_{c}$ decreased from 1750 Oe to 1200 Oe and ${\theta}_F$ increased due to the interference of the reflected laser light as the thickness of the films increased from $2000\;{\AA}$ to $4000\;{\AA}$.

• Asian Journal of Turfgrass Science
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• v.10 no.1
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• pp.41-47
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• 1996

The theory of slope erosion is developed along similar lines to the theory of heat flow in solid added to the correcting factor. if slope erosion in the forest and grassland proceeds according to the hypothesis, it is $\delta$y $\delta^2$y = k $\delta^2$y $\delta$$X^2$+f(s b. t) where 5 is internal properties of slope soil and b is biota on slope. When the variables of the equation of slope erosion are x = -λ the initial elevation=-f(λ), x=λ, x==a, the steady value of the initial elevation=y, and dy dx x=0> =O(t>o), respectively, the houndary condition due to the solution of the equation of slope erosion is y= 2 √$\pi$kt [∫a o λe $(X-λ)^2$4kt dλ- ∫ao- $(x+λ)^2$4kt dλ] + ∫∫∫ f (s.b. t)dtdbds