• 한국결정성장학회지
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• 제10권5호
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• pp.350-355
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• 2000

수평 Bridgeman방식으로 성장된 C축 방향의 사파이어 결정기판을 연마 가공하였으며, 또한 유기금속 기상화학 증착 방법으로 사파이어 기판 위에 GaN 박막을 증착하였다. 사파이어 인고트를 성장하여 2인치 사파이어 기판으로 이용하였으며 웨이퍼 절편장치 및 연마장치를 개발하였다. 이러한 다단계의 연마 가공은 기판 표면을 경면화하였다. 표면 평탄도 및 조도는 원자힘현미경으로 측정하였다. 개발된 사파이어 기판위에 성장된 GaN 박막의 특성 및 청색광소자로의 응용 가능성을 확인하였다.

• 한국전기전자재료학회논문지
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• 제37권4호
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• pp.412-419
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• 2024

Mn-doped Pb(In_1/2Nb_1/2)O₃-Pb(Mg_2/3Nb_1/3)O₃-PbTiO₃ (Mn:PIN-PMN-PT) single crystals, which exhibit improved phase transition temperatures and coercive field properties compared to Pb(In_1/2Nb_1/2)O₃-Pb(Mg_2/3Nb_1/3)O₃-PbTiO₃ (PIN-PMN-PT) single crystals, are expected to be utilized in high-power acoustic transducers. Bridgeman method, growing single crystals along the axial direction from melt, is most widely used method for single crystal growth with large size and high quality. However, single crystal boules grown by the Bridgeman method demonstrate a PT compositional variation, giving rise a distribution of crystal structure and material properties along the growing axis. To employ piezoelectric single crystals grown by the Bridgeman method for acoustic transducers, it is essential to investigate their overall property distribution. In this study, the compositional distribution and property variation of Mn:PIN-PMN-PT single crystals grown by the Bridgeman method was investigated. Measured compositional distribution of PT was from 29% to 32.5% in the Rhombohedral crystal region of the boule. Two types of specimen, [011]-poled Mn:PIN-PMN-29PT and Mn:PIN-PMN-32PT single crystals, were fabricated and tested to obtain full property variation at both ends of the Rhombohedral crystal region. The properties related to the 32 directional vibration mode and the properties related to high-power driving were measured to confirm the overall distribution of properties by composition.

• 센서학회지
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• 제12권6호
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• pp.273-281
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• 2003

수평 전기로에서 $CdIn_2Te_4$ 다결정을 합성하여 Bridgeman 법으로 3단 수직 전기로에서 $CdIn_2Te_4$ 단결정을 성장하였다. 성장된 결정의 특성은 x선 회절과 광발광 측정으로 조사하였다. $CdIn_2Te_4$ 단결정 시료는 Laue에 배면 반사법에 의해서 (001)면으로 성장되었음을 확인하였다. Hall 효과는 van der Pauw 방법에 의해 측정되었으며, 온도에 의존하는 운반자 농도와 이동도는 293K에서 각각 $8.61{\times}10^{16}/cm^3$, $242\;cm^2/V{\codt}s$였다. $CdIn_2Te_4$ 단결정의 광흡수와 광전류 spectra를 293K에서 10K까지 측정하였다. 광흡수 스펙트럼으로부터 band gap $E_g(T)$는 Varshni공식에 따라 계산한 결과 1.4750eV - $(7.69{\times}10^{-3}\;eV/K)T^2$/(T+2147 K)임을 확인하였다. 막 성장된(as-grown) $CdIn_2Te_4$ 단결정 시료를 Cd-, In-, Te 분위기에서 열처리하여 10K에서 Photoluminescence(PL) spectra를 측정하여 점 결함의 기원을 알아보았다. $CdIn_2Te_4$ 단결정내에서 내재된 결함들의 기원을 10 K에서 광발광을 측정하여 연구되었다. PL 측정으로 부터 얻어진 $V_{Te}$, $Cd_{int}$, $V_{Cd}$, 그리고 $Te_{int}$는 주개와 받개로 분류되어졌다. $CdIn_2Te_4$ 단결정 시료를 Cd 분위기에서 열처리하면 n형으로 변환됨을 악 수 있었고, In 분위기에서 열처리하면 열처리 이전의 PL spectra를 보이고 있어서 $I_2$, $I_1$ 및 S.A emission에 의한 PL peak에는 영향을 주지 않는다고 보았다.

• 한국재료학회지
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• 제13권3호
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• pp.195-199
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• 2003

The $p-CdIn_2$$Te_4$single crystal was grown in the three-stage vertical electric furnace by using Bridgman method. The quality of the grown crystal has been investigated by the x-ray diffraction and the photoluminescence measurements. From the photoluminescence spectra of the as-grown $CdIn_2$$Te_4$crystal and the various heat-treated crystals, the ($D^{\circ}$, X) emission was found to be the dominant intensity in the photoluminescence spectrum of the $CdIn_2$T $e_4$:Cd, while the ($A^{\circ}$, X) emission completely disappeared in the $CdIn_2$T $e_4$:Cd. However, the ($A^{\circ}$, X) emission in the photoluminescence spectrum of the $CdIn_2$T $e_4$:Te was the dominant intensity like an as-grown $CdIn_2$T $e_4$crystal. These results indicated that the ($D^{\circ}$, X) is associated with $V_{Te}$ acted as donor and that the ($A^{\circ}$, X) emission is related to $V_{cd}$ acted as acceptor, respectively. The $p-CdIn_2$T $e_4$crystal was found to be obviously converted into the n-type after annealing in the Cd atmosphere. The origin of ( $D^{\circ}$, $A^{\circ}$) emission and its TO phonon replicas is related to the interaction between donors such as $V_{Te}$ or $Cd_{int}$, and accepters such as $V_{cd}$ or T $e_{int}$. Also, the In in the $CdIn_2$X$CdIn_4$was confirmed not to form the native defects because it existed in the stable form of bonds.

• 센서학회지
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• 제21권4호
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• pp.293-297
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• 2012

CsI:Gd crystal was grown by the Bridgeman method and its scintillation properties were investigated. The wavelength peak of the luminescence spectrum for the crystal excited by X-ray was 419 nm. The range of the spectrum was from 300 nm to 800 nm. The spectrum well matched to the quantum efficiency of a typical bi-alkali photo-multiplier tube(PMT). An energy resolution of 48.2 % was obtained for 662 keV ${\gamma}$-rays of $^{137}Cs$. The three decay times were obtained as a fast(557.4 ns, 42.2 %), intermediate (1.78 ${\mu}s$, 29.7 %) and slow (5.43 ${\mu}s$, 28.1 %) components, respectively.

• 연구논문집
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• 통권23호
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• pp.15-27
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• 1993

The single crystal specimens were solidified by modified Bridgeman method. The surface recrystallized single crystal specimens were prepared by shot peening followed by heat treatment. The surface recrystallization begins at the dendrite cores on the surface. The recrystallized grains grew into the inner side of the specimen. The growth of recrystallized grains was inhibited by the pores and eutectic phases. The primary $\gamma'$ phases were dissolved at the recrystallized grain boundaries during the grain growth. The grain growth of recrystallized grains was similar to the cellular type transformation. No orientation relationships were found bewteen the recrystallized grains and the parent phase.

• 한국수소및신에너지학회논문집
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• 제18권3호
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• pp.342-347
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• 2007

The research on production and application of hydrogen as an alternative energy in the future is being carried out actively. It hydrogen storage is necessary in order that user use hydrogen economically without much difficulty. Among the ways of hydrogen storage the method which is compressed hydrogen gas by high pressure is easier for application than other methods. In this study, we have been calculated gas with changing pressure and temperature variation of container wall through applied to mass and energy balance equation when compressing hydrogen by high pressure, and also to Beattie-Bridgeman equation of state for the kinetic of hydrogen. We will apply above date as a preliminary for design of hydrogen storage tank.

• 한국결정성장학회:학술대회논문집
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• 한국결정성장학회 1998년도 PROCEEDINGS OF THE 14TH KACG TECHNICAL MEETING AND THE 5TH KOREA-JAPAN EMGS (ELECTRONIC MATERIALS GROWTH SYMPOSIUM)
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• pp.39-43
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• 1998

Single crystals of{{{{ { Zn}_{ 1-x} {Mn }_{x }{Te} }}}} with x=0.3-0.6 were prepared by the standard Bridgeman method. Diffuse neutron diffraction intensities due to the short range magnetic ordering is found in the vicinities of 1 1/2 0 reciprocal point and its equivalent point, indicating that the magnetic correlation of the clusters is the type III antiferromangetic one do the F-type Bravais class crystals, being identical with that of {{{{{ Cd}_{ 1-x} {Mn }_{x }Te }}}}. Neutron inelastic scattering measure-ment has been performed for {{{{{ Zn}_{ 0.6} { Mn}_{ 0.4}Te }}}} sample using the cold neutron spectrometer. AGNES. High resolution measurement with the energy resolution of {{{{ TRIANGLE E= +- .01meV}}}} was carried out in the temperature range from 10K to the ambient. Critical scattering, closely related with the spin glass transition, has been observed for the first time in this semimagnetic semi-conductor. The critical scattering is observed at temperatures in the vicinity of the spin glass transition temperature, 17K. The scattering is observed as a kind of quasielastic scattering in the reciprocal range where the elastic magnetic diffuse scattering has been observed, e.g., 11/20 reciprocal point, indicating the spin fluctuation has dynamic components in this material. Photoconductivity has been discovered below 150K in {{{{{ Zn}_{ 0.4} {Mn }_{0.6 } Te}}}}. The electric AC conductivity has been increased dramatically under the laser light with the wave lengths of {{{{ lambda =6328,5145 and4880 }}}}$\AA$ ,respectively. After the light was darkened, the conductivity was reduced to the original level after about 2000 seconds at 50K, being above the spin glass transition temperature. This phenomenon is the typical persistent photoconductivity; PPC which was similarly found in {{{{ { Zn}_{ 1-x} { Mn}_{x} Te}}}}.

• Nuclear Engineering and Technology
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• 제55권8호
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• pp.2797-2801
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• 2023

CdZnTeSe (CZTS) has attracted attention for applications in X- and gamma-ray detectors owing to its improved properties compared to those of CdZnTe (CZT). In this study, we grew and processed single crystals of CZT and CZTS using the Bridgeman method to confirm the feasibility of using a dosimeter for high-energy X-rays in radiotherapy. We evaluated their linearity and precision using the coefficient of determination (R²) and relative standard deviation (RSD). CZTS showed sufficient RSD values lower than 1.5% of the standard for X-ray dosimetry, whereas CZT's RSD values increased dramatically under some conditions. CZTS exhibited an R² value of 0.9968 at 500 V/cm, whereas CZT has an R² value of 0.9373 under the same conditions. The X-ray response of CZTS maintains its pulse shape at various dose rates, and its properties are improved by adding selenium to the CdTe matrix to lower the defect density and sub-grain boundaries. Thus, we validated that CZTS shows a better response than CZT to high-energy X-rays used for radiotherapy. Further, the applicability of an onboard imager, a high-energy X-ray (>6 MV) image, is presented. The proposed methodology and results can guide future advances in X-ray dose detection.

• 한국결정성장학회지
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• 제11권1호
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• pp.6-13
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• 2001

수직 Bridgman 방법으로 $Mg_xZn_{1-x}Te(0{\le}X{\le}0.48)$ 단결정을 성장하였다. 성장된 단결정의 결정구조는 X = 0~ 0.48 범위내에서는 zincblende 이었고, 성분이 증가함에 따라 격자 상수 값이 6.103$\AA$(X = 0.0)으로부터 6.239$\AA$(X = 0.48)까지 a(X)=6.103 + (0.33)X 를 만족하며 선형적으로 증가하였으며, 외사법에 의해 얻어진 zincblende MgTe의 격자상수는 6.433$\pm$0.002$\AA$로 주어졌다. 광전류 스펙트럼 측정 결과 $Mg_xZn_{1-x}Te$(X=0) 단결정의 에너지 띠 간격은 4.2K와 294K에서 각각 2.380 eV와 2.260eV 이었다. X 값에 따른 광전류 스펙트럼은 성분이 증가함에 따라 피크가 단파장 쪽으로 이동하였으며, X 값에 따른 에너지 띠 간격의 변화는 $E_g$(X)=b+(0.8)X를 만족하는 선형적인 변화를 보였다. 외사법으로부터 구한 zincblende MgTe의 에너지 띠 간격은 4.2K와 297K에서 각각 3.18ev와 3.06eV로 주어졌다. 또한 광전류 peak는 온도가 상승함에 따라 장파장 쪽으로 이동하였으며, 100K 이상의 온도에서 온도계수 $dE_g$/dT=-(5.6~$6.1){\times}10^{-4}$eV/K 이었다.