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도시홍,이우교,홍시영,방신응,강갑중,김도성,김완,강희동,Doh, S.H.,Lee, W.G.,Hong, S.Y.,Bang, S.W.,Kang, K.J.,Kim, D.S.,Kim, W.,Kang, H.D. 한국센서학회 1998 센서학회지 Vol.7 No.4
Czochralski 방법을 사용하여 격자결함이 적은 CsI 단결정 섬광체를 육성하기 위한 최적육성조건을 구하기 위하여 광투과율의 변화와 열형광특성을 이용하였다. 결정화과정을 반복할수록 불필요한 불순물 분포와 열형광강도 및 glow 피이크의 수가 감소하였다. 결정성장방향은 (110)이었고, 육성한 CsI의 결정구조는 체심입방체이었다. 그리고 격자상수는 $4.568{\AA}$ 임을 확인할 수 있었다. CsI:3rd의 활성화 에너지(trap깊이)는 약 0.45 eV 이었고, 주파수인자는 $5.18{\times}10^5\;sec^{-1}$이었다. Changes in transmission and thermoluminescent characteristics were used in order to find out the optimum growth condition of CsI single crystal scintillators which were made relatively defect-free using Czochralski method. Impurity distribution in the crystals and the intensity and number of thermoluminescent glow peaks decreased as the process of crystallization was repeated. The direction of crystal growth turned out to be (110), the crystal structure of grown CsI was bee, and its lattice constant was found to be $4.568{\AA}$. The activation energy (trap depths) of CsI:3rd was 0.45 eV and its frequency factor was $5.18{\times}10^5\;sec^{-1}$.
LiF:Mg,Cu,P TLD 의 잠상퇴행과 열처리 특성
도시홍,이우교,유명진,강희동,김도성 ( Sih Hong Doh,Woo Gyo Lee,Myung Jin Yoo,Hee Dong kang ) 한국센서학회 1998 센서학회지 Vol.7 No.5
The thermal annealing, reusability and fading characteristics of the highly sensitive LiF:Mg,Cu,P TLDs are investigated. Thermoluminescent sensitivity of the fabricated LiF:Mg,Cu,P TLD is 25.3 times higher than the commercial dosimeter TLD-700(Harshaw Chemical Co.). The main dosimetric peak shows no fading for 1 month at room temperature and 50% for 7 days at 100 ℃. The thermal annealing characteristics is examined in the temperature range from 260 ℃ to 320 ℃. For annealing the TLD at 280 ℃ for 10 minutes, TLDs can be reusable by recovering the initial sensitivity.
SrCI_2:Eu^2+ 형광체의 광발광 및 광자극발광 특성
도시홍,서효진,김영국,김도성,김성환,김찬중,이병화,김완,강희동 한국센서학회 2002 센서학회지 Vol.11 No.6
고상반응법으로 SrCl_2:Eu^2+ 형광체를 제작하고, 제작한 형광체의 광자극발광과 광발광 특성을 조사하였다. SrCl_2:Eu^2+ 형광체와 광발광 및 광자극발광은 Eu^2+ 의 5d->4f 천이에 기인되었으며, 355 nm의 광으로 여기시켰을 때 광자극발광과 광발광 스펙트럼의 파장범위는 모두 380~440nm이었고, 피이크 파장은 407nm이었다. SrCl_2:Eu^2+형광체의 선량의존성은 2.5 mGy~200mGy영역에서 우수한 선형성을 나타내었으며, 상온에서 광자극발광의 fading은 20분에 60%이었다. SrCl_2:Eu^2+ phosphors were prepared by the solid phase reaction method, and their photostimulated luminescence(PSL) and photoluminescence(PL) characteristics were investigated. The PSL and PL peak of the SrCl_2:Eu^2+ phosphors are due to the 5d->4f transition of Eu^2+ ions in phosphors. The PSL and PL spectrum obtained by the 355 nm exitation was observed in 380~440 nm region with the peak at 407 nm. The dose response of the PSL phosphors were linear within 2.5 mGy ~ 200 mGy of 100kV X-ray. The fading of the phosphors at room temperature was approximately 60% after 20 min.
도시홍,이우교,오문영,정용조,강갑중,김도성,김완,강희동 경북대학교 센서기술연구소 1998 센서技術學術大會論文集 Vol.9 No.1
CsI(Ag) single crystals doped with 0.001, 0.003 and 0.005 mole % silver as activator were grown using the Czochralski method. The gamma ray energy spectrum is measured by the CsI(Ag) single crystals coupled to photomultiflier tube. It was confirmed that the crystal structure of grown CsI(Ag) was bcc, and that its lattice constant was 4.568Å. The energy resolution of CsI(Ag) for Cs-137 gamma ray was maximum when CsI(Ag) was doped 0.003 mole % silver, and its value was 9.84% the pulse height from the scintillation detector system using the CsI(Ag) single crystals was linear to gamma ray energy.
BaFBr:Eu^2+ 형광체의 열발광 및 광자극발광 특성
도시홍,서효진,강갑중,김영국,김도성,김성환,김찬중,이병화,김완,강희동 한국센서학회 2002 센서학회지 Vol.11 No.5
BaFBr:Eu^2+ 형광체를 제조하고, 이 형광체의 열발광 특성과 광자극발광 특성을 조사하였다. 이 형광체의 열발광 g1ow 피이크 온도는 352K와 448K였으며, 주 피이크(352K)에 관여하는 트랩의 활성화에너지는 약 0.96eV이었다. 또한 이 형광체의 광자극발광 스펙트럼의 파장범위는 350~450nm 사이였으며, 광자극발광에 기여하는 트랩의 활성화에너지는 약 0.98eV이었다. 열발광트랩과 광자극발광 트랩의 활성화에너지는 실험오차 내에서 일치하였다. BaFBr:Eu^2+ phosphors were prepared, and the thermoluminescence(TL) and photostimulatedluminescence(PSL) of the prepared phosphors were measured. Two glow peaks around 352 and 448 K are observed for x-ray irradiated BaFBr:Eu^2+ phosphors, and the activation energy of the main glow peak(352 K) was about 0.96 eV. The spectral range of the PSL was 350 ~450 nm, and the activation energy of the trap giving rise to PSL was about 0.98 eV. The activation energy of the traps giving rise to TL is agreed to those giving rise to PSL within experimental error.