• Journal of the Korean Vacuum Society
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• v.18 no.5
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• pp.358-364
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• 2009

We investigated the growth of ZnO thin films with prominent emission characteristics through minimizing the formation of defects by using pulsed laser deposition (PLD). To do so, the ZnO films were deposited on sapphire(0001) substrates at the substrate temperature of $400-850^{\circ}C$ and then the variation of their structural and optical properties were analyzed by x-ray diffraction, atomic force microscope and photoluminescence. As a result, all ZnO films were grown with c-axis preferential orientation irrespective of the substrate temperature. However, the crystallinity and stress state were dependent on the substrate temperature and the ZnO film deposited at $600^{\circ}C$ showed the best surface morphology and crystallinity with nearly no strain. And also this film exhibited outstanding emission characteristics from the viewpoint of full width half maximum of UV emission peak as well as visible emission due to defects. These results indicate that the emission characteristics of the ZnO films are strongly related to their structural characteristics influenced by substrate temperature. Consequently, ZnO films with strong UV emission and nearly no visible emission, which are applicable to UV emission devices, could be grown at the substrate temperature of $600^{\circ}C$ by PLD.

• Proceedings of the KIEE Conference
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• 1997.07d
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• pp.1236-1238
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• 1997

유전체 PLT(28) ($Pb_{0.72}La_{0.28}Ti_{0.93}O_3$) 박막을 레이저 어블레이션 기법으로 Pt/Ti/$SiO_3$/Si기판을 $500^{\circ}C{\sim}700^{\circ}C$까지 가열한 상태에서 $O_2$분위기에서 증착시켰다. 증착된 박막은 SEM, XRD 등의 구조적 분석을 통하여 $600^{\circ}C$이상에서 증착된 경우, (111)방향으로 우세하게 성장한, 결정성이 양호한 박막임을 확인하였다. 박막의 전기적 특성은, 증착 온도가 $650^{\circ}C$일 때 약 1400정도의 높은 비유전율을 얻었으며, 전하저장밀도는 100[KV/cm]에서 약 9[${\mu}C/cm^2$]이었다.

• Proceedings of the Korean Vacuum Society Conference
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• 2000.02a
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• pp.68-68
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• 2000

펄스레이저 증착법(이하 PLD)을 이용하여 마이크로파 유전체 소자 및 절연 산화막으로의 응용을 위한 MgTiO3 박막을 다양한 기판상에서 증착하였다. 사파이어 기판에 (a,c-plane Al2O3) 성장된 MgTiO3 박막은 에피텍셜 성장(epitaxial growth)이 되었으며, SiO2/Si 및 Pt/Ti/Si 기판위세 성장된 MgTiO3 박막의 경우 003방향으로 배향(oriented) 되었다. MgTiO3 박막은 450~75$0^{\circ}C$까지 기판온도를 변화시키면서 증착시켰으며, 증착시 산소분압은 50~200 mTorr로 변화시켰다. PLD 증착시 타켓에 조사된 레이저 에너지 밀도는 약 2J/cm2였으며, MgTiO3 박막 증착후 200Torr O2 분위기에서 상온까지 1$0^{\circ}C$/min 의 속도로 냉각시켰다. 사파이어 c-plane 상에서 일머나잇(ilminite) MgTiO3 구조가 55$0^{\circ}C$ 에피텍셜 성장하는 것을 관찰할 수 있었으며, 사파이어 a-plane 상에서는 MgTiO3 구조가 $650^{\circ}C$ 이상부터 110방향으로 배향되며 성장하였다. $600^{\circ}C$ 이상에서 c-축으로 배향된 구조를 갖고 있었다. 증착된 MgTiO3 박막의 조성분석(stoichio metric analysis)을 위해 RBS 분석을 수행하여, 증착에 이용된 타켓과 동일한 조성을 갖는 MgTiO3 박막이 성장된 것을 확인할 수 있었다. 사파이어 기판상에 증착된 MgTiO3 박막은 가시영역에서 투명하였으며, 약 270nm 파장을 갖는 영역에서 급격한 흡수단을 보였다. 이때의 MgTiO3 박막은 AFM 분석을 통해 약 0.87mn rms roughness 값을 갖는 매우 평탄한 표면구조를 갖고 있는 것을 확인하였다. MIM(Pt/MgTiO3/Pt) 구조의 캐패시터를 형성시켜 MgTiO3 박막의 유전특성(dielectric properties)을 관찰하였다. PLD로 성장된 MgTiO3 박막의 유전율(relative dielectric constant)은 약 22였으며, 1MHz에서 약 1.5%의 유전손실(dielectirc loss) 값을 보였다. 또한 이때 MgTiO3 박막은 낮은 유전분산값을 보였다.

• Proceedings of the Korean Ceranic Society Conference
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• 2004.10a
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• pp.79.2-79.2
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• 2004

• Journal of the Korean Vacuum Society
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• v.9 no.3
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• pp.249-253
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• 2000

We have analyzed electrical characteristics of the amorphous $MgTiO_3$thin films deposited by pulsed laser deposition (PLD) technique with the temperature of 400~$500^{\circ}C$. The electrical characteristics of $MgTiO_3$films heavily depend on the deposition temperature. We speculate that the density of anomalous positive charge (APC) substantially increases as the deposition temperature lowers, causing the HF C-V curves shift to the direction of the negative gate voltage. We further observed that both the degree of C-V shift as a function of the deposition temperature and the density of APC were minimized by the use of $SiO_2$with thickness of approximately 100 $\AA$ between $MgTiO_3$films and the Si substrate.

• Proceedings of the Korean Magnestics Society Conference
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• 2004.12a
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• pp.156-157
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• 2004

• The Transactions of The Korean Institute of Electrical Engineers
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• v.59 no.1
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• pp.113-115
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• 2010

In this study, ZnO films have been grown on PES(polyethersu]fone) substrate by PLD(pulsed laser deposition) and characterized as a change of laser density and substrate temperature. Growing conditions were changed with substrate temperatures ranging from 50 to $200^{\circ}C$ and laser densities ranging from $0.2\sim0.4 J/cm^2$. Optical and structural properties were measured by XRD, SEM, AFM, PL measurement.

• Proceedings of the Korean Vacuum Society Conference
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• 2009.08a
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• pp.137-137
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• 2009

• Journal of Sensor Science and Technology
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• v.7 no.1
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• pp.61-66
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• 1998

High quality c-axis oriented $YBa_{2}Cu_{3}O_{7}$ films were prepared using the pulsed laser deposition on $SrTiO_{3}$(100) substrate. The atomically smooth $SrTiO_{3}$surface with terraces one unit cell in height could be obtained by a high temperature annealing. $YBa_{2}Cu_{3}O_{7}$ thin films deposited on the substrates exhibited layer-by-layer growth with a c-axis unit cell height. $YBa_{2}Cu_{3}O_{7}$ thin films thus prepared showed critical temperature ${\ge}90$ K with transition width ${\le}0.6$ K, room temperature resistivity of ${\sim}300{\mu}{\Omega}cm$, and critical current density ${\sim}4.6{\times}10^{6}A/cm^{2}$ at 77 K.

• Journal of the Korean Vacuum Society
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• v.7 no.4
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• pp.355-360
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• 1998

Epitaxial $Ba_{0.5}Sr_{0.5}TiO_3$thin films of two different thickness (~250 $\AA$ and ~1340 $\AA$) on MgO(001) prepared by a pulsed laser deposition method were studied by synchroton x-ray scattering measurements. The film initially grew on MgO(001) with a cube-on-cube relationship, maintaining it during further growth. As the film grew, the surface of the film became rough significantly, but the interface between the film and the substrate seemed to have changed little. In the early stage, the film was highly strained in a tetragonal structure with the longer axis parallel to the surface normal direction. As the growth proceeded further, it was mostly relaxed to a cubic structure with the lattice parameter of the bulk value and the mosaic distribution improved significantly in both in-plane and out-of-plane directions.