• Journal of the Korean Institute of Electrical and Electronic Material Engineers
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• v.14 no.5
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• pp.417-422
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• 2001

The needs of new materials that substitute Si Oxide capacitor layer in high density DRAM increase. So in this paper, we choose the slim region 14/50/50 PLZT composition and fabricated thin films by PLD and estimated the characteristics for DRAM application. 14/50/50 PLZT thin films have crystallized into perovskite structure in the $600^{\circ}C$ deposition temperature and 200 mTorr Oxygen pressure. In this condition, PLZT thin films had 985 dielectric constant, storage charge density 8.17 $\mu$C/$\textrm{cm}^2$ and charging time 0.20ns. Leakage Current density was less than 10$^{-10}$ A/$\textrm{cm}^2$ until 5V bias voltage.

• Journal of the Korean Ceramic Society
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• v.44 no.8
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• pp.403-406
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• 2007

Ferroelectric Ce-doped $Bi_4Ti_3O_{12}$ (BCT) thin films were deposited by liquid delivery metal organic chemical vapor deposition (MOCVD) onto a $Pt(111)/Ti/SiO_2/Si(100)$ substrate. X-ray diffraction (XRD) and scanning electron microscopy (SEM) were used to identify the crystal structure, the surface, and the cross-section morphology of the deposited ferroelectric flims. After annealing above $640^{\circ}C$, the BCT films exhibited a polycrystalline structure with preferred (001) and (117) orientations. The BCT lam capacitor with a top Pt electrode showed a large remnant polarization ($2P_r$) of $44.56{\mu}C/cm^2$ at an applied voltage of 5 V and exhibited fatigue-free behavior up to $1.0{\times}10^{11}$ switching cycles at a frequency of 1 MHz. This study clearly reveals that BCT thin film has potential for application in non-volatile ferroelectric random access memories and dynamic random access memories.

• Electrical & Electronic Materials
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• v.7 no.1
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• pp.57-63
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• 1994

Aluminum oxide($Al_2{O_3}$) offers some unique advantages over the conventional silicon dioxide( $SiO_{2}$) gate insulator: greater resistance to ionic motion, better radiation hardness, possibility of obtaining low threshold voltage MOS FETs, and possibility of use as the gate insulator in nonvolatile memory devices. We have undertaken a study of the dielectric breakdown of $Al_2{O_3}$ on Si deposited by GAIVBE technique. In our experiments, we have varied the $Al_2{O_3}$ thickness from 300.angs. to 1400.angs. The resistivity of $Al_2{O_3}$ films varies from 108 ohm-cm for films less than 100.angs. to 10$_{13}$ ohm-cm for flims on the order of 1000.angs. The flat band shift is positive, indicating negative charging of oxide. The magnitude of the flat band shift is less for negative bias than for positive bias. The relative dielectric constant was 8.5-10.5 and the electric breakdown fields were 6-7 MV/cm(+bias) and 11-12 MV/cm (-bias).

• Journal of the Korean Ceramic Society
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• v.35 no.7
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• pp.647-647
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• 1998

(La,Sr)CoO3/Pb(Zr,Ti)O3/(La,Sr)CoO3 (LSCO) heterostructures have been grown on LaAlO3 substrates by pulsed laser deposition (PLD) to investigate asymmetric polarization of Pb(Zr,Ti)O3 (PZT) thin flims with different electrode configuration. P-V hysteresis loop of LSCO/PZT/LSCO was symmetric. However, LaCoO3 (LCO_/PZT/LSCO showed a largely asymmetric P-V hystersis loop and large relaxation of the remanent polarization at the negatively poled state, which means that the negatively poled state was unstable. On the other hand, LSCO/PZT/LCO exhibited large relaxation of the positively poled state. The asymmetric behavior of the polarized states implies the presence of an interal electric firld inside the PZT layer. It is suggested that internal electric field is caused by built-in voltages at LCO/PZT and LSCO/PZT interfaces. The built-in voltages at LCO/PZT and CSCO/PZT interfaces were 0.6 V and -0.12 V, respectively.