• 한국전기전자재료학회:학술대회논문집
• /
• 한국전기전자재료학회 2007년도 하계학술대회 논문집 Vol.8
• /
• pp.140-141
• /
• 2007

To fabricate the metal-ferroelectric-insulator-semiconductor (MFIS) structure for the ferroelectric random access memory (FRAM) application, we prepared the ferroelectric $Sr_{0.9}Bi_{2.1}Ta_2O_9$ (SBT) and the insulator LaZrOx (LZO) thin films on the silicon substrate using a sol-gel method. In this study, we will investigate the feasibility of the SBT/LZO/Si structure as one of the promising gate configuration for the 1-transistor (1-T) type FRAM, by measurements of the electrical properties and the physical properties.

• 한국전기전자재료학회:학술대회논문집
• /
• 한국전기전자재료학회 1999년도 추계학술대회 논문집
• /
• pp.433-436
• /
• 1999

In this paper we applied TVS(Triangular Voltage Sweep) method to calculate the mobile ionic charge densities in some ferroelectric thin films. During the measurement, the temperature of specimens were maintained at 20$0^{\circ}C$. By this method, the amount of mobile ionic charge Q$_{m}$ and mobile ionic charge density N$_{m}$ of a MFIS structure were calculated 3.5 [pC] and about 4.3$\times$10$^{11}$ [ions/cm$^2$], respectively. In order to successful TVS measurement, the gate leakage current density of films must be low 10$^{-9}$ (A/cm$^2$) order.der.

• 한국전기전자재료학회:학술대회논문집
• /
• 한국전기전자재료학회 2009년도 하계학술대회 논문집
• /
• pp.140-140
• /
• 2009

The Metal-ferroelectric-semiconductor (MFS) structure has superior advantages such as high density integration and non-destructive read-out operation. However, to obtain the desired electrical characteristics of an MFS structure is difficult because of interfacial reactions between ferroelectric thin film and Si substrate. As an alternative solution, the MFS structure with buffer insulating layer, i.e. metal-ferroelectric-insulator-semiconductor (MFIS), has been proposed to improve the interfacial properties. Insulators investigated as a buffer insulator in a MFIS structure, include $Ta_2O_5$, $HfO_2$, and $ZrO_2$ which are mainly high-k dielectrics. In this study, we prepared the Dy-doped $La_2O_3$ solution buffer layer as an insulator. To form a Dy-doped $La_2O_3$ buffer layer, the solution was spin-coated on p-type Si(100) wafer. The coated Dy-doped $La_2O_3$ films were annealed at various temperatures by rapid thermal annealing (RTA). To evaluate electrical properties, Au electrodes were thermally evaporated onto the surface of the samples. Finally, we observed the surface morphology and crystallization quality of the Dy-doped $La_2O_3$ on Si using atomic force microscopy (AFM) and x-ray diffractometer (XRD), respectively. To evaluate electrical properties, the capacitance-voltage (C-V) and current density-voltage (J-V) characteristics of Au/Dy-doped La2O3/Si structure were measured.

• 한국전기전자재료학회:학술대회논문집
• /
• 한국전기전자재료학회 2009년도 하계학술대회 논문집
• /
• pp.80-80
• /
• 2009

Recently, multiferroics have attracted much attention due to their numorous potentials. In this work, we attemped to utilize the multiferroics as an alternative material for ferroelectrics. Ferroelectric materials have been stadied to ferroelectric random access memories, however, some inevitable problems prevent it from inplementation. multiferroics shows a ferroelectricity and has low process temperature $BiFeO_3$(BFO) films have good ferroelectric properties but poor leakage characterization. Thus we tried, in this work, to adopt $HfO_2$ insulating layer for metal-ferroelectric-insulator-semiconductor(MFMIS) structure to surpress to leakage current. $BiFeO_3$(BFO) thin films were fabricared by using a sol-gel method on $HfO_2/Si$ structure. Ferroelectric BFO films on a p-type Si(100)wafer with a $HfO_2$ buffer layer have been fabricated to form a metal-ferroelectric-insulator-semiconductor (MFIS) structure. The $HfO_2$ insulator were deposited by using a sol-gel method. Then, they were carried out a rapid thermal annealing(RTA) furnace at $750\;^{\circ}C$ for 10 min in $N_2$. BFO films on the $HfO_2/Si$ structures were deposited by sol-gel method and they were crystallized rapid thermal annealing in $N_2$ atomsphere at $550\;^{\circ}C$ for 5 min. They were characterized by atomic force microscopy(AFM) and Capacitance-voltage(C-V) curve.

• 한국세라믹학회지
• /
• 제42권9호
• /
• pp.624-630
• /
• 2005

To investigate the possibility of the $ZrO_2$ buffer layer as the insulator for the Metal-Ferroelectric-Insulator-semiconductor (MFIS) structure, $ZrO_2$ and $SrBi_2Ta_2O_9$ (SBT) thin films were deposited on the P-type Si(111) wafer by the R.F. magnetron-sputtering method. According to the process with and without the post-annealing of the $ZrO_2$ buffer layer and SBT thin film, the diffusion amount of Sr, Bi, Ta elements show slight difference through the Glow Discharge Spectrometer (GDS) analysis. From X-ray Photoelectron Spectroscopy (XPS) results, we could confirm that the post-annealing process affects the chemical binding condition of the interface between the $ZrO_2$ thin film and the Si substrate. Compared to the MFIS structure without the post-annealing of the $ZrO_2$ buffer layer, memory window value of MFlS structure with post-annealing of the $ZrO_2$ buffer layer were considerably improved. The window memory of the Pt/SBT (260 nm, $800^{\circ}C)/ZrO_2$ (20 nm) structure increases from 0.75 to 2.2 V under the applied voltage of 9 V after post-annealing.

• 한국정보전자통신기술학회논문지
• /
• 제17권2호
• /
• pp.108-112
• /
• 2024

회내족은 넙다리두갈래근의 활성화를 증가시키거나 근피로 또는 과사용증후군(overuse syndromes)을 초래한다. 본 연구에서는 회내각(pronation angles)이 20° 이상인 회내족 피험자를 대상으로 회내각과 근피로지수와의 관계를 파악하는 것이다. 나이 범위가 15-61세인 12명의 피험자가 실험에 참여하였으며, 30초 동안 4.5 km/h의 속도로 트레드밀 보행시 넙다리두갈래근의 근전도를 측정하여 근피로지수인 중앙주파수와 저주파수 대역 크기의 기울기를 산출하였다. 본 연구에 참여한 피험자로부터 산출한 두 가지 근피로지수와 회내각 사이의 관계가 정상인과 유사할 것이라는 가정 하에 실험한 결과, 근피로지수와 회내각 사이의 유의한 상관성을 얻을 수 있었다 (r>0.60; p<0.05).

• 한국진공학회지
• /
• 제7권3호
• /
• pp.195-200
• /
• 1998

본 연구에서는 강유전체 박막의 게이트 산화물로 사용한 $Pt/SrBi_2Ta_2O_9(SBT)/CeO_2/Si(MFS)$와 Pt/SBT/Si(MFS) 구조의 결정 구조 및 전기적 성질 의 차이를 연구하였다. XRD 및 SEM 측정 결과 SBT/$CeO_2$/Si박막은 약5nm정도의 $SiO_2$층 이 형성되었고 비교적 평탄한 계면의 미세구조를 가지는 반면, SBT/Si는 각각 약6nm와 7nm정도의 $SiO_2$층과 비정질 중간상층이 형성되었음을 알 수 있다. 즉 CeO2 박막을 완충층 으로 사용함으로써 SBT박막과 Si기판의 상호 반응을 적절히 억제할 수 있음을 확인하였다. Pt/SBT/$CeO_2/Pt/SiO_2$/와 Pt/SBT/Pt/$SiO_2$/Si구조에서 Polarization-Electric field(P-E) 특 성을 비교해 본 결과 CeO2박막의 첨가에 따라 잔류분극값은 감소하였고 항전계값은 증가하 였다. MFIS구조에서 memory window값은 항전계값과 직접적 관련이 있으므로 이러한 항 전계값의 증가는 MFIS구조에서의 memory window값이 증가할 수 있음을 나타낸다. Pt-SBT(140nm)/$CeO_2$(25nm)/Si구조에서 Capacitance-Voltage(C-V) 측정 결과로부터 동작 전압 4-6V에서 memory wondows가 1-2V정도로 나타났다. SBT박막의 두께가 증가할수록 memory window값은 증가하였는데 memory wondows가 1-2V정도로 나타났다. SBT박막의 두께가 증가할수록 memory window값은 증가하였는데 이는 SBT박막에 걸리는 전압강하가 증가하기 때문인 것으로 생각되어진다. Pt/SBT/$CeO_2$/Si의 누설전류는 10-8A/cm2정도였고 Pt/SBT/Si 구조에서는 약10-6A/cm2정도로 약간 높은 값을 나타내었다.

• 한국재료학회:학술대회논문집
• /
• 한국재료학회 2001년도 춘계학술발표강연 및 논문개요집
• /
• pp.94-94
• /
• 2001

• 한국재료학회:학술대회논문집
• /
• 한국재료학회 1998년도 IUMRS-ICEM ABSTRACT BOOK
• /
• pp.64.1-64
• /
• 1998

• 한국재료학회:학술대회논문집
• /
• 한국재료학회 1998년도 IUMRS-ICEM ABSTRACT BOOK
• /
• pp.133.4-133
• /
• 1998