• Title/Summary/Keyword: RTA temperature

Search Result 243, Processing Time 0.026 seconds

Effect of RTA temperature on the leakage current characteristics of PZT thin films (RTA 온도가 PZT 박막의 누설전류에 미치는 영향)

  • 김현덕;여동훈;임승혁;송준태
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
    • /
    • 2001.07a
    • /
    • pp.709-712
    • /
    • 2001
  • The effects of post annealing temperature by the Rapid Thermal Annealing(RTA) on the electrical properties of Pb(Zr,Ti)O$_3$(PZT) thin film were investigated. Analyses by the RTA treatments reveled that the leakage current of PZT thin films strongly depend on heating temperature and time. It was found that leakage current properties of PZT capacitor were changed by heating temperature during the RTA annealing. On Pt/Ti/Si substrates, PZT films are deposited at 350 $^{\circ}C$ by rf magnetron sputtering. The X-ray diffusion (XRD) was confirmed the formation of PZT thin film. Leakage current characteristics were improved with decreasing the post annealing temperature of PZT thin film. RTA annealed film on the 700$^{\circ}C$ shows ferroelectric and electrical properties with a remanent polarization of 12.4${\mu}$C/$\textrm{cm}^2$ coercive field of 117kV/cm, leakage current J= 6.2${\times}$10$\^$-6/ A/$\textrm{cm}^2$

  • PDF

RTA Post-treatment of Thermal T${a_2}{O_5}$ Thin Films (열산화 T${a_2}{O_5}$박막에 미치는 RTA후처리의 영향)

  • Mun, Hwan-Seong;Lee, Jae-Seok;Han, Seong-Uk;Park, Sang-Gyun;Yang, Seung-Ji;Lee, Jae-Cheon;Park, Jong-Wan
    • Korean Journal of Materials Research
    • /
    • v.3 no.3
    • /
    • pp.310-315
    • /
    • 1993
  • The effects of RT A treatment on the breakdown strengths were studied for tantalum pentoxide(${Ta_2}{O_5}$) films prepared by thermal oxidation of dc-sputtered Ta(400$\AA$) on p-type (100) Si wafer. While the relative dielectric constants of the RT A -treated specimens were not remarkably affected, the breakdown strengths of the RTA-treated specimens were greatly changed by RTA temperature and time. After the RTA treatment, the breakdown strengths of the specimens RTA-treated at the temperature below the crystallization temperature were increased to 5.4MV /cm, while those of the specimens RTA -treated at the temperature above it were decreased to 0.5MV /cm. RTA time-independence of the flat-bant voltage shift refleted that the RT A post-annealing effects on the breakdown strengths were not due to the interface reaction between the ${Ta_2}{O_5}$ layer and the Si substrate but, through the RBS analysis, to densification of the ${Ta_2}{O_5}$ films.

  • PDF

Dependence of luminescence property of ZnMgS:Mn thin film phosphor on RTA temperature (ZnMgS:Mn 박막 형광체의 RTA 온도 변화에 따른 발광 특성 의존성)

  • Lee, Dong-Chin;Yun, Sun-Jin;Jeon, Duk-Young
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
    • /
    • 2004.05a
    • /
    • pp.102-105
    • /
    • 2004
  • With varying rapid thermal annealing (RTA) temperature, luminescent properties of ZnMgS:Mn thin film sputter-deposited with one target were measured. Although all samples have the same composition, $Zn_{1-x}Mg_xS:Mn$ (x=0.25) can emit luminescence between 580 and 614 nm, which is controlled by only RTA temperature. It is understood that the energy band gap shift of ZnMgS:Mn thin film phosphor occurs with varying RTA temperature.

  • PDF

Effects of Rapid Thermal Annealing Temperature on Performances of Nanoscale FinFETs

  • Sengupta, M.;Chattopadhyay, S.;Maiti, C.K.
    • JSTS:Journal of Semiconductor Technology and Science
    • /
    • v.9 no.4
    • /
    • pp.266-272
    • /
    • 2009
  • In the present work three dimensional process and device simulations were employed to study the performance variations with RTA. It is observed that with the increase in RTA temperature, the arsenic dopants from the source /drain region diffuse laterally under the spacer region and simultaneously acceptors (Boron) are redistributed from the central axis region of the fin towards the Si/SiO2 interface. As a consequence both drive current and peak cut-off frequency of an n-FinFET are observed to improve with RTA temperatures. Volume inversion and hence the flow of carries through the central axis region of the fin due to reduced scattering was found behind the performance improvements with increasing RTA temperature.

RTA system design modeling to reduce slip (Slip 현상을 줄이기위한 RTA(고속열처리) 장치 설계모델링)

  • Jang, Hyeon-Yong;Hang, Seung-Yun;Hwang, Ho-Jung
    • Proceedings of the KIEE Conference
    • /
    • 1988.07a
    • /
    • pp.379-382
    • /
    • 1988
  • In this paper optimal light source arraies are calculated to reduce slips in RTA process. A two-channel temperature controller is constructed on a board using IBM - XT to improve the temperature uniformity. The proposed RTA structure has also advantage of power dissipation.

  • PDF

The Growth and Its Characteristics of Low Temperature (LT. $250^{\circ}C$) GaAS Epilayer (Low Temperature (LT) GaAs 에피층의 성장과 그 특성연구)

  • 김태근;박정호;조훈영;민석기
    • Journal of the Korean Institute of Telematics and Electronics A
    • /
    • v.31A no.9
    • /
    • pp.96-103
    • /
    • 1994
  • The GaAs epilayer was grown at low temperature (LT. 250.deg. C) by molecular beam epitaxy. The properties of the LTT GaAs, before and after Rapid Thermal Annealing(RTA), were analyzed by Reflection of High Energy Electron Diffraction (RHEED), Double Crystal X-ray(DCX), Raman spectroscopy, PL and Photo-Induced Current Transient Spectroscopy (PICTS). The LT GaAs before RTA, was analyzed by RHEED and DCX, with a result of an improved surface morphology under a relatively As-rich(As/Ga ratio :28) condition, and of an increased lattics parameter of 1.1 1.7% in comparison with a GaAs substrate. However DCX and Raman spectroscopy revealed that the expanded lattics parameter and the crystallinity of LT GaAs could be recovered after RTA. On the other hand, PL spectra indicated that LT GaAs after RTA showed low optical sensitivity unlike High Temperature(HT) GaAs, and that its surface morphology and crystallinity were corresponded with those of HT GaAs. Finally PICTS spectra proved the fact that low sensitivity of LT GaAs was due to the deep level defects (Ec-0.85eV) which were strogly formed by raising RTA temperature to 750.deg. C.

  • PDF

In-doping effects on the Structural and Electrical Properties of ZnO Films prepared by Ultrasonic Spray Pyrolysis (초음파 분무 열분해법으로 제초한 ZnO막의 전기적, 구조적 특성에 미치는 In첨가 효과)

  • 심대근;양영신;마대영
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
    • /
    • 2001.07a
    • /
    • pp.1010-1013
    • /
    • 2001
  • Zinc oxide(ZnO) films were prepared by ultrasonic spray pyrolysis on indium (In) films deposited by evaporation and subsequently submitted to rapid thermal annealing (RTA). The RTA was processed in air or a vacuum ambient. The crystallographic properties and surface morphologies of the films were characterized before and after the RTA by X-ray diffraction (XRD) and scanning electron microscopy(SEM), respectively. The resistivity variation of the films with RTA temperature and time was measured by the 4-point probe method. Auger electron spectroscopy(AES) was carried out to figure out the distribution of indium atoms in the ZnO films. The resistivity of the ZnO on In(ZnO/In) films decreased to 2${\times}$10$\^$-3/ $\Omega$cm by diffusion of the In. The In diffusion into the ZnO films roughened the surface of the ZnO films. The results of depth profile by AES showed a hump of In atoms around ZnO/In interface after the RTA at 800$^{\circ}C$, which disappeared by the RTA at 1000$^{\circ}C$. The effects of temperature, time and ambient during the RTA on the structural and electrical properties of the ZnO/In films were discussed.

  • PDF

Effects of Rapid Thermal Annealing on Thermal Stability of FeMn Spin Valve Sensors

  • Park, Seung-Young;Choi, Yeon-Bong;Jo, Soon-Chul
    • Journal of Magnetics
    • /
    • v.10 no.2
    • /
    • pp.52-57
    • /
    • 2005
  • In this research, magnetoresistance (MR) ratio (MR), resistivity, and exchange coupling field $(H_{ex})$ behaviors for sputter deposited spin valves with FeMn antiferromagnetic layer have been extensively investigated by rapid thermal annealing (RTA) as well as conventional annealing (CA) method. 10 s of RTA revealed that interdiffusion was not significant up to $325^{\circ}C$ at the interfaces between the layers when the RTA time was short. The MR of FeMn spin valves were reduced when the spin valves were exposed to temperature of $250^{\circ}C$, even for a short time period of 10 s prior to CA. $H_{ex}$ was maintained up to $325^{\circ}C$ of CA when the specimen was subjected to 10 s of RTA at $200^{\circ}C$ prior to CA, which is $25^{\circ}C$ higher than the result obtained from the CA without prior RTA. Therefore, the stability of $H_{ex}$ could be enhanced by a prior RTA before performing CA up to annealing temperature of $325^{\circ}C$. MR and sensitivity of the specimens annealed without magnetic field up to $275^{\circ}C$ were recovered to the values prior to CA, but $H_{ex}$ was not recovered. This means that reduced MR sensitivity and MR during the device fabrication can be recovered by a field RTA.

Effect of Pb Content on the Phase Transformation of Sputter-Deposited PZT Thin Film During RTA (PZT 박막의 급속열처리시 Pb 함량이 상변태에 미치는 영향)

  • 주재현;길덕신;주승기
    • Journal of the Korean Ceramic Society
    • /
    • v.30 no.10
    • /
    • pp.803-810
    • /
    • 1993
  • PbxZr0.4Ti0.6O3 thin films were prepared by reactive co-sputtering and annealed by RTA(Rapid Thermal Annealing) process. Effect of Pb content in PbxZr0.4Ti0.6O3 films on the phase transformation was intensively studied. It has been found out that depending on the Pb content as well as RTA temperature, crystal structure of PbxZr0.4Ti0.6O3 films change greatly. It turned out that transformation temperature for perovskite can be lowered and the width of transition temperature region was reduced by increasing Pb content in the film. And the lattice was expanded with increasing Pb content. With increasing RTA temperature, as-deposited phase was transformed into perovskite through three different transformation paths depending on Pb content. It was confirmed that activation energies for nucleation of perovskite structure are much larger than those of its growth.

  • PDF

The Formation of the Shallow Junction by RTD and Characteristic Analysis for $n^+$ -p Diode with Ti-silicide (고속 열 확산에 의한 얕은 접합 형성과 Ti-실리시이드화된 $n^+$ -p 다이오드 특성 분석)

  • 최동영;이성욱;주정규;강명구;윤석범;오환술
    • Journal of the Korean Institute of Telematics and Electronics A
    • /
    • v.31A no.8
    • /
    • pp.80-90
    • /
    • 1994
  • The ultra shallow junction was formed by 2-step RTP. Phosphorus solid source(P$_{2}O_{5}$) was transfered on wafer surface during RTG(Rapid Thermal Glass Transfer) of which process condition was 80$0^{\circ}C$ and 60sec. The process temperature and time of the RTD(Rapid Thermal Diffusion) were 950~105$0^{\circ}C$ during 5~15sec respectively sheet resistances were measured as 175~320$\Omega$/m and junction depth and dopth and dopant surface concentration were measured as 0.075~0.18$\mu$m and 5${\times}10^{19}cm^{4}$ respectively. Ti-silicide was formed by 2-step RTA after 300$\AA$ Titanium was deposited. The 1st RTA (2nd RTA) was carried out at the temperature of $600^{\circ}C$(700~80$0^{\circ}C$) for 30 seconds (10~60 seconds) under N$_2$ ambient. Sheet resistances after 2nd RTA were measured as 46~63$\Omega$/D. Si/Ti component ratio was evaulated as 1.6~1.9 from Auger depth profile. Ti-Silicided n-p junction diode (pattern size : 400$\times$400$\mu$m) was fabricated under the RTD(the process was carried out at the temperature of 100$0^{\circ}C$ for 10seconds) and 2nd RTA(theprocess was carried out at the temperature of 750$^{\circ}C$ for 60 seconds). Leakage current was measured 1.8${\times}10^{7}A/mm^{2}$ at 5V reverse voltage. Whent the RTD process condition is at the temperature of 100$0^{\circ}C$ for 10seconds and the 2nd RTA process condition is at the temperature of 75$0^{\circ}C$ for 60 seconds leakage current was 29.15${\times}10^{9}A$(at 5V).

  • PDF