• Title/Summary/Keyword: RTA annealing

Search Result 391, Processing Time 0.03 seconds

Annealing-temperature Dependent Characteristics of PLZT Thin Films on ITO Coated Glass (ITO 기판에 제작된 PLZT 박막의 소성온도에 따른 특성)

  • Choi, Hyung-Wook;Jang, Nak-Won;Park, Chang-Yub
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
    • /
    • v.11 no.2
    • /
    • pp.128-132
    • /
    • 1998
  • 2/65/35 PLZT stock solution prepared by Sol-Gel processing was spin-coated on ITO coated glass and annealed by RTA(Rapid Thermal Annealing). The crystal structure of films was reported based on the observation of crystallization process and microstructure of the film fabricated at different fabrication condition. Films were crystallized into rhombohedral structure by annealing at $750^{\circ}C$ for 5 min. As the annealing temperature increased, the size of rosette structure of the films was grown up from $2.4{\mu}m$ to $15{\mu}m$, dielectric constant was increased, coercive field was decreased 33.82 kV/cm, remnant polarization was increased to 39.84 ${\mu}C/cm^2$ and Optical transmittance was decreased.

  • PDF

Activation energy for the loss of substitutional carbon in $Si_{0.984}C_{0.016}$ grown by solid phase epitaxy

  • Kim, Yong-Jeong;Kim, Tae-Joon;Park, Byungwoo;Song, Jong-Han
    • Journal of Korean Vacuum Science & Technology
    • /
    • v.4 no.2
    • /
    • pp.50-54
    • /
    • 2000
  • We studied the synthesis of S $i_{1-x}$ Cx (x=0.016) epitaxial layer using ion implantation and solid phase epitaxy (SPE). The activation energy Ea was obtained for the loss of substitutional carbon using fourier transform-infrared spectroscopy (FTIR) and high-resolution x-ray diffraction (HR-XRD). In FTIR analysis, the integrated peak intensity was used to quantify the loss of carbon atoms from substitutional to interstitial sites during annealing. The substitutional carbon contents in S $i_{0.984}$ $C_{0.016}$ were also measured using HR-XRD. By dynamic simulations of x-ray rocking curves, the fraction of substitutional carbon was obtained. The effects of annealing temperature and time were also studied by comparing vacuum furnace annealing with rapid thermal annealing (RTA))))))

  • PDF

ELA Poly-Si과 SLS Poly-Si에서 Boron Activation에 관한 연구

  • Hong, Won-Ui;No, Jae-Sang
    • Proceedings of the Korean Vacuum Society Conference
    • /
    • 2012.02a
    • /
    • pp.376-376
    • /
    • 2012
  • 본 연구는 Poly-Si에 이온 주입된 Boron의 Activation 거동을 연구하고자 SLS (Sequential Lateral Solidification) Poly-Si과 ELA (Excimer Laser Annealing) Poly-Si의 활성화 거동을 비교 분석하였다. SLS 및 ELA 결정화 방법으로 제조된 Poly-Si을 모재로 비 질량 분리 방식의 ISD (Ion Shower Doping) System을 사용하여 2.5~7.0 kV까지 이온주입 하였다. 이온주입 후 두 가지의 열처리 방법, 즉, FA 열처리(Furnace Annealing)와 RTA 열처리(Rapid Thermal Annealing)를 사용하여 도펀트 활성화 열처리를 수행하고 이온주입 조건 및 활성화 열처리 방법에 따른 결함 회복 및 도펀트 활성화 거동의 변화를 관찰하였다. TRIM-code Simulation 결과 가속 이온 에너지와 조사량이 증가 할수록 이온주입 시 발생하는 결함의 양이 증가하는 것을 정량적으로 계산하였다. 실험 결과 결함의 양이 증가 할수록 Activation이 잘되는 것을 관찰할 수 있었다. SLS Poly-Si에 비하여 ELA Poly-Si의 경우 도펀트 활성화 열처리 후 활성화 효율이 높게 나타났다. 본 결과는 Grain Boundary의 역할과 밀접한 관계가 있으며 간단한 정성적인 Model을 제시하였다. 활성화 효율의 경우 RTA 열처리 시편이 FA 시편에 비하여 높은 것이 관찰되었다. 본 결과는 열처리 온도 및 시간에 따라 변화하는 Boron의 특이한 활성화 거동인 Reverse Annealing 효과에 기인하는 것으로 규명되었다.

  • PDF

Effect of rapid thermal annealing on CdS films prepared by RF magnetron sputtering

  • Hwang, Dong-Hyeon;Gam, Dae-Ung;An, Jeong-Hun;Son, Yeong-Guk
    • Proceedings of the Korean Vacuum Society Conference
    • /
    • 2010.02a
    • /
    • pp.164-164
    • /
    • 2010
  • Cds films were deposited on glass substrates using rf magnetron sputtering method followed by rapid thermal annealing(RTA). Effects of annealing temperature on surface characteristic, structural, electrical and optical property of CdS films were investigated at different temperatures ranging from 250 to $550^{\circ}C$ with various holding time. The film annealed at $450^{\circ}C$ with less than 1 min holding time is attributed to the improved crystalline quality of CdS film due to the effective relaxation of residual compressive stress and achieving maximum grain size. The results show that RTA treatments under optimal annealing condition can provide significant improvements in the properties of CdS films.

  • PDF

The Crystallinity and Electrical Properties of SrBi2Ta2O9 Thin Films Fabricated by New Low Temperature Annealing (새로운 저온 열처리 공정으로 제조된 SrBi2Ta2O9 박막의 결정성 및 전기적 특성)

  • Lee, Kwan;Choi, Hoon-Sang;Jang, Yu-Min;Choi, In-Hoon
    • Korean Journal of Materials Research
    • /
    • v.12 no.5
    • /
    • pp.382-386
    • /
    • 2002
  • We studied growth and characterization of $SrBi_2Ta_2O_9$ (SBT) thin films fabricated by low temperature process under vacuum and/or oxygen ambient. A metal organic decomposition (MOD) method based on a spin-on technique and annealing process using a rapid thermal annealing (RTA) method was used to prepare the SBT films. The crystallinity of a ferroelectric phase of SBT thin films is related to the oxygen partial pressure during RTA process. Under an oxygen partial pressure higher than 30 Torr, the crystallization temperature inducing the ferroelectric SBT phase can be lowered to $650^{\circ}C$. Those films annealed at $650^{\circ}C$ in vacuum and oxygen ambient showed good ferroelectric properties, that is, the memory window of 0.5~0.9 V at applied voltage of 3~7 V and the leakage current density of 1.80{\times}10^{-8}$ A/$\textrm{cm}^2$ at an applied voltage of 5V. In comparison with the SBT thin films prepared at 80$0^{\circ}C$ in $O_2$ ambient by furnace annealing process, the SBT thin films prepared at $650^{\circ}C$ in vacuum and oxygen ambient using the RTA process showed a good crystallization and electrical properties which would be able to apply to the virtul device fabrication precess.

Reflow of Sn Solder Bumps using Rapid Thermal Annealing(RTA) method and Intermetallic Formation (급속 열처리 방법에 의한 Sn 솔더 범프의 리플로와 금속간 화합물 형성)

  • Yang, Ju-Heon;Cho, Hae-Young;Kim, Young-Ho
    • Journal of the Microelectronics and Packaging Society
    • /
    • v.15 no.4
    • /
    • pp.1-7
    • /
    • 2008
  • We studied a growth behavior of Intermetallic compounds(IMCs) during solder bumping with two reflow methods. Ti(50 nm), Cu($1{\mu}m$), Au(50 nm) and Ti(50 nm) thin films were deposited on $SiO_2$/Si wafer using the DC magnetron sputtering system as the under bump metallization(UBM). And the $5{\mu}m$ thick Cu bumps and $20{\mu}m$ thick Sn bumps were fabricated on UBM by electroplating. Sn bumps were reflowed in RTA(Rapid Thermal Annealing) system and convection reflow oven. When RTA system was used, reflow was possible without using flux and IMC thickness formed in the solder interface was thinner than that of a convectional method.

  • PDF

Study on Low Temperature Formation of Ferroelectric $Sr_{0.9}4$Bi_{2.1}$$Ta_2$$O_9$ Thin Films by Sol-Gel Process and Rapid Thermal Annealing (솔-젤법 및 급속열처리에 의한 $Sr_{0.9}4$Bi_{2.1}$$Ta_2$$O_9$ 박막의 저온형성에 관한 연구)

  • 장현호;송석표;김병호
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
    • /
    • v.13 no.4
    • /
    • pp.312-317
    • /
    • 2000
  • Ferroelectric S $r_{0.9}$/B $i_{2.1}$/T $a_{2}$/ $O_{9}$ solutions were synthesized using sol-gel process in which strontinum ethoxide bismuth ethoxide trantalum ethoxide were used a s startring materials. SBT thin films were coated on Pt/Ti/ $SiO_2$/Si substrates by spin-coating. rapid thermal annealing (RTA) was used to promote crystallization. Thin films were annealed at $700^{\circ}C$ for 1 hr in an oxygen atmosphere. This temperature is about 10$0^{\circ}C$ lower than the usual annealing temperature for SBT thin films. Pt top-electrode was deposited by sputtering and thin films were post-annealed at $700^{\circ}C$ for 30 min. to enhance electrical properties. As the RTA temperature increased the higher 2 $P_{r}$ values were obtained. At RTA temperature being 78$0^{\circ}C$ remanent polarization of S $r_{0.9}$/B $i_{2.1}$/T $a_{2}$/ $O_{9}$ thin film was 7.73 $\mu$C/cm $_2$ and the leakage current density was 1.14$\times$10$^{-7}$ A/c $m^2$ at 3 V. As RTA temperature increased the breakdown voltage was decreased. It is considered that the low-field breadown is caused by the rough surface of SBT films and forming bismuth metal in SBT thin films.films.lms.

  • PDF

Large-Area Synthesis of High-Quality Graphene Films with Controllable Thickness by Rapid Thermal Annealing

  • Chu, Jae Hwan;Kwak, Jinsung;Kwon, Tae-Yang;Park, Soon-Dong;Go, Heungseok;Kim, Sung Youb;Park, Kibog;Kang, Seoktae;Kwon, Soon-Yong
    • Proceedings of the Korean Vacuum Society Conference
    • /
    • 2013.08a
    • /
    • pp.130.2-130.2
    • /
    • 2013
  • Today, chemical vapor deposition (CVD) of hydrocarbon gases has been demonstrated as an attractive method to synthesize large-area graphene layers. However, special care should be taken to precisely control the resulting graphene layers in CVD due to its sensitivity to various process parameters. Therefore, a facile synthesis to grow graphene layers with high controllability will have great advantages for scalable practical applications. In order to simplify and create efficiency in graphene synthesis, the graphene growth by thermal annealing process has been discussed by several groups. However, the study on growth mechanism and the detailed structural and optoelectronic properties in the resulting graphene films have not been reported yet, which will be of particular interest to explore for the practical application of graphene. In this study, we report the growth of few-layer, large-area graphene films using rapid thermal annealing (RTA) without the use of intentional carbon-containing precursor. The instability of nickel films in air facilitates the spontaneous formation of ultrathin (<2~3 nm) carbon- and oxygen-containing compounds on a nickel surface and high-temperature annealing of the nickel samples results in the formation of few-layer graphene films with high crystallinity. From annealing temperature and ambient studies during RTA, it was found that the evaporation of oxygen atoms from the surface is the dominant factor affecting the formation of graphene films. The thickness of the graphene layers is strongly dependent on the RTA temperature and time and the resulting films have a limited thickness less than 2 nm even for an extended RTA time. The transferred films have a low sheet resistance of ~380 ${\Omega}/sq$, with ~93% optical transparency. This simple and potentially inexpensive method of synthesizing novel 2-dimensional carbon films offers a wide choice of graphene films for various potential applications.

  • PDF

Ferroelectric Properties of PZT thin Films by Rapid Thermal Annealing (RTA처리한 PZT 박막의 강유전 특성)

  • Jeong, Kyu-Won;Park, Young;Ju, Pil-Yeon;Cho, Ik-Hyun;Lim, Dong-Gun;Yi, Jun-Sin;Song, Joon-Tae
    • The Transactions of the Korean Institute of Electrical Engineers C
    • /
    • v.49 no.4
    • /
    • pp.232-238
    • /
    • 2000
  • PZT thin films(3500 ) have been prepared onto $Pt/Ti/SiO_2/Si$ substrates with a RF magnetron sputtering system using PB1.05(Zr0.52,Ti0.48)O3 ceramic target. We used two-step annealing techniques. As the RTA times and temperatures were increased, crystallization of PZT thin films were enhanced. The ferroelectric characteristics of PZT capacitors fabricated at $700^{\circ}C$ for 60 seconds were like these remanent polarization were $12.1 \muC/cm^2$, coercive field were 110 kV/cm, leakage current density were $4.1\times10-7 A/cm^2,\; \varepsilonr=442,$ and remanent polarization were decreased by 22% after 1010 cycles, respectively.

  • PDF

Recrystallization of Phosphorus Ion Implanted Silicon on Insulator(SOI) by RTA Method (절연층상에 인을 주입시킨 실리콘 박막의 RTA 방법에 의한 재결정화)

  • Kim, Chun-Keun;Kim, Hyun-Soo;Kim, Yong-Tae;Min, Suk-Ki
    • Proceedings of the KIEE Conference
    • /
    • 1987.07a
    • /
    • pp.546-548
    • /
    • 1987
  • We have studied 1iquid phase regrowth of phosphorus ion implanted silicon films on insulator (SOI) by rapid thermal annealing (RTA) method. Many twin boundaries were observed on the regrown silicon layer and mobility of the layer was increased from $14\;cm^2/v.sec$ to $38\;cm^2/v.sec$ after annealing at $1150^{\circ}C$ for 15 sec.

  • PDF