• Title/Summary/Keyword: Interface trap charge density

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Charge Pumping 기술을 응용한 열화된 SONOSFET 비휘발성 기억소자의 Si-SiO$_2$ 계면트랩에 관한 연구 (A Study on the Si-SiO$_2$Interface Traps of the Degraded SONOSFET Nonveolatile Memories with the Charge Pumping Techniques)

  • 김주열;김선주;이성배;이상배;서광열
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 1994년도 추계학술대회 논문집
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    • pp.59-64
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    • 1994
  • The Si-SiO$_2$interface trpas of the degraded short-channel SONOSFET memory devices were investigated using the charge pumping techniques. The degradation of devices with write/erase cycle appeared as the increase of the Si-SiO$_2$interface trap density. In order to determine the capture cross-section of the interface trap. I$\_$CP/-V$\_$GL/ characteristic curves were measured at different temperatures. Also, the spatial distributions of Si-SiO$_2$interface trap were examined by the variable-reverse bias boltage method.

Analysis of SOHOS Flash Memory with 3-level Charge Pumping Method

  • Yang, Seung-Dong;Kim, Seong-Hyeon;Yun, Ho-Jin;Jeong, Kwang-Seok;Kim, Yu-Mi;Kim, Jin-Seop;Ko, Young-Uk;An, Jin-Un;Lee, Hi-Deok;Lee, Ga-Won
    • JSTS:Journal of Semiconductor Technology and Science
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    • 제14권1호
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    • pp.34-39
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    • 2014
  • This paper discusses the 3-level charge pumping (CP) method in planar-type Silicon-Oxide-High-k-Oxide-Silicon (SOHOS) and Silicon-Oxide-Nitride-Oxide-Silicon (SONOS) devices to find out the reason of the degradation of data retention properties. In the CP technique, pulses are applied to the gate of the MOSFET which alternately fill the traps with electrons and holes, thereby causing a recombination current Icp to flow in the substrate. The 3-level charge pumping method may be used to determine not only interface trap densities but also capture cross sections as a function of trap energy. By applying this method, SOHOS device found to have a higher interface trap density than SONOS device. Therefore, degradation of data retention characteristics is attributed to the many interface trap sites.

GaN Schottky Barrier MOSFET의 출력 전류에 대한 계면 트랩의 영향 (Interface Trap Effects on the Output Characteristics of GaN Schottky Barrier MOSFET)

  • 박병준;김한솔;함성호
    • 센서학회지
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    • 제31권4호
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    • pp.271-277
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    • 2022
  • We analyzed the effects of the interface trap on the output characteristics of an inversion mode n-channel GaN Schottky barrier (SB)-MOSFET based on the Nit distribution using TCAD simulation. As interface trap number density (Nit) increased, the threshold voltage increased while the drain current density decreased. Under Nit=5.0×1010 cm-2 condition, the threshold voltage was 3.2 V for VDS=1 V, and the drain current density reduced to 2.4 mA/mm relative to the non-trap condition. Regardless of the Nit distribution type, there was an increase in the subthreshold swing (SS) following an increase in Nit. Under U-shaped Nit distribution, it was confirmed that the SS varied depending on the gate voltage. The interface fixed charge (Qf) caused an shift in the threshold voltage and increased the off-state current collectively with the surface trap. In summary, GaN SB-MOSFET can be a building block for high power UV optoelectronic circuit provided the surface state is significantly reduced.

3차원 순차적 집적회로에서 계면 포획 전하 밀도 분포와 그 영향 (Interface trap density distribution in 3D sequential Integrated-Circuit and Its effect)

  • 안태준;이시현;유윤섭
    • 한국정보통신학회논문지
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    • 제19권12호
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    • pp.2899-2904
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    • 2015
  • 3차원 순차적 집적회로에서 열에 의한 손상으로 생성되는 계면 포획 전하가 트랜지스터의 드레인 전류-게이트 전압 특성에 미치는 영향을 소개한다. 2차원 소자 시뮬레이터를 이용해서 산화막 층에 계면 포획 전자 분포를 추출한 결과를 설명한다. 이 계면 포획 전자분포를 고려한 3차원 순차적 집적회로에서 Inter Layer Dielectric (ILD)의 길이에 따른 하층 트랜지스터의 게이트 전압의 변화에 따라서 상층 트랜지스터의 문턱전압 $V_{th}$의 변화량에 대해서 소개한다. 상대적으로 더 늦은 공정인 상층 $HfO_2$층 보다 하층 $HfO_2$층과 양쪽 $SiO_2$층이 열에 의한 영향을 더 많이 받았다. 계면 포획 전하 밀도 분포를 사용하지 않았을 때 보다 사용 했을 때 $V_{th}$ 변화량이 더 적게 변하는 것을 확인 했다. 3차원 순차적 인버터에서 ILD의 길이가 50nm이하로 짧아질수록 점점 더 $V_{th}$ 변화량이 급격히 증가하였다.

전하보유모델에 기초한 SONOS 플래시 메모리의 전하 저장층 두께에 따른 트랩 분석 (Analysis of Trap Dependence on Charge Trapping Layer Thickness in SONOS Flash Memory Devices Based on Charge Retention Model)

  • 송유민;정준교;성재영;이가원
    • 반도체디스플레이기술학회지
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    • 제18권4호
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    • pp.134-137
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    • 2019
  • In this paper, the data retention characteristics were analyzed to find out the thickness effect on the trap energy distribution of silicon nitride in the silicon-oxide-nitride-oxide-silicon (SONOS) flash memory devices. The nitride films were prepared by low pressure chemical vapor deposition (LPCVD). The flat band voltage shift in the programmed device was measured at the elevated temperatures to observe the thermal excitation of electrons from the nitride traps in the retention mode. The trap energy distribution was extracted using the charge decay rates and the experimental results show that the portion of the shallow interface trap in the total nitride trap amount including interface and bulk trap increases as the nitride thickness decreases.

재산화 질화산화 게이트 유전막을 갖는 전하트랩형 비휘발성 기억소자의 트랩특성 (Trap characteristics of charge trap type NVSM with reoxidized nitrided oxide gate dielectrics)

  • 홍순혁;서광열
    • 한국결정성장학회지
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    • 제12권6호
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    • pp.304-310
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    • 2002
  • 실리콘 기판 위의 초기 산화막을 NO 열처리 및 재산화 공정방법으로 성장한 재산화된 질화산화막을 게이트 유전막으로 사용한 새로운 전하트랠형 기억소자로의 응용가능성과 계면트랩특성을 조사하였다. 0.35$\mu$m CMOS 공정기술을 사용하여 게이트 유전막은 초기산화막을 $800^{\circ}C$에서 습식 산화하였다 전하트랩영역인 질화막 층을 형성하기 위해 $800^{\circ}C$에서 30분간 NO 열처리를 한 후 터널 산화막을 만들기 위해 $850^{\circ}C$에서 습식 산화방법으로 재산화하였다. 프로그램은 11 V, 500$\mu$s으로 소거는 -l3 V, 1 ms의 조건에서 프로그래밍이 가능하였으며, 최대 기억창은 2.28 V이었다. 또한 11 V, 1 ms와 -l3 V, 1 ms로 프로그램과 소거시 각각 20년 이상과 28시간의 기억유지특성을 보였으며 $3 \times 10^3$회 정도의 전기적 내구성을 나타내었다. 단일접합 전하펌핑 방법으로 소자의 계면트랩 밀도와 기억트랩 밀도의 공간적 분포를 구하였다. 초기상태에서 채널 중심 부근의 계면트랩 및 기억트랩 밀도는 각각 $4.5 \times 10^{10}/{cm}^2$$3.7\times 10^{1R}/{cm}^3$ 이었다. $1 \times 10^3$프로그램/소거 반복 후, 계면트랩은 $2.3\times 10^{12}/{cm}^2$으로 증가하였으며, 기억트랩에 기억된 전하량은 감소하였다.

금속후 어닐링 방법이 Si-$SiO_2$ 계면 전하 농도에 미치는 영향 (Effect of Post-Metallization Anneal (PMA) on Interface Trap Density of Si-$SiO_2$)

  • 정종완
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2007년도 추계학술대회 논문집
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    • pp.157-158
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    • 2007
  • Effects of post-metallization anneal (PMA) on interface trap characteristics of Si-$SiO_2$ are studied. The conventional PMA method utilizes forming gas anneal, where 10% hydrogen in nitrogen atmosphere is used. A new PMA method utilizes hydrogen rich PECVD- silicon nitride $(SiN_x)$ film as a hydrogen diffusion source and a out-diffusion blocking layer. It can be shown through charge pumping current measurement that the new PMA is indeed effective to decrease Si-$SiO_2$ interface trap density.

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SANOS 메모리 셀 트랜지스터에서 Tunnel Oxide-Si Substrate 계면 트랩에 따른 소자의 전기적 특성 및 신뢰성 분석 (Analysis of the Interface Trap Effect on Electrical Characteristic and Reliability of SANOS Memory Cell Transistor)

  • 박성수;최원호;한인식;나민기;엄재철;이승석;배기현;이희덕;이가원
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2007년도 추계학술대회 논문집
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    • pp.94-95
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    • 2007
  • In this paper, the dependence of electrical characteristics of Silicon-$Al_2O_3$-Nitride-Oxide-Silicon (SANOS) memory cell transistors and program speed, reliability of memory device on interface trap between Si substrate and tunneling oxide was investigated. The devices were fabricated by the identical processing in a single lot except the deposition method of the charge trapping layer, nitride. In the case of P/E speed, it was shown that P/E speed is slower in the SONOS cell transistors with larger interface trap density by charge blocking effect, which is confirmed by simulation results. However, the data retention characteristics show much less dependence on interface trap. Therefore, to improve SANOS memory characteristic, it is very important to optimize the interface trap and charge trapping layer.

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Investigation of Endurance Degradation in a CTF NOR Array Using Charge Pumping Methods

  • An, Ho-Myoung;Kim, Byungcheul
    • Transactions on Electrical and Electronic Materials
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    • 제17권1호
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    • pp.25-28
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    • 2016
  • We investigate the effect of interface states on the endurance of a charge trap flash (CTF) NOR array using charge pumping methods. The endurance test was completed from one cell selected randomly from 128 bit cells, where the memory window value after 102 program/erase (P/E) cycles decreased slightly from 2.2 V to 1.7 V. However, the memory window closure abruptly accelerated after 103 P/E cycles or more (i.e. 0.97 V or 0.7 V) due to a degraded programming speed. On the other hand, the interface trap density (Nit) gradually increased from 3.13×1011 cm−2 for the initial state to 4×1012 cm−2 for 102 P/E cycles. Over 103 P/E cycles, the Nit increased dramatically from 5.51×1012 cm−2 for 103 P/E cycles to 5.79×1012 cm−2 for 104 P/E cycles due to tunnel oxide damages. These results show good correlation between the interface traps and endurance degradation of CTF devices in actual flash cell arrays.

Characterization of the Vertical Position of the Trapped Charge in Charge-trap Flash Memory

  • Kim, Seunghyun;Kwon, Dae Woong;Lee, Sang-Ho;Park, Sang-Ku;Kim, Youngmin;Kim, Hyungmin;Kim, Young Goan;Cho, Seongjae;Park, Byung-Gook
    • JSTS:Journal of Semiconductor Technology and Science
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    • 제17권2호
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    • pp.167-173
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    • 2017
  • In this paper, the characterization of the vertical position of trapped charges in the charge-trap flash (CTF) memory is performed in the novel CTF memory cell with gate-all-around structure using technology computer-aided design (TCAD) simulation. In the CTF memories, injected charges are not stored in the conductive poly-crystalline silicon layer in the trapping layer such as silicon nitride. Thus, a reliable technique for exactly locating the trapped charges is required for making up an accurate macro-models for CTF memory cells. When a programming operation is performed initially, the injected charges are trapped near the interface between tunneling oxide and trapping nitride layers. However, as the program voltage gets higher and a larger threshold voltage shift is resulted, additional charges are trapped near the blocking oxide interface. Intrinsic properties of nitride including trap density and effective capture cross-sectional area substantially affect the position of charge centroid. By exactly locating the charge centroid from the charge distribution in programmed cells under various operation conditions, the relation between charge centroid and program operation condition is closely investigated.