• 제목/요약/키워드: Substrate bias voltage generator

검색결과 5건 처리시간 0.019초

초저전압 구동 논리 회로의누설 전류 억제를 위한 기판 전압 발생회로 (Substrate-bias voltage generator for leakage power reduction of digital logic circuits operating at low supply voltage)

  • 김길수;김형주;박상수;유재택;기훈재;김수원
    • 대한전자공학회논문지SD
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    • 제43권1호
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    • pp.1-6
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    • 2006
  • 본 논문에서는 VTCMOS(Variable-Threshold CMOS) 기법을 이용하는 초저전압 구동 논리 회로의 누설 전류 억제를 위한 기판 전압 발생회로를 제안한다. 제안하는 기판 전압 발생회로는 VSS 발생회로와 VBB 발생회로로 구성되어 있다. VSS 발생회로는 네거티브 전압을 발생시켜 VBB 발생회로에 공급하며, nB 발생회로는 공급받은 네거티브 전압을 이용하여 또 다른 네거티브 전압을 발생시킨다. 제안하는 회로의 동작을 검증하기 위해서 0.18um 1Poly-6Metal CMOS 공정을 사용하여 회로를 구현하였으며, 측정 결과 -0.95V의 기판 전압을 얻을 수 있었다. 제안한 기판 전압 발생회로를 이용함으로써, 0.5V의 전원 전압에서 동작하는 논리 회로의 누설 전류 성분을 효과적으로 줄일 수 있다.

DRAM 의 저전력 구현을 위한 안정한 기판전압 발생기 설계에 관한 연구 (A study on the Design of a stable Substrate Bias Generator for Low power DRAM's)

  • 곽승욱;성양현곽계달
    • 대한전자공학회:학술대회논문집
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    • 대한전자공학회 1998년도 추계종합학술대회 논문집
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    • pp.703-706
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    • 1998
  • This paper presents an efficient substrate-bias generator(SBG)for low-power, high-density DRAM's The proposed SBG can supply stable voltage with switching the supply voltage of driving circuit, and it can substitude the small capacitance for the large capacitance. The charge pumping circuit of the SBG suffere no VT loss and is to be applicable to low-voltage DRAM's. Also it can reduce the power consumption to make VBB because of it's high pumping efficiency. Using biasing voltage with positive temperature coefficient, VBB level detecting circuit can detect constant value of VBB against temperature variation. VBB level during VBB maintaining period varies 0.19% and the power dissipation during this period is 0.16mw. Charge pumping circuit can make VBB level up to -1.47V using VCC-1.5V, and do charge pumping operation one and half faster than the conventional ones. The temperature dependency of the VBB level detecting circuit is 0.34%. Therefore the proposed SBG is expected to supply a stable VBB with less power consumption when it is used in low power DRAM's.

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Hydrocarbon Plasma of a Low-Pressure Arc Discharge for Deposition of Highly-Adhesive Hydrogenated DLC Films

  • Chun, Hui-Gon;Oskomov, Konstantin V.;Sochugov, Nikolay S.;Lee, Jing-Hyuk;You, Yong-Zoo;Cho, Tong-Yul
    • 반도체디스플레이기술학회지
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    • 제2권1호
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    • pp.1-5
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    • 2003
  • Plasma generator based on non-self-sustained low-pressure arc discharge has been examined as a tool for deposition of highly-adhesive hydrogenated amorphous diamond-like carbon(DLC) films. Since the discharge is stable in wide range of gas pressures and currents, this plasma source makes possible to realize both plasma-immersion ion implantation(PIII) and plasma-immersion ion deposition(PIID) in a unified vacuum cycle. The plasma parameters were measured as functions of discharge current. Discharge and substrate bias voltage parameters have been determined for the PIII and PIID modes. For PIID it has been demonstrated that hard and well-adherent DLC coating are produced at 200-500 eV energies per deposited carbon atom. The growth rates of DLC films in this case are about 200-300 nm/h. It was also shown that short(∼60$\mu\textrm{s}$) high-voltage(> 1kV) substrate bias pulses are the most favorable for achieving high hardness and good adhesion of DLC, as well as for reducing of residual intrinsic stress are.

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NEW APPLICATIONS OF R.F. PLASMA TO MATERIALS PROCESSING

  • Akashi, Kazuo;Ito, Shigru
    • 한국표면공학회지
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    • 제29권5호
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    • pp.371-378
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    • 1996
  • An RF inductively coupled plasma (ICP) torch has been developed as a typical thermal plasma generator and reactor. It has been applied to various materials processings such as plasma flash evaporation, thermal plasma CVD, plasma spraying, and plasma waste disposal. The RF ICP reactor has been generally operated under one atmospheric pressure. Lately the characteristics of low pressure RF ICP is attracting a great deal of attention in the field of plasma application. In our researches of RF plasma applications, low pressure RF ICP is mainly used. In many cases, the plasma generated by the ICP torch under low pressure seems to be rather capacitive, but high density ICP can be easily generated by our RF plasma torch with 3 turns coil and a suitable maching circuiit, using 13.56 MHz RF generator. Plasma surface modification (surface hardening by plasma nitriding and plasma carbo-nitriding), plasma synthesis of AIN, and plasma CVD of BN, B-C-N compound and diamond were practiced by using low pressure RF plasma, and the effects of negative and positive bias voltage impression to the substrate on surface modification and CVD were investigated in details. Only a part of the interesting results obtained is reported in this paper.

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Diamond-Like Carbon Films Deposited by Pulsed Magnetron Sputtering System with Rotating Cathode

  • Chun, Hui-Gon;You, Yong-Zoo;Nikolay S. Sochugov;Sergey V. Rabotkin
    • 한국표면공학회지
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    • 제36권4호
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    • pp.296-300
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    • 2003
  • Extended cylindrical magnetron sputtering system with rotating 600-mm long and 90-mm diameter graphite cathode and pulsed power supply voltage generator were developed and fabricated. Time-dependent Langmuir probe characteristics as well as carbon films thickness were measured. It was shown that ratio of ions flux to carbon atoms flux for pulsed magnetron discharge mode was equal to $\Phi_{i}$ $\Phi$sub C/ = 0.2. It did not depend on the discharge current in the range of $I_{d}$ / = 10∼60 A since both the plasma density and the film deposition rate were found approximately proportional to the discharge current. In spite of this fact carbon film structure was found to be strongly dependent on the discharge current. Grain size increased from 100 nm at $I_{d}$ = 10∼20 A to 500 nm at $I_{d}$ = 40∼60 A. To deposit fine-grained hard nanocrystalline or amorphous carbon coating current regime with $I_{d}$ = 20 A was chosen. Pulsed negative bias voltage ($\tau$= 40 ${\mu}\textrm{s}$, $U_{b}$ = 0∼10 ㎸) synchronized with magnetron discharge pulses was applied to a substrate and voltage of $U_{b}$ = 3.4 ㎸ was shown to be optimum for a hard carbon film deposition. Lower voltages were not sufficient for amorphization of a growing graphite film, while higher voltages led to excessive ion bombardment and effects of recrystalization and graphitization.