K. Itoh

Trends in low-power circuit technologies of CMOS RAM chips are reviewed in terms of three key issues: charging capacitance, operating voltage, and dc current. The discussion includes a general description of power sources in a RAM chip, and covers both DRAMs and SRAMs. In DRAMs, successive circuit advancements have produced a power reduction equivalent to two to three orders of magnitude over the last decade for a fixed memory capacity chip. Coupled with the low-power advantage of CMOS circuits, two technologies have been the major contributors to power reduction: lower charging capacitance due to partial activation of multi-divided arrays that use multi-divisions of data and word lines; and lower operating voltage resulting from external power supply reduction, half-V/sub DD/ precharging and on-chip voltage down converting scheme. In SRAMs, partial activation of a multi-divided word line drastically reduces the dc current from the data-line load to the selected cell. In addition to advances in the sense amplifier circuit, an auto power down scheme that uses address transition detection for word driver and column circuitry further reduces the dc current. It is also shown that to design ultralow voltage DRAMs and SRAMs, the application of subthreshold current reduction circuits (such as source-gate back biasing) to cell and iterative circuit blocks will be indispensable in the future.< <ETX xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">&gt;</ETX>

Low-voltage circuit technologies for higher-density dynamic RAMs (DRAMs) and their application to an experimental 64-Mb DRAM with a 1.5-V internal operating voltage are presented. A complementary current sensing scheme is proposed to reduce data transmission delay. A speed improvement of 20 ns was achieved when utilizing a 1.5-V power supply. An accurate and speed-enhanced half-V/sub CC/ voltage generator with a current-mirror amplifier and tri-state buffer is proposed. With it, a response time reduction of about 1.5 decades was realized. A word-line driver with a charge-pump circuit was developed to achieve a high boost ratio. A ratio of about 1.8 was obtained from a power supply voltage as low as 1.0 V. A 1.28 mu m/sup 2/ crown-shaped stacked-capacitor (CROWN) cell was also made to ensure a sufficient storage charge and to minimize data-line interference noise. An experimental 1.5 V 64 Mb DRAM was designed and fabricated with these technologies and 0.3 mu m electron-beam lithography. A typical access time of 70 ns was obtained, and a further reduction of 50 ns is expected based on simulation results. Thus, a high-speed performance, comparable to that of 16-Mb DRAMs, can be achieved with a typical power dissipation of 44 mW, one tenth that of 16-Mb DRAMs. This indicates that a low-voltage battery operation is a promising target for future DRAMs.< <ETX xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">&gt;</ETX>

This paper describes low-voltage random-access memory (RAM) cells and peripheral circuits for standalone and embedded RAMs, focusing on stable operation and reduced subthreshold current in standby and active modes. First, technology trends in low-voltage dynamic RAMs (DRAMs) and static RAMs (SRAMs) are reviewed and the challenges of low-voltage RAMs in terms of cell signal charge are clarified, including the necessary threshold voltage, V <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">T</inf> , and its variations in the MOS field-effect transistors (MOSFETs) of RAM cells and sense amplifiers, leakage currents (subthreshold current and gate-tunnel current), and speed variations resulting from design parameter variations. Second, developments in conventional RAM cells and emerging cells, such as DRAM gain cells and leakage-immune SRAM cells, are discussed from the viewpoints of cell area, operating voltage, and leakage currents of MOSFETs. Third, the concepts proposed to date to reduce subthreshold current and the advantages of RAMs with respect to reducing the subthreshold current are summarized, including their applications to RAM circuits to reduce the current in standby and active modes, exemplified by DRAMs. After this, design issues in other peripheral circuits, such as sense amplifiers and low-voltage supporting circuits, are discussed, as are power management to suppress speed variations and reduce the power of power-aware systems, and testing. Finally, future prospects based on the above discussion are examined.

A switched-source-impedance (SSI) CMOS circuit is proposed as a means of reducing the exponential increase of subthreshold current with threshold-voltage scaling. Inserting a switched impedance at the source of a MOS transistor reduces the standby subthreshold current of giga-scale LSI's operating at room temperature by three to four orders of magnitude and suppresses the current variation caused by threshold-voltage and temperature fluctuations. The scheme is applicable to any combinational and sequential CMOS logic circuits as long as their standby node voltages are predictable. The standby current of a 16-Gb DRAM is expected to be reduced from 1.1 A to 0.29 mA using this scheme. Hence, battery backup of giga-scale LSI's will be possible even at room temperature and above.< <ETX xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">&gt;</ETX>

A realistic model structure of the ferrielectric phase is proposed by taking into account the apparent tilt angle measurements. On the basis of the model, the electric and optical responses are investigated in the ferrielectric SmC γ * as well as in the antiferroelectric SmC A * phases of MHPOBC (C 8 H 17 O- - -COO- -COOC * H(CH 3 )C 6 H 13 ) under triangular waves of various frequencies. At low frequencies, D - E curves show double and triple hysteresis loops characteristic of the antiferroelectric and the ferrielectric phases, respectively. T (transmittance)- E curves also reveal similar hysteresis loops. With increasing frequency, the direct switching between the two ferroelectric states occurs without passing through the antiferroelectric state or the ferrielectric states. The complicated frequency dependence is interpreted based on the spatially inhomogeneous domain switching.