Several attempts have been made to store charges in the channel regions of silicon transistors, such as in zero-capacitor random-access memories (Z-RAMs), [7,8] metastable DRAMs (MSDRAMs), [9,10] advanced RAMs (A-RAMs), [11,12] and zeroslope and zero-impact ionization RAMs (Z 2-RAMs). [13,14] Among these, Z 2-RAMs are capable of low-voltage operation with high speed, long retention time, and nondestructive reading capability, because of the positive feedback loop. [15] However, electrostatic doping induced by gate bias is required to form a potential well, which is important for the positive feedback loop. [16,17] Although thyristor RAMs (T-RAMs) employ doping regions to form the potential well, external bias is still necessary for TRAMs to retain the stored charges. [18-20] This indispensable bias for holding the stored charges has restricted their use in quasi-nonvolatile memory applications. In this paper, we propose a fully CMOS-compatible p +-n-pn + silicon memory device to enable quasi-nonvolatile memory functionality with high speed, long retention time, and nondestructive reading capability. Using a well-defined potential well in a p +-n-p-n + silicon structure with a gated n-channel region, our device utilizes holes as majority charge carriers for the positive feedback loop, unlike TRAMs which use electrons as majority charge carriers. Hence, our quasi-nonvolatile silicon memory device can retain the charges stored in the channel region without requiring any external bias, for a long time. In addition, the positive-feedback loop enables low-voltage operation, high speed, and nondestructive reading for quasi-nonvolatile memory applications. 2. Results and Discussion A quasi-nonvolatile silicon memory device consists of p +-n-p-n + regions on a silicon-on-insulator (SOI) substrate (Figure 1a). An SiO 2 /poly-Si gate stack is located on the upper side of the n-channel region. The poly-Si gate modulates the potential barrier of the n-channel region; it controls the hole injection from the p + drain region. The p-channel region is designated to block the electron injection from the n + source region. The channel regions also form potential wells; states "1" and "0" are defined by presence and absence of excess charge carriers in the potential wells, respectively. The corresponding energy band diagrams exhibit the difference in the channel region between the two states (Figure 1b). Barrier-height modulation by carrier accumulation in the potential wells is essential for the positive feedback loop, which allows memory operations. Memory hierarchy among conventional memory technologies is one of the main bottlenecks in modern computer systems; alternative memory technologies are thus necessary for quasi-nonvolatile memory applications. Herein, a fully complementary metal-oxide-semiconductor-compatible quasi-nonvolatile memory composed of p +-n-p-n + silicon on a silicon-on-insulator substrate is presented. The quasi-nonvolatile silicon memory device demonstrates highspeed write capability (≤100 ns), long retenti...

In this paper, we propose inverting logic-in-memory (LIM) cells comprising silicon nanowire feedback field-effect transistors with steep switching and holding characteristics. The timing diagrams of the proposed inverting LIM cells under dynamic and static conditions are investigated via mixed-mode technology computer-aided design simulation to verify the performance. The inverting LIM cells have an operating speed of the order of nanoseconds, an ultra-high voltage gain, and a longer retention time than that of conventional dynamic random access memory. The disturbance characteristics of half-selected cells within an inverting LIM array confirm the appropriate functioning of the random access memory array.

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In this study, we fabricated a 2 × 2 one-transistor static random-access memory (1T-SRAM) cell array comprising single-gated feedback field-effect transistors and examined their operation and memory characteristics. The individual 1T-SRAM cell had a retention time of over 900 s, nondestructive reading characteristics of 10,000 s, and an endurance of 108 cycles. The standby power of the individual 1T-SRAM cell was estimated to be 0.7 pW for holding the “0” state and 6 nW for holding the “1” state. For a selected cell in the 2 × 2 1T-SRAM cell array, nondestructive reading of the memory was conducted without any disturbance in the half-selected cells. This immunity to disturbances validated the reliability of the 1T-SRAM cell array.

The processing of large amounts of data requires a high energy efficiency and fast processing time for high-performance computing systems. However, conventional von Neumann computing systems have performance limitations because of bottlenecks in data movement between separated processing and memory hierarchy, which causes latency and high power consumption. To overcome this hindrance, logic-in-memory (LIM) has been proposed that performs both data processing and memory operations. Here, we present a NAND and NOR LIM composed of silicon nanowire feedback field-effect transistors, whose configuration resembles that of CMOS logic gate circuits. The LIM can perform memory operations to retain its output logic under zero-bias conditions as well as logic operations with a high processing speed of nanoseconds. The newly proposed dynamic voltage-transfer characteristics verify the operating principle of the LIM. This study demonstrates that the NAND and NOR LIM has promising potential to resolve power and processing speed issues.

In this paper, we propose a logic-in-memory (LIM) inverter comprising a silicon nanowire (SiNW) n-channel feedback field-effect transistor (n-FBFET) and a SiNW p-channel metal oxide semiconductor field-effect transistor (p-MOSFET). The hybrid logic and memory operations of the LIM inverter were investigated by mixed-mode technology computer-aided design simulations. Our LIM inverter exhibited a high voltage gain of 296.8 (V/V) when transitioning from logic ‘1’ to ‘0’ and 7.9 (V/V) when transitioning from logic ‘0’ to ‘1’, while holding calculated logic at zero input voltage. The energy band diagrams of the n-FBFET structure demonstrated that the holding operation of the inverter was implemented by controlling the positive feedback loop. Moreover, the output logic can remain constant without any supply voltage, resulting in zero static power consumption.

In this study, we examine the electrical characteristics of silicon nanowire feedback field-effect transistors (FBFETs) with interface trap charges between the channel and gate oxide. The band diagram, I–V characteristics, memory window, and operation were analyzed using a commercial technology computer-aided design simulation. In an n-channel FBFET, the memory window narrows (widens) from 5.47 to 3.59 V (9.24 V), as the density of the positive (negative) trap charges increases. In contrast, in the p-channel FBFET, the memory window widens (narrows) from 5.38 to 7.38 V (4.18 V), as the density of the positive (negative) trap charges increases. Moreover, we investigate the difference in the output drain current based on the interface trap charges during the memory operation.

In this study, we examined electrical stability of the p-channel feedback field-effect transistors (FBFETs) under negative bias stress (NBS) and positive bias stress (PBS). The intact FBFETs have a subthreshold swing (SS) of 0.12 mV/dec, an on-current of ~10 -4 A, and a threshold voltage (V TH ) of -0.76 V. There is a negligible change in the on-current and SS when the FBFETs are stressed by a gate-bias voltage corresponding to an electric field of 5.4 MV/cm across the gate oxide. On the other hand, as the duration of the stress increases to 1000 s, the V TH shifts to -0.89 V and -0.67 V for NBS and PBS, respectively. The V TH was recovered to over 83% at a recovery bias voltage of 5 V. The electrical stabilities of FBFETs under NBS and PBS are discussed in this study.