1474
Towards InGaAs MSDRAM Capacitor-Less Cells

Tuesday, 15 May 2018: 14:00
Room 309 (Washington State Convention Center)
C. Navarro, S. Navarro, C. Marquez, C. Sampedro, L. Donetti (University of Granada), S. Karg, H. Riel (IBM Research, Zurich), and F. Gamiz (University of Granada)
The need of a low-power, fast and low-cost CMOS compatible embedded DRAM cell is rising incessantly with the upcoming Internet of Things (IoT) era [1]. Capacitor-less DRAM cells [2, 3] have emerged as a promising solution since they do not require dedicated fabrication steps to deal with the storage node. Among this breeze of cells, the MSDRAM [4] can be highlighted due to the simpler manufacturing process.

The MSDRAM (Meta-Stable-Dip RAM) memory operation is based on inter-gate coupling [5] and non-equilibrium state [6]. The back gate (ground-plane) is biased positively to induce a virtual n-type back-channel while the front-gate voltage is negative to retain any available hole in the body. By modulating the hole population at the front-channel, the vertical top-gate induced electric field is screened (or not) so that the back electron-channel is maintained (or depleted). Depending upon the back-channel depletion degree different conductance values are achieved defining the logic ‘1’ and ‘0’ memory states. State programming is carried out by injecting holes by band-to-band tunneling at the drain edge (W1) or evacuating holes by top-gate capacitive coupling (W0)

In this work, a III-V InGaAs MSDRAM cell is built and its memory operation is demonstrated by TCAD numerical simulations in Synopsys [7, 8]. The detailed structure and the doping are shown in Fig.1. The basic memory operation is depicted in Fig. 2a for a W0-R-W1-R-W0-R sequence with W1/0 being the ‘1’/’0’ state programming and R the reading. The current after any W0 operation remains much lower than after W1. Figure 2b represents the body electron and hole densities after the first W0 and W1, respectively. Following W0, the hole density is limited underneath the top dielectric allowing a strong vertical field that depletes the back-channel from electrons leading to a drastic drop in the conductance and thus in the drain current. On the contrary, after generating holes by band-to-band tunneling during W1, the electron back-channel is reinforced enabling a larger current level while reading afterward.

In conclusion, preliminary TCAD results demonstrate the feasibility of implementing the MSDRAM concept on III-V materials.

REMINDER project (No 687931) is thanked for support.