dRAM Design Using the Taper-Isolated Dynamic RAM Cell
J.E. Leiss, Pallab K. Chatterjee, T.C. Holloway
Abstract
J.E. Leiss, Pallab K. Chatterjee, T.C. Holloway
Abstract
The TI dRAM cell, a MOSFET with two dynamically programmable threshold states, is very attractive for VLSI dRAM's because of its potential 3X density advantage over the one-transistor and -capacitor (1-T) cell, 10X lower leakage at high temperatures compared to the 1-T cell, and its immunity to soft errors. Linear scaling of the 1-T cell by a factor k reduces the available signal by ~k/sup 3/, whereas the charging current for the TI RAM cell is invariant to scaling since the W/L ratio remains constant allowing it to scale to higher density. An experimental array (64 rows by 8 columns), representing a cross section of a 16K dRAM, with on-chip decoding and sensing has been fabricated using the TI RAM cell as the memory element, Using 4-spl mu/m design rules, the cell size was 204 /spl mu/m/sup 2/ due to pitch requirements for the decoder and sense amplifier. This compares with 170-200 /spl mu/m/sup 2/ for the 1-T cell using 2.5-/spl mu/m design rules being fabricated in the 64K dRAM's today. The array which is compatible with 5-V-only operation was designed to provide diagnostic capability rather than speed and shows the data can be accessed 85-100 ns after the CAS signal, In this paper, the physics of the TI RAM cell are discussed as well as circuit considerations for its implementation into an array.
OpenAlex reports 1 citations for this work. Citation counts describe recorded attention and do not establish research quality.
A contribution statement is not available in the OpenAlex record.
Method details are not available in the OpenAlex metadata.
Findings are not separately available in the OpenAlex metadata.
Limitations are not available in the OpenAlex metadata.
Application details are not available in the OpenAlex metadata.
The TI dRAM cell, a MOSFET with two dynamically programmable threshold states, is very attractive for VLSI dRAM's because of its potential 3X density advantage over the one-transistor and -capacitor (1-T) cell, 10X lower leakage at high temperatures compared to the 1-T cell, and its immunity to soft errors. Linear scaling of the 1-T cell by a factor k reduces the available signal by ~k/sup 3/, whereas the charging current for the TI RAM cell is invariant to scaling since the W/L ratio remains constant allowing it to scale to higher density. An experimental array (64 rows by 8 columns), representing a cross section of a 16K dRAM, with on-chip decoding and sensing has been fabricated using the TI RAM cell as the memory element, Using 4-spl mu/m design rules, the cell size was 204 /spl mu/m/sup 2/ due to pitch requirements for the decoder and sense amplifier. This compares with 170-200 /spl mu/m/sup 2/ for the 1-T cell using 2.5-/spl mu/m design rules being fabricated in the 64K dRAM's today. The array which is compatible with 5-V-only operation was designed to provide diagnostic capability rather than speed and shows the data can be accessed 85-100 ns after the CAS signal, In this paper, the physics of the TI RAM cell are discussed as well as circuit considerations for its implementation into an array.
Key concepts: Dram, Sense amplifier, Dynamic random-access memory, Very-large-scale integration, CAS latency, Memory cell, Chip, Transistor