Ming-Hsiu Lee

Ultra-Thin Phase-Change Bridge Memory Device Using GeSb

An ultra-thin phase-change bridge (PCB) memory cell, implemented with doped GeSb, is shown with < 100muA RESET current. The device concept provides for simplified scaling to small cross-sectional area (60nm2) through ultra-thin (3nm) films; the doped GeSb phase-change material offers the potential for both fast crystallization and good data retention

High Performance 45-nm SOI Technology with Enhanced Strain, Porous Low-k BEOL, and Immersion Lithography

We present a 45-nm SOI CMOS technology that features: i) aggressive ground-rule (GR) scaling enabled by 1.2NA/193nm immersion lithography, ii) high-performance FET response enabled by the integration of multiple advanced strain and activation techniques, iii) a functional SRAM with cell size of 0.37mum2, and iv) a porous low-k (k=2.4) dielectric for minimized back-end wiring delay. The list of FET-specific performance elements includes enhanced dual-stress liner (DSL), advanced eSiGe, stress memorization (SMT), and advanced anneal (AA). The resulting PFET/NFET Idsat values, at Vdd of 1.0V and 45nm GR gate pitch, are 840muA/mum and 1240muA/mum respectively. The global wiring delay achieved with k=2.4 reflects a 20% reduction compared to k=3.0

Novel One-Mask Self-Heating Pillar Phase Change Memory

A novel Pillar phase change memory based on fully integrated test arrays in 180nm CMOS technology has been successfully fabricated. A current-confining Pillar structure leads to a self-heating at the center of the chalcogenide layer, and needs only one additional mask level for its fabrication. Switching characteristics with write currents less than 900muA at 75nm diameter and multilevel operation are reported

A low power phase change memory using thermally confined TaN/TiN bottom electrode

Application of phase change memory (PCM) has been limited by the high power required to reset the device (changing from crystalline to amorphous state by melting the phase change material). Utilizing the poor thermal and electrical conductivity of TaN we have designed a simple structure that thermally insulates the bottom electrode and thus drastically reduces the heat loss. A 39nm bottom electrode with a TaN thermal barrier and 1.5nm of TiN conductor has demonstrated 30µA reset current, representing a 90% reduction. The benefit of thermal insulation is understood through electrothermal simulation, and the benefit is demonstrated in a 256Mb test chip. The low reset current also improves the reliability and excellent cycling endurance >1E9 is observed. This low power device is promising for expanding the application for PCM.

On the dynamic resistance and reliability of phase change memory

A novel characterization metric for phase change memory based on the measured cell resistance during RESET programming is introduced. We show that this dasiadynamic resistancepsila (Rd) is inversely related to the programming current (I), as Rd = [A/I] + B. While the slope parameter A depends only on the intrinsic properties of the phase change material, the intercept B also depends on the effective physical dimensions of the memory element. We demonstrate that these two parameters provide characterization and insight into the degradation mechanisms of memory cells during operation.

Understanding amorphous states of phase-change memory using Frenkel-Poole model

A method based on Frenkel-Poole emission is proposed to model the amorphous state (high resistance state) in mushroom-type phase-change memory devices. The model provides unique insights to probe the device after amorphizing (RESET) operation. Even when the resistance appears the same under different RESET conditions, our model suggests that both the amorphous region size and the defect states are different. With this powerful new tool, detailed changes inside the amorphous GST for MLC operation and retention tests are revealed.

Endurance Improvement of Ge2Sb2Te5-Based Phase Change Memory

We describe a cycling failure mode in Ge 2 Sb 2 Te 5 -based phase change memory, based on density difference of GST in different phases and the SET/RESET thermal operations. Voids that develop and merge with each other within GST programming volume after cycling eventually lead to cell failure. By adding suitable amount of doping material into GST, we are able to delay this void formation process and to significantly improve the cell endurance to more than 10 9 cycles.

Mechanisms of retention loss in Ge 2 Sb 2 Te 5 -based Phase-Change Memory

Data retention loss from the amorphous (RESET) state over time in Phase-Change Memory cells is associated with spontaneous crystallization. In this paper, the change in the threshold voltage (VT) of memory cells in the RESET state before and after heating is used as a probe into the nature of the retention loss mechanisms. Two mechanisms for the retention loss behavior are identified, responsible for the main distribution and the tail distribution, respectively. Experimental results suggest that (i) an optimized RESET operation produces a fully amorphized Ge2Sb2Te5 (aGST) active region, with no crystalline domains inside, (ii) cells in the tail distribution fail to retain their RESET state due to spontaneous generation of crystallization nuclei and grain growth, and (iii) cells in the main distribution fail due to grain growth from the amorphous/crystalline GST boundary, instead of nucleation within the active region.

A double precision floating point multiply

A 2.2GHz 53/spl times/54 bit pipelined multiplier is fabricated in 130nm CMOS technology with an area of 0.15mm/sup 2/. The circuit implementation results in a 50% size reduction over the previously reported values. The circuit operates at 2.2GHz and uses 522mW at 80% switching factor, 1.2V supply and 25/spl deg/C.

Multi-level 40nm WO X resistive memory with excellent reliability

40nm WOX ReRAM has several unique characteristics that are very favorable for MLC application. (1) Although the resistance has strong temperature dependence (as for all ReRAMs) the J-V characteristics can be accurately described, thus all MLC levels are easily modeled. (2) The device is immune to over-erase, thus allow fast MLC programming. (3) The programming is self-converging (as Flash memories) and is independent of history. Thus an algorithm similar to ISPP (Incremental Step Pulse Programming), commonly used by MLC NAND flash, is designed to achieve accurate MLC states. Consequently, fast 50ns switching, 2-bit/cell and 3-bit/cell MLC states with good cycling characteristics and low read disturbance (> 1010) is achieved.