A Finite Element Model for Stochastic Set Operation in Phase-Change Memory

Author(s):  
Min-Kyu Shin ◽  
Donghwa Lee ◽  
Pil-Ryung Cha ◽  
Yongwoo Kwon
2017 ◽  
Author(s):  
J. An ◽  
K. Kim ◽  
C. Choi ◽  
S. Shindo ◽  
Y. Sutou ◽  
...  

2009 ◽  
Vol 23 (17) ◽  
pp. 3625-3630 ◽  
Author(s):  
SANCHAI HARNSOONGNOEN ◽  
CHIRANUT SA-NGIAMSAK ◽  
APIRAT SIRITARATIWAT

This works reports, for the first time, the thorough study and optimisation of Phase Change Memory (PCM) structure with thin metal inserted chalcogenide via electrical resistivity (ρ) using finite element modeling. PCM is one of the best candidates for next generation non-volatile memory. It has received much attention recently due to its fast write speed, non-destructive readout, superb scalability, and great compatibility with current silicon-based mass fabrication. The setback of PCM is a high reset current typically higher than 1mA based on 180nm lithography. To reduce the reset current and to solve the over-programming failure, PCM with thin metal inserted chalcogenide (bottom chalcogenide/metal inserted/top chalcogenide) structure has been proposed. Nevertheless, reports on optimisation of the electrical resistivity using the finite element method for this new PCM structure have never been published. This work aims to minimize the reset current of this PCM structure by optimizing the level of the electrical resistivity of the PCM profile using the finite element approach. This work clearly shows that PCM characteristics are strongly affected by the electrical resistivity. The 2-D simulation results reveal clearly that the best thermal transfer of and self-joule-heating at the bottom chalcogenide layer can be achieved under conditions; ρ_bottom chalcogenide > ρ_metal inserted > ρ_top chalcogenide More specifically, the optimized electrical resistivity of PCMTMI is attained with ρ_top chalcogenide: ρ_metal inserted: ρ_bottom chalcogenide ratio of 1:6:16 when ρ_top chalcogenide is 10-3 Ωm. In conclusion, high energy efficiency can be obtained with the reset current as low as 0.3mA and with high speed operation of less than 30ns.


2018 ◽  
Vol 54 (6) ◽  
pp. 350-351 ◽  
Author(s):  
J.S. An ◽  
K.J. Kim ◽  
C.M. Choi ◽  
S. Shindo ◽  
Y. Sutou ◽  
...  

2013 ◽  
Vol 534 ◽  
pp. 136-140
Author(s):  
Rosalena Irma Alip ◽  
Ryota Kobayashi ◽  
Yu Long Zhang ◽  
Zulfakri bin Mohamad ◽  
You Yin ◽  
...  

A novel phase change memory structure with a separate heater was proposed for a multilevel storage. Finite element analysis was conducted to investigate the possibility of multilevel storage. 100 ns SET pulses, with an increasing amplitude from 0.5 V to 3 V, were applied for heating the phase change layer, Ge2Se2T5 (GST). From the simulation result, it was exhibited that the temperature in the GST layer increased gradually when an increasing pulse is applied to the separate heater layer (N-TiSi3). This implies that crystallization is well controlled by changing the amplitude of the applied SET pulse. The gradual increase in the temperature leads to gradual resistance drop, depending strongly on the capping material. The gradual resistance drop will allow multilevel storage for the memory device.


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