Three-dimensional ovonic threshold switching model with combination of in-band and trap-to-band hopping mechanism for chalcogenide-based phase-change memory

Author(s):  
Chong Chen ◽  
Yiqun Wei ◽  
Jianwei Zhao ◽  
Xinnan Lin ◽  
Zhitang Song
2012 ◽  
Vol 100 (25) ◽  
pp. 253105 ◽  
Author(s):  
Jorge A. Vázquez Diosdado ◽  
Peter Ashwin ◽  
Krisztian I. Kohary ◽  
C. David Wright

2018 ◽  
Vol 57 (4S) ◽  
pp. 04FE13 ◽  
Author(s):  
Corentin Pigot ◽  
Fabien Gilibert ◽  
Marina Reyboz ◽  
Marc Bocquet ◽  
Paola Zuliani ◽  
...  

2008 ◽  
Vol 103 (11) ◽  
pp. 111101 ◽  
Author(s):  
A. Redaelli ◽  
A. Pirovano ◽  
A. Benvenuti ◽  
A. L. Lacaita

2003 ◽  
Vol 803 ◽  
Author(s):  
L. P. Shi ◽  
T. C. Chong ◽  
J. M. Li ◽  
H. X. Yang ◽  
J. Q. Mou

ABSTRACTIn this paper, a three-dimensional finite-element modeling is performed for the analyses of Chalcogenide Random Access Memory (C-RAM), a non-rotation nonvolatile phase change memory cell. The thermal effect generated by an incident electric pulse was mainly discussed. Thermal performances of the cell as a result of electrical and geometrical variations were quantified. Current density distribution, temperature profiles, temperature history, heating rate, cooling rate, and heat flow characteristics were obtained and analyzed. The study is useful for the failure analysis of the C-RAM.


2020 ◽  
Author(s):  
Nafisa Noor ◽  
Sadid Muneer ◽  
Raihan Sayeed Khan ◽  
Anna Gorbenko ◽  
Helena Silva

The dimensions of amorphized regions in phase-change memory cells are critical parameters to design devices for different applications but are difficult to determine by direct imaging. In this work, the length of amorphized regions in multiple, identical Ge2Sb2Te5 (GST) line cells was extracted from electrical measurements. After each cell was programmed to an amorphous state, a sequence of increasing amplitude post-reset voltage pulses separated by low-amplitude read DC-sweeps was applied. When a sufficient amplitude post-reset voltage pulse was applied to a given cell, the measured current and the post-pulse resistance increased drastically, indicating the cell re-amorphized after threshold switching, melting, and quenching. The amorphized length was calculated using the measured voltage at which threshold switching took place and the expected drifted threshold field at that time. The measured threshold voltages, hence, the extracted amorphized lengths, generally increase linearly with the programmed resistance levels, but significant variability arises from the intrinsic uniqueness in the crystallization and amorphization processes in these devices. For example, cells programmed to ~50 MΩ amorphous resistance show threshold voltages of ~5-7 V, corresponding to amorphized lengths of ~240-360 nm. This unpredictable programming feature in phase-change memory devices can be utilized in hardware security applications.


Sign in / Sign up

Export Citation Format

Share Document