AVS 63rd International Symposium & Exhibition | |
Electronic Materials and Photonics | Tuesday Sessions |
Session EM+MI+MN-TuA |
Session: | New Materials and Devices for Emerging Memory Technologies |
Presenter: | Kai-wen Hsu, University of Wisconsin-Madison |
Authors: | K. Hsu, University of Wisconsin-Madison T. Chang, University of Wisconsin-Madison L. Zhao, Stanford University Z. Wang, Stanford University R. Agasie, University of Wisconsin-Madison T. Betthauser, University of Wisconsin-Madison J. Nickles, University of Wisconsin-Madison Z. Ma, University of Wisconsin-Madison J. Chang, University of Wisconsin-Madison Y. Nishi, Stanford University J.L. Shohet, University of Wisconsin-Madison |
Correspondent: | Click to Email |
Many Type 1 RRAM cells can be formed under neutron irradiation and end up in the LRS. On the other hand, unformed neutron-irradiated Type 1 RRAM cells only require a lower voltage to form. In addition, the resistance of the HRS increased on the Type 1 RRAM cell. The shift in values of the set voltage can be seen on the I-V characteristic of the neutron-irradiated Type 1 RRAM cell. A similar increase in the resistance of HRS is also observed in proton-irradiated Type 1 RRAM cells. The shift in values of the set voltage can be seen on the I-V characteristic of the proton-irradiated Type 1 RRAM cell.
There are no obvious changes to Type 2 RRAM cells after either neutron or proton irradiation. It is very likely that both the changes in thickness and fabrication are very important since these two modifications can cut down on the number of defects which affect the switching mechanism of the RRAM cell.
This work was supported by the Semiconductor Research Corporation under Contract No. 2012-KJ-2359, by the National Science Foundation under Grant No. CBET-1066231.
[1] H.-S. Philip Wong, H-Y Lee, S. Yu, Y. S. Chen, Y. Wu, P-S Chen, B. Lee, F. T. Chen, and M-J Tsai, “Metal–oxide RRAM,” Proceedings of the IEEE 100 1951 (2012).