Hostname: page-component-78c5997874-xbtfd Total loading time: 0 Render date: 2024-11-18T12:19:00.897Z Has data issue: false hasContentIssue false

SET Characteristics of Phase Change Bridge Devices

Published online by Cambridge University Press:  01 February 2011

Daniel Krebs
Affiliation:
krebs@physik.rwth-aachen.de, RWTH Aachen University, I. Institute of Physics, Jakobstraße 164, Aachen, 52064, Germany
Simone Raoux
Affiliation:
simone_raoux@almaden.ibm.com, IBM - Macronix PCRAM Joint Project: IBM Almaden Research Center, 650 Harry Road, San Jose, CA, 95120, United States
Charles T. Rettner
Affiliation:
rettner@almaden.ibm.com, IBM - Macronix PCRAM Joint Project: IBM Almaden Research Center, 650 Harry Road, San Jose, CA, 95120, United States
Robert M. Shelby
Affiliation:
shelby@almaden.ibm.com, IBM - Macronix PCRAM Joint Project: IBM Almaden Research Center, 650 Harry Road, San Jose, CA, 95120, United States
Geoffrey W. Burr
Affiliation:
burr@almaden.ibm.com, IBM - Macronix PCRAM Joint Project: IBM Almaden Research Center, 650 Harry Road, San Jose, CA, 95120, United States
Matthias Wuttig
Affiliation:
wuttig@physik.rwth-aachen.de, RWTH Aachen University, IBM - Macronix PCRAM Joint Project: I. Institute of Physics, Sommerfeldstraße 14, Aachen, 52074, Germany
Get access

Abstract

Scaling studies have demonstrated that Phase Change Random Access Memory (PCRAM) is one of the most promising candidates for future non-volatile memory applications. The search for suitable phase change materials with optimized properties is therefore actively pursuit. In this paper, SET (crystallization) characteristics of an ultra fast switching material Ge15Sb85 in phase change memory bridge cell devices are presented. It was found that reproducible switching between two stable states with one decade resistance contrast and current pulses as short as 10 ns for SET and RESET (re-amorphization) operation is possible. Particular emphasis was placed on the difference in crystallization kinetics between the as-deposited and melt-quenched amorphous phase. Evidence is given for the existence of an electrical field as the critical parameter for threshold switching rather than a threshold voltage. For Ge15Sb85 a threshold switching field of 9MV/m was measured and it was shown that switching from the melt-quenched amorphous phase to the crystalline phase is about 600 times faster than crystallization from the as-deposited amorphous phase.

Type
Research Article
Copyright
Copyright © Materials Research Society 2008

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

1. Ovshinsky, S. R. Phys. Rev. Lett. 21, 1450 (1968).Google Scholar
2. Yamada, N. Ohno, E. Nishiuchi, K. Akahira, N. and Takao, M. J. Appl. Phys. 69, 2849 (1991).Google Scholar
3. Chen, Y. C. et al. , IEDM Technical Digest, p.777780 (2006).Google Scholar
4. Adler, D. Shur, M. S. Silver, M. and Ovshinsky, S. R. J. Appl. Phys. 51, 3289 (1980).Google Scholar
5. Shenoy, S. R. J. of Non-Cry. Solids 85, 273 (1986).Google Scholar
6. Ielmini, D. and Zhang, Y., J. Appl. Phys. 102, 054517 (2007).Google Scholar