Abstract

Electrical transport in chalcogenide-based phase change materials is an active area of research owing to the prominent role played by these materials in the field of information technology. Here, we present transport measurements (IV curves) obtained on line-cells of as-deposited amorphous phase change materials (Ge2Sb2Te5, GeTe, Ag4In3Sb66Te27) over a wide voltage and temperature range (300 K to 160 K). The well defined geometry of our devices enables a description of the transport behavior in terms of conductivity vs. electric field. At higher temperatures (300 K ≥ T ≥ 220 K) and low to intermediate fields (F < 20 V/μm), the data can be described within the framework of a previously developed model, which is based on multiple trapping transport together with 3D Poole-Frenkel emission from a two-center Coulomb potential. Based on this model, we observe a temperature dependence of the inter-trap distance, which we can relate to a temperature dependence in the occupation of the defect creating the Coulomb potential governing Poole-Frenkel emission. At higher fields and lower temperatures, the dependency of the IV curve on the electric field can be described by ln(I/I0) = (F/Fc)2. By combining this contribution with that of the Poole-Frenkel emission, we can show that the slope at high fields, Fc, is independent of temperature. We argue that models based on direct tunneling or thermally assisted tunneling from a single defect into the valence band cannot explain the observed behavior quantitatively.

Highlights

  • Phase change memory technology (PCRAM) is an active field of research with the objective to realize CMOS compatible, multi-bit nonvolatile memories.1–5 In a PCRAM cell, a nano-sized volume of phase change material is switched quickly (order of ns (Ref. 6)) and reversibly (1 Â 1011 times (Ref. 7)) between a melt-quenched amorphous and a crystalline state

  • We argue that models based on direct tunneling or thermally assisted tunneling from a single defect into the valence band cannot explain the observed behavior quantitatively

  • The transport at low to intermediate fields is of significance for the read process,9 whereas the high field regime plays a key role in the write process

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Summary

Introduction

Phase change memory technology (PCRAM) is an active field of research with the objective to realize CMOS compatible, multi-bit nonvolatile memories. In a PCRAM cell, a nano-sized volume of phase change material (chalcogenides such as Ge2Sb2Te5 or GeTe) is switched quickly (order of ns (Ref. 6)) and reversibly (1 Â 1011 times (Ref. 7)) between a melt-quenched amorphous (glassy) and a crystalline state. In a PCRAM cell, a nano-sized volume of phase change material (chalcogenides such as Ge2Sb2Te5 or GeTe) is switched quickly (order of ns (Ref. 6)) and reversibly (1 Â 1011 times (Ref. 7)) between a melt-quenched amorphous (glassy) and a crystalline state. These states differ by orders of magnitude in electrical conductivity, which enables the storage and retrieval of information.. The transport at low to intermediate fields is of significance for the read process, whereas the high field regime plays a key role in the write process. Studying steady-state electrical transport at high fields close to the threshold switching field can provide valuable insights into the threshold switching mechanism and suggest ways to tailor its behavior

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Conclusion

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