Resistance Drift in Melt-Quenched Ge 2 Sb 2 Te 5 Phase Change Memory Line Cells at Cryogenic Temperatures
We characterized resistance drift in phase change memory devices in the 80 K to 300 K temperature range by performing measurements on 20 nm thick, ∼70–100 nm wide lateral Ge 2 Sb 2 Te 5 (GST) line cells. The cells were amorphized using 1.5–2.5 V pulses with ∼50–100 ns duration leading to ∼0.4–1.1 mA...
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Veröffentlicht in: | ECS journal of solid state science and technology 2024-02, Vol.13 (2), p.25001 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | We characterized resistance drift in phase change memory devices in the 80 K to 300 K temperature range by performing measurements on 20 nm thick, ∼70–100 nm wide lateral Ge
2
Sb
2
Te
5
(GST) line cells. The cells were amorphized using 1.5–2.5 V pulses with ∼50–100 ns duration leading to ∼0.4–1.1 mA peak reset currents resulting in amorphized lengths between ∼50 and 700 nm. Resistance drift coefficients in the amorphized cells are calculated using constant voltage measurements starting as fast as within a second after amorphization and for 1 h duration. Drift coefficients range between ∼0.02 and 0.1 with significant device-to-device variability and variations during the measurement period. At lower temperatures (higher resistance states) some devices show a complex dynamic behavior, with the resistance repeatedly increasing and decreasing significantly over periods in the order of seconds. These results point to charge trapping and de-trapping events as the cause of resistance drift.
Resistance drift measurements in a set of narrow and wider Ge2Sb2Te5 line cells at 80–300 K.
Significant temporal and device-to-device variability in determination of resistance drift coefficients.
Amorphization pulse characterization and correlation of amorphized length to the cell current during melt-quench process.
Improved experimental setup for extremely low-leakage and fast measurements. |
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ISSN: | 2162-8769 2162-8777 |
DOI: | 10.1149/2162-8777/ad2332 |