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Table 2 Different material systems showing conductance quantization effect

From: Conductance Quantization in Resistive Random Access Memory

System

RS mechanism

CF

Quantization level

RS polarity

QC observed in SET or RESET

Ag2S or Cu2S (vacuum gap) [169]

ECM

Ag

G 0

Bipolar

SET

Ag/AgI/Pt [180]

ECM

Ag

G 0

Bipolar

SET

Ag/SiO2/Pt [195, 213]

ECM

Ag

0.5 G 0

Bipolar

SET

Ag/Ta2O5/Pt [181]

ECM

Ag

G 0

Bipolar

SET and RESET

Ag/Ag2S/Pt (STM tip) [182]

ECM

Ag

G 0

Bipolar

RESET

Ag/P3HT:PCBM/ITO [183]

ECM

Ag

G 0/0.5 G 0

Bipolar

SET and RESET

Ag/a-La1-xSrxMnO3/Pt [185]

ECM

Ag

G 0

Bipolar

SET

Ag/ionic conductor-layer/W tip [191]

ECM

Ag

G 0

Bipolar

SET

Ag/GeS2/W [193]

ECM

Ag

G 0

Bipolar

SET

Cr/p+-amorphous silicon/V [192]

ECM

Metal

0.5 G 0

Unipolar

SET

Nb/ZnOx/Pt [170]

ECM

Nb or Vo

G 0/0.5 G 0

Bipolar

SET and RESET

Cu/HfOX/Pt [190]

ECM

Cu

0.5 G 0

Bipolar

SET

Pt/HfO2/Pt [69]

VCM

Vo

0.5 G 0

Unipolar

RESET

ITO/ZnOx/ITO [170]

VCM

Vo

0.5 G 0

Unipolar

SET and RESET

Ti (Ta, W)/Ta2O5/Pt [171]

VCM

Vo

G 0

Bipolar

SET and RESET

V/V2O5/V [174]

-

-

0.5 G 0

-

SET

W/CeOx/SiO2/NiSi2 [179]

VCM

Vo

0.5 G 0

Bipolar

RESET

n-Si/SiOx/p-Si [186]

VCM

Vo

G 0/0.5 G 0

Bipolar and Unipolar

SET

Ti/HfO2/TiN [188]

VCM

Vo

G 0

Bipolar

RESET

Ti/TiO2/SrTiO3/n-Si [194]

VCM

Vo

G 0

Bipolar

SET

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