The Voltage and Composition Dependence of Switching in a Polymer Current Limiter Device

1999 ◽  
Vol 600 ◽  
Author(s):  
Anil R. Duggal
Keyword(s):  
Composite Material ◽  
High Resistance ◽  
Composition Dependence ◽  
Arc Discharge ◽  
High Resistance State ◽  
Switching Behavior ◽  
Electrical Characteristics ◽  
Electrical Switching ◽  
Resistance State ◽  
Current Limiter

AbstractThe high power electrical switching properties of a polymer current limiter device are studied as a function of applied voltage. It is shown that a dramatic change in switching behavior occurs at a characteristic voltage. Below this voltage, the device switches to a high resistance state whereas at higher applied voltages it does not. It is shown that the high voltage, low resistance state has similar electrical characteristics to an arc discharge. Material variation experiments are also described which demonstrate that the changeover depends sensitively on the contact resistance between the filler particles of the composite material.

Non-Volatile Giant Resistance Switching in Metal-Insulator-Manganite Junctions

2004 ◽  
Vol 830 ◽  
Author(s):  
Rickard Fors ◽  
Sergey I. Khartsev ◽  
Alexander M. Grishin
Keyword(s):  
Single Crystals ◽  
High Resistance ◽  
Pulsed Laser ◽  
High Resistance State ◽  
Resistance Switching ◽  
Pulse Regime ◽  
Metal Insulator ◽  
Electrical Switching ◽  
Resistance State ◽  
Insulating Properties

ABSTRACTHeteroepitaxial CeO2(80nm)/L0.67Ca0.33MnO3(400nm) film structures have been pulsed laser deposited on LaAlO3(001) single crystals to fabricate two terminal resistance switching devices. Ag/CeO2/L0.67Ca0.33MnO3 junctions exhibit reproducible switching between a high resistance state (HRS) with insulating properties and a semiconducting or metallic low resistance state (LRS) with resistance ratios up to 105. Reversible electrical switching is a polar effect achievable both in continuous sweeping mode and in the pulse regime.

Enhanced Resistance Switching of Ga2O3 Thin Films by Ultraviolet Radiation

2020 ◽  
Vol 20 (5) ◽  
pp. 3283-3286 ◽  
Author(s):  
Yuehua An ◽  
Xia Shen ◽  
Yuying Hao ◽  
Pengfei Guo ◽  
Weihua Tang
Keyword(s):  
Ultraviolet Radiation ◽  
High Resistance ◽  
High Resistance State ◽  
High Ratio ◽  
Resistance Switching ◽  
Resistive State ◽  
Oxide Systems ◽  
Low Resistance ◽  
Resistance State

Conductive filament mechanism can explain major resistance switching behaviors. The forming/deforming of the filaments define the high/low resistance states. The ratio of high/low resistance depends on the characterization of the filaments. In many oxide systems, the oxygen vacancies are important to forming the conductive filaments for the resistance switching behaviors. As ultrawide band gap semiconductor, Ga2O3 has very high resistance for its high resistance state, while its low resistive state has relative high resistance, which normally results in low ratio of high/low resistance. In this letter, we report a high ratio of high/low resistance by ultraviolet radiation. The I–V characteristics of Au/Ti/β-Ga2O3/W sandwich structure device shows that the HRS to LRS ratio of 5 orders is achieved.

Study of the Structural Transformation of Ge2Sb2Te5 Induced by Current Pulse in Phase Change Memory

2003 ◽  
Vol 803 ◽  
Author(s):  
Rong Zhao ◽  
Tow Chong Chong ◽  
Lu Ping Shi ◽  
Pik Kie Tan ◽  
Hao Meng ◽  
...  
Keyword(s):  
Phase Change ◽  
Structural Transformation ◽  
Active Layer ◽  
High Resistance ◽  
Phase Change Memory ◽  
High Resistance State ◽  
Face Centered Cubic ◽  
Cycle Number ◽  
Resistance State ◽  
Change Memory

ABSTRACTThe electrical induced structural transformation of Ge2Sb2Te5 thin film in phase change memory device was investigated using micro-Raman spectroscopy and transmission electronic microscopy (TEM). Selected area electron diffraction (SAD) pattern showed that the electrical-induced Ge2Sb2Te5 film was crystallized into a face-centered cubic structure. Micro-Raman spectra show that the Ge2Sb2Te5 active layer at the high resistance state exhibited two minor peaks superposed on the broad peak after several switch cycles, which is identical to those of the Ge2Sb2Te5 active layer at the low resistance state. This is most likely due to the accumulation of segregated crystallites. TEM results suggest that the existence of nano-sized nuclei clusters resulted in the reduced resistance for the Ge2Sb2Te5 active layer at the high resistance state after first several switches. The dependence of resistance on the cycle number indicates that the deterioration of the Ge2Sb2Te5 active layer is resulted from the incomplete amorphization process, which is consistent with the micro-Raman results.

Impact of electrode thermal conductivity on high resistance state level in HfO2-based RRAM

2020 ◽  
Vol 53 (39) ◽  
pp. 395101 ◽  
Author(s):  
Shih-Kai Lin ◽  
Cheng-Hsien Wu ◽  
Min-Chen Chen ◽  
Ting-Chang Chang ◽  
Chen-Hsin Lien ◽  
...  
Keyword(s):  
Thermal Conductivity ◽  
High Resistance ◽  
State Level ◽  
High Resistance State ◽  
Resistance State

Two modes of bipolar resistive switching characteristics in asymmetric TaOx-based ReRAM cells

MRS Advances ◽  
2019 ◽  
Vol 4 (48) ◽  
pp. 2601-2607
Author(s):  
Toshiki Miyatani ◽  
Yusuke Nishi ◽  
Tsunenobu Kimoto
Keyword(s):  
Resistive Switching ◽  
High Resistance State ◽  
Opposite Polarity ◽  
Electrical Characteristics ◽  
Forming Process ◽  
Initial State ◽  
Bipolar Resistive Switching ◽  
Change Mechanism ◽  
Resistance State ◽  
Switching Characteristics

ABSTRACTImpacts of a forming process on bipolar resistive switching (RS) characteristics in Pt/TaOx/Ta2O5/Pt cells were investigated. We found that the forming resulted in a transition from an initial state to a particular high resistance state (HRS) in most of the Pt/TaOx/Ta2O5/Pt cells. Evaluation of electrical characteristics after the transition to the particular HRS revealed that two modes of bipolar RS with the conventional polarity based on valence change mechanism and with the opposite polarity could be selectively obtained by adjusting the magnitude of the applied voltage. Moreover, the cell resistance decreased gradually during set processes in the bipolar RS with the opposite polarity.

Reversible multilevel resistance switching of Ag–La0.7Ca0.3MnO3–Pt heterostructures

2008 ◽  
Vol 23 (2) ◽  
pp. 302-307 ◽  
Author(s):  
Dashan Shang ◽  
Lidong Chen ◽  
Qun Wang ◽  
Zihua Wu ◽  
Wenqing Zhang ◽  
...  
Keyword(s):  
High Resistance ◽  
Electric Pulse ◽  
Interface Layer ◽  
Resistance Switching ◽  
The Other ◽  
Switching Behavior ◽  
Parallel Effect ◽  
Initial Resistance ◽  
Resistance State ◽  
Multilevel Memory

The electric-pulse–induced resistance switching of the Ag–La0.7Ca03MnO3(LCMO)–Pt heterostructures was studied. The multilevel resistance switching (MLRS), in which several resistance states can be obtained, was observed in the switching from high to low resistance state (HRS → LRS) by applying electric pulse with various pulse voltages. The threshold pulse voltages of MLRS are related to the initial resistance values as well as the switching directions. On the other hand, the resistance switching behavior from low to high resistance states (LRS → HRS) shows unobvious MLRS. According to the resistance switching behavior in serial and parallel modes, MLRS was explained by the parallel effect of multifilament forming/rupture in the Ag–LCMO interface layer. The present results suggest a possible application of Ag–LCMO–Pt heterostructures as multilevel memory devices.

Unipolar resistive switching behavior of high-k ternary rare-earth oxide LaHoO3 thin films for non-volatile memory applications

2015 ◽  
Vol 1729 ◽  
pp. 23-28 ◽  
Author(s):  
Yogesh Sharma ◽  
Pankaj Misra ◽  
Shojan P. Pavunny ◽  
Ram S. Katiyar
Keyword(s):  
Thin Films ◽  
Rare Earth ◽  
Resistive Switching ◽  
High Resistance ◽  
Rare Earth Oxide ◽  
Switching Behavior ◽  
Resistive Switching Behavior ◽  
Device Structure ◽  
Resistance State ◽  
Unipolar Resistive Switching

ABSTRACTRare-earth oxides have attracted considerable research interest in resistive random access memories (ReRAMs) due to their compatibility with complementary metal-oxide semiconductor (CMOS) process. To this end we report unipolar resistive switching in a novel ternary rare-earth oxide LaHoO3 (LHO) to accelerate progress and to support advances in this emerging densely scalable research architecture. Amorphous thin films of LHO were fabricated on Pt/TiO2/SiO2/Si substrate by pulsed laser deposition, followed by sputter deposition of platinum top electrode through shadow mask in order to elucidate the resistive switching behavior of the resulting Pt/LHO/Pt metal-insulator-metal (MIM) device structure. Stable unipolar resistive switching characteristics with interesting switching parameters like, high resistance ratio of about 105 between high resistance state (HRS) and low resistance state (LRS), non-overlapping switching voltages with narrow dispersion, and excellent retention and endurance features were observed in Pt/LHO/Pt device structure. The observed resistive switching in LHO was explained by the formation/rupture of conductive filaments formed out of oxygen vacancies and metallic Ho atom. From the current-voltage characteristics of Pt/LHO/Pt structure, the conduction mechanism in LRS and HRS was found to be dominated by Ohm’s law and Poole-Frenkel emission, respectively.

Influence of SiO2 Layer on Resistive Switching Properties of SiO2/CuXO Stack Structure

2011 ◽  
Vol 687 ◽  
pp. 106-111
Author(s):  
Chih Yi Liu ◽  
Yu Chen Li ◽  
Chun Hung Lai ◽  
Shih Kun Liu
Keyword(s):  
Resistive Switching ◽  
High Resistance State ◽  
Switching Behavior ◽  
Forming Process ◽  
Dc Voltage ◽  
Si Substrates ◽  
Non Volatile Memory ◽  
Resistance State ◽  
The Difference ◽  
Switching Characteristics

CuxO and SiO2thin films were deposited using a radio-frequency magnetron sputter on Pt/Ti/SiO2/Si substrates to form SiO2/CuxO/Pt and CuxO/Pt structures. The current-voltage characteristics were measured by DC voltage sweeping using a tungsten (W) probe. The two structures needed a large voltage to initiate the first resistive switching; this sweep was called the forming process. Afterwards, the resistances of the two structures could be switched reversibly between the low-resistance-state (LRS) and high-resistance-state (HRS) by applying a DC voltage. The conduction mechanisms of the LRS and the HRS were dominated by Ohmic conduction. Structures with non-destructive readout characteristics and long retention time were suitable for use in non-volatile memory. The difference between resistive switching in W-probe/SiO2/CuxO/Pt and W-probe/CuxO/Pt structures was investigated. The additional SiO2layer decreased the switching voltages and currents; this should be due to the presence of pinholes within the SiO2layer. The influence of SiO2thickness on the resistive switching characteristics was also investigated. The switching voltages and currents, except the forming voltage, decreased as the thickness of SiO2decreased. The conducting filament model with a thermochemical reaction was suggested to best explain the resistive switching behavior that was observed.

scholarly journals Electric Modulation of Conduction in MAPbBr3 Single Crystals

2020 ◽  
Author(s):  
Shanming Ke ◽  
Shangyu Luo ◽  
Jinhui Gong ◽  
Liwen Qiu ◽  
Renhong Liang ◽  
...  
Keyword(s):  
Electric Field ◽  
Single Crystals ◽  
Resistive Switching ◽  
High Resistance ◽  
High Resistance State ◽  
Pt Symmetry ◽  
Interface Trap ◽  
Electrode Area ◽  
Resistance State ◽  
Open Question

Abstract The resistive switching (RS) mechanism of hybrid organic-inorganic perovskites is an open question until now. Here, a switchable diode-like RS behavior in MAPbBr3 single crystals using Au (or Pt) symmetry electrodes is reported. Both the high resistance state (HRS) and low resistance state (LRS) are electrode-area dependent and light responsive. We propose an electric-field-driven inner p-n junction accompanied by an interface trap-controlled SCLC mechanism to explain this switchable diode-like RS behavior in MAPbBr3 single crystals.

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