Abstract:The repeatable bipolar resistive switching phenomenon is observed in amorphous Al2O3 prepared by metalorganic chemical vapor deposition on ITO glass, with ITO as the bottom electrode and Ag as the top electrode. The crystal structure, morphology, composition and optical properties of Al2O3 thin films are investigated by x-ray diffraction, x-ray photoelectron spectroscopy, atomic force microscopy and ultraviolet-visible-infrared spectroscopy, respectively. The electronic character of Ag/Al2O3/ITO structure is t… Show more
“…Metal-oxide-based resistive random-access memories (RRAMs) [ 17 , 18 ] are promising nonvolatile memories [ 19 , 20 , 21 ]. Various binary oxides, such as Al 2 O 3 [ 22 , 23 ], HfO 2 [ 24 , 25 , 26 ], ZrO 2 [ 27 , 28 , 29 ], Ta 2 O 5 [ 30 , 31 ], and ZnO [ 32 , 33 ], have been studied for resistive-switching (RS)-memory devices owing to their relatively simple structure and ease of fabrication. Additionally, multicomponent perovskite oxides, such as Pr 0.3 Ca 0.7 MnO 3 [ 34 , 35 , 36 ], have been widely examined for their nonvolatile, forming-free memory switching; area scalability; low variability; and good reliability.…”
The resistive random-access memory (RRAM) with multi-level storage capability has been considered one of the most promising emerging devices to mimic synaptic behavior and accelerate analog computations. In this study, we investigated the reset-first bipolar resistive switching (RS) and multi-level characteristics of a LaNiO3−x thin film deposited using a reactive magnetron co-sputtering method. Polycrystalline phases of LaNiO3 (LNO), without La2O3 and NiO phases, were observed at similar fractions of Ni and La at a constant partial pressure of oxygen. The relative chemical proportions of Ni3+ and Ni2+ ions in LaNiO3−x indicated that it was an oxygen-deficient LaNiO3−x thin film, exhibiting RS behavior, compared to LNO without Ni2+ ions. The TiN/LaNiO3−x/Pt devices exhibited gradual resistance changes under various DC/AC voltage sweeps and consecutive pulse modes. The nonlinearity values of the conductance, measured via constant-pulse programming, were 0.15 for potentiation and 0.35 for depression, indicating the potential of the as-fabricated devices as analog computing devices. The LaNiO3−x-based device could reach multi-level states without an electroforming step and is a promising candidate for state-of-the-art RS memory and synaptic devices for neuromorphic computing.
“…Metal-oxide-based resistive random-access memories (RRAMs) [ 17 , 18 ] are promising nonvolatile memories [ 19 , 20 , 21 ]. Various binary oxides, such as Al 2 O 3 [ 22 , 23 ], HfO 2 [ 24 , 25 , 26 ], ZrO 2 [ 27 , 28 , 29 ], Ta 2 O 5 [ 30 , 31 ], and ZnO [ 32 , 33 ], have been studied for resistive-switching (RS)-memory devices owing to their relatively simple structure and ease of fabrication. Additionally, multicomponent perovskite oxides, such as Pr 0.3 Ca 0.7 MnO 3 [ 34 , 35 , 36 ], have been widely examined for their nonvolatile, forming-free memory switching; area scalability; low variability; and good reliability.…”
The resistive random-access memory (RRAM) with multi-level storage capability has been considered one of the most promising emerging devices to mimic synaptic behavior and accelerate analog computations. In this study, we investigated the reset-first bipolar resistive switching (RS) and multi-level characteristics of a LaNiO3−x thin film deposited using a reactive magnetron co-sputtering method. Polycrystalline phases of LaNiO3 (LNO), without La2O3 and NiO phases, were observed at similar fractions of Ni and La at a constant partial pressure of oxygen. The relative chemical proportions of Ni3+ and Ni2+ ions in LaNiO3−x indicated that it was an oxygen-deficient LaNiO3−x thin film, exhibiting RS behavior, compared to LNO without Ni2+ ions. The TiN/LaNiO3−x/Pt devices exhibited gradual resistance changes under various DC/AC voltage sweeps and consecutive pulse modes. The nonlinearity values of the conductance, measured via constant-pulse programming, were 0.15 for potentiation and 0.35 for depression, indicating the potential of the as-fabricated devices as analog computing devices. The LaNiO3−x-based device could reach multi-level states without an electroforming step and is a promising candidate for state-of-the-art RS memory and synaptic devices for neuromorphic computing.
“…In addition, the device could be fabricated in a simple metal-insulator-metal (MIM) [3] structure, enabling the high-density cell structure of a cross-bar array with 4F 2 [4,5]. It was reported that numerous transition metal oxides, including Al 2 O 3 [6,7], HfO 2 [8][9][10], NiO x [11][12][13][14], TiO x [15,16], TaO x [17,18], Nb 2 O 5 [19,20], and Pr 1−x Ca x MnO 3 [21][22][23] show resistive switching (RS) characteristics. Moreover, various deposition techniques, such as sputtering [24][25][26][27][28], atomic layer deposition (ALD) [29] and pulsed laser deposition (PLD) [30] were used for the formation of such oxides.…”
Reset-first resistive random access memory (RRAM) devices were demonstrated for off-stoichiometric Ni1−xO thin films deposited using reactive sputtering with a high oxygen partial pressure. The Ni1−xO based RRAM devices exhibited both unipolar and bipolar resistive switching characteristics without an electroforming step. Auger electron spectroscopy showed nickel deficiency in the Ni1−xO films, and X-ray photoemission spectroscopy showed that the Ni3+ valence state in the Ni1−xO films increased with increasing oxygen partial pressure. Conductive atomic force microscopy showed that the conductivity of the Ni1−xO films increased with increasing oxygen partial pressure during deposition, possibly contributing to the reset-first switching of the Ni1−xO films.
“…This development has attracted widespread attention in the industry and academia, and many new investigations of resistive memory have been initiated by researchers [13,14]. The RS effect of the insulator layer has been discovered in various kinds of amorphous metal oxides, such as ZnO, HfO 2 , TiO 2 , MgO, Al 2 O 3 , and Y 2 O 3 [15][16][17][18][19]; and in amorphous perovskite and layered perovskite oxides such as YCrO 3 , Pr 0.67 Sr 0.33 MnO 3 , Bi 3.15 Bd 0.85 Ti 3 O 12 , SrTiO 3 and Nb-doped SrTiO 3 [20][21][22][23][24][25][26], etc. Among these, the amorphous strontium titanate-based memory structure uses the following electrodes: Pt, Ti, and indium tin oxide (ITO) [23][24][25][26].…”
Amorphous SrTiO 3 thin films grown on fluorine-doped tin oxide (FTO) glass were fabricated via the sol-gel route and coating process. The composition and chemical state of the thin films were studied by X-ray photoelectron spectroscopy. A high switching ratio and good endurance were demonstrated in the Au/amorphous SrTiO 3 /FTO/glass memory cells, with an ability to achieve a ratio of high and low resistance (R off /R on) of 10 2. A stable switching voltage and uniform resistance states could be identified, moreover, using standard Weibull distribution. The results showed that Ohmic and space charge limited conduction mechanisms coexisted in the amorphous SrTiO 3 thin films. Ohmic conduction dominated in the initial high-and low-resistance state, but the space charge limited conduction mechanism was dominant in the later high-resistance field. The resistance switching effect in the device was explained by the formation and rupture of oxygen vacancies interrelated with filaments. These amorphous SrTiO 3 films have potential resistive memory applications.
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