2014
DOI: 10.1007/s00339-014-8769-5
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Ferromagnetic nano-conductive filament formed in Ni/TiO2/Pt resistive-switching memory

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Cited by 28 publications
(25 citation statements)
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“…10(e)]. [29,30] This is consistent with the fact that AMR occurred in ferromagnetic transition metal depends strongly on the direction of the magnetization with respect to the electric current direction. [57,58] By rotating the direction of the out-of-plane magnetic field with respect to the substrate surface with a fixed magnitude of 2 T in the LRS of the Co/ HfO 2 /Pt device [ Fig.…”
Section: Prospective Articlesupporting
confidence: 76%
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“…10(e)]. [29,30] This is consistent with the fact that AMR occurred in ferromagnetic transition metal depends strongly on the direction of the magnetization with respect to the electric current direction. [57,58] By rotating the direction of the out-of-plane magnetic field with respect to the substrate surface with a fixed magnitude of 2 T in the LRS of the Co/ HfO 2 /Pt device [ Fig.…”
Section: Prospective Articlesupporting
confidence: 76%
“…10(a) and 10(b)]. [29][30][31] It is found that the Ni/ TiO 2 /Pt device shows convexity in its AMR plot when the direction of the magnetic field is perpendicular to the direction electric current flowing across the device [Figs. 10(c) and 10(d)], whereas a concavity is observed when the magnetic field is aligned in the direction parallel to that of the device currents [ Fig.…”
Section: Prospective Articlementioning
confidence: 99%
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“…(3) 阻变效应与隧道磁电阻效应(Tunnel Magnetoresistance, TMR) [228][229][230][231] 或巨磁电阻效应(Giant Magnetoresistance, GMR) [232] 的耦合. 山东大学的Li等人 [229] 利用CoO-ZnO纳米组分薄膜作为势垒层, 在Co/CoO- (4) 阻变效应与各向异性磁电阻效应(Anisotropic Magnetoresistance, AMR)的耦合 [233] . [239] , 在平面结构中可以 实现最小的存储单元面积--4F 2 (F为特征尺寸), 无 源阵列由于不依赖于CMOS工艺的前段制程, 可以进 行多层堆叠, 实现三维存储结构, 每个存储单元的有 效单元面积仅为4F 2 /N (N为堆叠的层数) [114] .…”
Section: 电化学金属化机制unclassified
“…Devices based on transition metal oxides, such as NiO x , 2-4 TiO x , 4,5 HfO x , 6 Ta 2 O 5 , 5,7,8 and SiO x , 9,10 have all demonstrated resistive switching with some devices exhibiting resistance ratios and cycling endurances sufficient for many computational memory applications. 9,[11][12][13][14][15][16] Resistive switching in oxide-based systems is thought to arise from the rupture and reformation of nanoscale conducting filaments that span the oxide. 1,4,13,[17][18][19] A fully formed, intact filament yields the conductive LRS, while a ruptured filament leads to the HRS.…”
mentioning
confidence: 99%