2017
DOI: 10.1002/aelm.201700264
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Top‐Down Synthesis of Hollow Graphene Nanostructures for Use in Resistive Switching Memory Devices

Abstract: Hollow nanostructures exhibit a wide range of potential applications because of the quantum confinement effect that arises from the narrow width of such nanostructures. It is challenging to synthesize hollow nanostructures of 2D materials. A facile top‐down approach is presented for synthesizing high‐quality hollow graphene nanostructures from highly oriented pyrolytic graphite target. Hollow graphene nanostructures composed of few‐layered graphene nanorings (GNRs) are synthesized in acetone and poly(4‐vinylpy… Show more

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Cited by 8 publications
(6 citation statements)
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References 70 publications
(140 reference statements)
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“…[45,46] In the Ohmic region, current is proportional to electric field; in the Child's region, the injected electrons are trapped to form the space charge effect and drift current; in the TCLC region, the traps are gradually filled by electrons with the increasing electric field, then the concentration of free electrons increases sharply, and the device enters LRS. [45][46][47][48][49] iv) Fowler-Nordheim (F-N) tunneling (ln(I/V 2 ) ∝ 1/V), a quantum effect that electrons directly pass through the triangular barrier at the interface between the metal and functional layer. [50,51] v) Poole-Frenkel (P-F) emission (ln(I/V) ∝ V 1/2 ), in which the electrons in traps are excited into the conduction band.…”
Section: Classification Of Memristorsmentioning
confidence: 99%
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“…[45,46] In the Ohmic region, current is proportional to electric field; in the Child's region, the injected electrons are trapped to form the space charge effect and drift current; in the TCLC region, the traps are gradually filled by electrons with the increasing electric field, then the concentration of free electrons increases sharply, and the device enters LRS. [45][46][47][48][49] iv) Fowler-Nordheim (F-N) tunneling (ln(I/V 2 ) ∝ 1/V), a quantum effect that electrons directly pass through the triangular barrier at the interface between the metal and functional layer. [50,51] v) Poole-Frenkel (P-F) emission (ln(I/V) ∝ V 1/2 ), in which the electrons in traps are excited into the conduction band.…”
Section: Classification Of Memristorsmentioning
confidence: 99%
“…As hollow GQDs, graphene nanorings (GNRs) in the Pt/ GNRs-P4VP/ITO/PET memristor modulate memristance by electron trapping and detrapping effect. [46] Typical bipolar resistive switching behavior shows a switching current ratio of 2 × 10 4 in Figure 9a. The electron transport mode of HRS is in keeping with the classic SCLC (Figure 9b).…”
Section: Electron Trapping and Detrapping Effect Of Cdsmentioning
confidence: 99%
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“…材料制备过程中的缺陷、掺杂与空位等因素都 会影响其阻变行为. 研究者提出了许多阻变效应的 作用机理, 如导电细丝形成/断裂 [12,27,28] 、陷阱填充 限制电流 [13,29,30] 与界面肖特基势垒调制 [18,31,32] 等, 得到了广泛认可; 而量子点材料的阻变机理较为复 电细丝/形成断裂机理的基本特征 [33,34] ; 同时I-V 曲线中并未出现界面肖特基势垒调制机理常有的 正 负 向 偏 压 LRS电 流 不 对 称 现 象 [35,36] , 这 表 明 SnO 2 QDs的阻变效应并非由单一的阻变机理控制.…”
Section: 阻变机理及调控机制研究unclassified
“…Meanwhile, graphene‐based materials have been extensively studied in the RRAM field because of their excellent mechanical and electrical properties . Recently, a zinc oxide–graphene hybrid was prepared to harness the unique properties of these two components for novel applications .…”
mentioning
confidence: 99%