2018
DOI: 10.1109/lmag.2018.2829111
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Area-Efficient Multibit-per-Cell Architecture for Spin-Orbit-Torque Magnetic Random-Access Memory With Dedicated Diodes

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Cited by 11 publications
(8 citation statements)
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“…Such different vacancies distributions naturally lead to various metastable GST structures, and the most thermodynamically favorable GST phase was reported to have a highly ordered distribution of the vacancies in {111} planes, defined as GST phase 2 that comprises GST building blocks periodically separated by the vacancy layers between adjacent Te-Te planes [50], as illustrated in Figure 3(b). The Ge and Sb atoms are still off-center within Te(GeSb) 6 , as similar to phase 1, and the degree of vacancy ordering strongly pertains to the Te-Te distance. The distribution of Ge and Sb atomic species is random within individual cation layers, while the ordering of Sb and Ge atoms are preferable to be found in the cation layers next to the vacancy layers and in the middle of GST building units, respectively.…”
Section: Phase-change Materialsmentioning
confidence: 95%
See 1 more Smart Citation
“…Such different vacancies distributions naturally lead to various metastable GST structures, and the most thermodynamically favorable GST phase was reported to have a highly ordered distribution of the vacancies in {111} planes, defined as GST phase 2 that comprises GST building blocks periodically separated by the vacancy layers between adjacent Te-Te planes [50], as illustrated in Figure 3(b). The Ge and Sb atoms are still off-center within Te(GeSb) 6 , as similar to phase 1, and the degree of vacancy ordering strongly pertains to the Te-Te distance. The distribution of Ge and Sb atomic species is random within individual cation layers, while the ordering of Sb and Ge atoms are preferable to be found in the cation layers next to the vacancy layers and in the middle of GST building units, respectively.…”
Section: Phase-change Materialsmentioning
confidence: 95%
“…As Moore's law approaches its limits, further boosting the integration density of conventional volatile memories becomes extremely difficult [1]. In view of this, the concept of properly scalable non-volatile memory has become a topic of intensive study over the past decade, resulting in the emergence of several non-volatile memory devices such as ferroelectric RAM (FeRAM) [2][3][4], magnetic RAM (MRAM) [5][6][7], phase-change RAM (PCRAM) [8][9][10], and resistive RAM (RRAM) [11][12][13]. Out of these competing possibillities, PCRAM offers the widest range of advantages including superb scalability [14], fast write/read speeds [15], low energy consumption [16], and a long data retention time [17].…”
Section: Introductionmentioning
confidence: 99%
“…Ali et al [18] extended the SLC diode-based SOT-MRAM proposal to be a multibit per cell (MBC). Their proposed design, shown in Figure 4, relies on a metaloxide-metal (MOM) diode (or also known as selector) stacked over an MTJ (forming a D-MTJ) to replace the task of the read Tx in controlling the read current flow.…”
Section: Multi-bit Per Cell Dedicated Diode (Mbc-dd) Sot-mrammentioning
confidence: 99%
“…3D structure of the proposed dedicated diode multi-bit per cell (MBC) DD SOT-MRAM with (a) uniform HM electrode and MTJs with different t fl[18], (b) different HM width and MTJs with similar t fl[18].…”
mentioning
confidence: 99%
“…Recent progress in the development of non-volatile nanoscale random access memories (RAMs) has led to them offering a viable solution to the von Neumann bottleneck. These devices come mainly in the form of ferroelectric RAM (FeRAM) [9][10][11][12][13], magnetic RAM (MRAM) [14][15][16][17][18], phase-change RAM (PCRAM) [19][20][21][22][23], and resistive RAM (RRAM) [24][25][26][27][28] (see Figure 2). They usually have two distinct physical states relating to when they are either immune to or subject to external excitations.…”
Section: Introductionmentioning
confidence: 99%