Journal of Semiconductors, Volume. 43, Issue 10, 102501(2022)

Integration of high-performance spin-orbit torque MRAM devices by 200-mm-wafer manufacturing platform

Hongchao Zhang1, Xiangyue Ma1, Chuanpeng Jiang1, Jialiang Yin1, Shuqin Lyu2, Shiyang Lu2, Xiantao Shang2, Bowen Man2, Cong Zhang2, Dandan Li2, Shuhui Li2, Wenjing Chen3, Hongxi Liu2、*, Gefei Wang2、**, Kaihua Cao1,3、***, Zhaohao Wang1, and Weisheng Zhao1,3
Author Affiliations
  • 1Fert Beijing Institute, School of Integrated Science and Engineering, Beihang University, Beijing 100191, China
  • 2Truth Memory Tech. Corporation, Beijing 100088, China
  • 3Beihang-Goertek Joint Microelectronics Institute, Qingdao Research Institute, Beihang University, Qingdao 266000, China
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    Figures & Tables(7)
    (Color online) SOT device structure and the SOT-MTJs process flow. (a) Three-dimensional schematic pictures of SOT device. (b) Cross-section TEM images cutting along the SOT track (x-direction). (c) Substrate treatment for low roughness. (d) SOT track, MTJ film stack deposition and magnetic anneal. (e) MTJ patterning and encapsulation. (f) Top electrode process.
    (Color online) Detailed microstructure of the MTJ film stack and the resistivity of W. (a) TEM diagram of the MTJ film stack. (b) Nano-beam diffraction analysis of W captured from the red box in (a). EDS mappings of (c) W, (d) Mg, (e) Co and (f) Fe. (g) The XRD curve for a simplified film structure of W/CoFeB/MgO/Ta. (h) The resistivities of W with various thicknesses. The resistivity of 5 nm W is highlighted by red circle. The orange color gradient indicate the W phase transition.
    (Color online) The typical electrical and magnetic properties of the SOT device. The wafer level distribution of theRSOT, MR,JSW, RAP andRP. (a) TypicalR–H hysteresis loops of the SOT-MTJs. (b) TypicalR–J hysteresis loops of the SOT MTJs obtained from the same sample in (a). The wafer-level electrical distribution of (c)RSOT, (d) MR, (e)JSW. (f–h) The corresponding CDF plots. (i) The bit-cell resistance distributions of SOT MTJs for both P and AP states.
    Normalized (a)ISW, (b)IFL, (c)ISOT, and (d)IFL/ISW as functions of MTJ long axisb. The data are normalized by the average value of MTJ withb = 2100 nm.
    (Color online) The switching probability (PSW) as a function of applied voltage when pulse widths were varied from 50µs down to 100 ns for both (a) P-to-AP and (b) AP-to-P directions. (c) The extractedJC at different pulse width for both P-to-AP and AP-to-P directions whenPSW = 50%.
    (Color online) (a)RSOT,RP,RAP measured after the corresponding cycling current pulses for a typical SOT-MTJ device. (b) The MR loops were recorded multiple times at each power of 10 pulses up to 1010. (c) The extractedJSW from (b) multiple times at each power of 10 pulses.
    (Color online) (a) The extracted switching probabilities as a function of the external magnetic field and the corresponding fitting curve. (b) Diamond plots of∆ for the MTJs with various MTJ long axisb. (c) The failure-bit rates of different bake time, i.e., 12, 24, 48 h at 200 °C, respectively.
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    Hongchao Zhang, Xiangyue Ma, Chuanpeng Jiang, Jialiang Yin, Shuqin Lyu, Shiyang Lu, Xiantao Shang, Bowen Man, Cong Zhang, Dandan Li, Shuhui Li, Wenjing Chen, Hongxi Liu, Gefei Wang, Kaihua Cao, Zhaohao Wang, Weisheng Zhao. Integration of high-performance spin-orbit torque MRAM devices by 200-mm-wafer manufacturing platform[J]. Journal of Semiconductors, 2022, 43(10): 102501

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    Paper Information

    Category: Articles

    Received: May. 25, 2022

    Accepted: --

    Published Online: Nov. 18, 2022

    The Author Email: Liu Hongxi (hongxi_liu@tmc-bj.cn), Wang Gefei (gefei_wang@tmc-bj.cn), Cao Kaihua (kaihua.cao@buaa.edu.cn)

    DOI:10.1088/1674-4926/43/10/102501

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