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Enhanced out-of-plane piezoelectric effect in In_2Se_3/transition metal dichalcogenide heterostructures

机译:在IN_2SE_3 /过渡金属二甲基异质结构中增强平面外压电效果

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摘要

The two-dimensional material α-In_2Se_3, which possesses both out-of-plane ferroelectricity and piezoelectricity in monolayer, opens opportunity for the smart material integration in a micro-electro-mechanical system. However, the piezoelectric response decreases with the decreasing thickness of α-In_2Se_3, hindering the application of few-layer α-In_2Se_3 in electromechanical transformation. In this work, we report a strategy to enhance the out-of-plane piezoelectric coefficients by constructing In_2Se_3/transition metal dichalcogenides (TMDs) heterostructures. Such a strategy shows great piezoelectric enhancement compared with monolayer In_2Se_3, and the largest e_(31) of 2.9× 10~(-10) C/m is achieved in MoS_2/In_2Se_3. A phenomenological model is further constructed to connect the piezoelectric coefficients with the polarizations of the heterostructures. Furthermore, the induced dipole moment strongly affects the band structure of heterostructures, yielding tunable light absorption. The proposed In_2Se_3/TMDs heterostructures represent an innovative strategy for the development of future efficient piezoelectric and are attractive for deployment in electromechanical systems.
机译:二维材料α-in_2se_3,在单层中具有平面外铁电性和压电性,打开微电机系统中智能材料集成的机会。然而,压电反应随着α-in_2se_3的厚度的降低而降低,阻碍了少层α-in_2se_3在机电变换中的应用。在这项工作中,我们通过构建IN_2SE_3 /过渡金属二甲基化物(TMDS)异质结构来报告一种策略来增强平面外压电系数。与单层IN_2SE_3相比,这种策略显示了较大的压电增强,并且在MOS_2 / IN_2SE_3中实现了2.9×10〜(-10)C / M的最大E_(31)。进一步构造一种现象学模型以将压电系数与异质结构的偏振连接。此外,诱导的偶极力矩强烈影响异质结构的带状结构,产生可调谐光吸收。建议的IN_2SE_3 / TMDS异质结构代表了未来高效压电的开发的创新策略,并且在机电系统中部署有吸引力。

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  • 来源
    《Physical review.B.Condensed matter and materials physics》 |2021年第7期|075449.1-075449.7|共7页
  • 作者单位

    School of Physics Sun Yat-sen University Guangzhou 510275 China State Key Laboratory of Optoelectronic Materials and Technologies Sun Yat-sen University Guangzhou 510275 China Centre for Physical Mechanics and Biophysics School of Physics Sun Yat-sen University Guangzhou 510275 China;

    School of Physics Sun Yat-sen University Guangzhou 510275 China State Key Laboratory of Optoelectronic Materials and Technologies Sun Yat-sen University Guangzhou 510275 China Centre for Physical Mechanics and Biophysics School of Physics Sun Yat-sen University Guangzhou 510275 China;

    School of Physics Sun Yat-sen University Guangzhou 510275 China State Key Laboratory of Optoelectronic Materials and Technologies Sun Yat-sen University Guangzhou 510275 China Centre for Physical Mechanics and Biophysics School of Physics Sun Yat-sen University Guangzhou 510275 China;

    School of Physics Sun Yat-sen University Guangzhou 510275 China;

    School of Physics Sun Yat-sen University Guangzhou 510275 China;

    School of Physics Sun Yat-sen University Guangzhou 510275 China State Key Laboratory of Optoelectronic Materials and Technologies Sun Yat-sen University Guangzhou 510275 China Centre for Physical Mechanics and Biophysics School of Physics Sun Yat-sen University Guangzhou 510275 China;

    School of Physics Sun Yat-sen University Guangzhou 510275 China State Key Laboratory of Optoelectronic Materials and Technologies Sun Yat-sen University Guangzhou 510275 China Centre for Physical Mechanics and Biophysics School of Physics Sun Yat-sen University Guangzhou 510275 China;

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