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首页> 外文期刊>Bulletin of the American Physical Society >APS -Joint Fall 2017 Meeting of the Texas Section of the APS, Texas Section of the AAPT, and Zone 13 of the Society of Physics Students- Event - Field-Effect Tunable Epsilon-Near-Zero Perfect Absorption.
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APS -Joint Fall 2017 Meeting of the Texas Section of the APS, Texas Section of the AAPT, and Zone 13 of the Society of Physics Students- Event - Field-Effect Tunable Epsilon-Near-Zero Perfect Absorption.

机译:APS-APS得克萨斯分部,AAPT得克萨斯分部以及物理学生协会第13区的2017年秋季联合会议-事件-场效应可调谐Epsilon-Near-Zero完美吸收

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High efficient light absorbers are in demand for light harvesting, high-resolution, and optical coating technologies. Recent studies suggest that zero-index or epsilon-near-zero (ENZ) materials can be used in making ultrathin perfect absorbers. Indium tin oxide (ITO) with electron concentration controllable over a broad range of 5exttimes 10$^{mathrm{20}}$-2exttimes 10$^{mathrm{21}}$ cm$^{mathrm{-3}}$ shows ENZ in the near-IR region of 700 nm -1.8~$mu $m. The ultrathin layers of ITO support certain plasmonic modes at ENZ frequencies. Excitation of these modes leads to resonant light absorption with 100{%} efficiency. In this talk, we show, for the first time, post-fabrication tuning of the ENZ perfect absorption in ITO thin film. We will discuss perfect absorption in deep subwavelength ($lambda $/100) ITO nanolayers due to the excitation of the bound and radiative ENZ modes. The nanolayer thickness required for the mode critical coupling and perfect absorption is computed for each ENZ mode and used to evaluate the optimal thickness for the perfect absorption tuning. The resonant absorption wavelength is tunable via the field-effect in a metal-oxide-semiconductor (MOS) capacitor. The direct tuning of the perfect absorption is possible due to the subwavelength thickness (extless 8 nm) of the ENZ perfect absorber - comparable to the Debye length (extasciitilde 1 nm) of the electron accumulation region. The post-fabrication tuning of about 20{%} of perfect absorption with respect to the full width at half maximum of the absorption peak is achieved for the devices under study.
机译:对于光收集,高分辨率和光学镀膜技术,需要高效的光吸收器。最近的研究表明,零折射率或epsilon-near-zero(ENZ)材料可用于制造超薄完美吸收体。电子浓度可控制在5倍10 $ ^ {mathrm {20}} $-2倍10 $ ^^ {mathrm {21}} $ cm $ ^ {mathrm {-3}} $范围内的铟锡氧化物(ITO)显示ENZ在700 nm -1.8〜$ mu $ m的近红外区域。 ITO的超薄层在ENZ频率下支持某些等离子体模式。激发这些模式会导致共振光吸收,效率达到100%。在本次演讲中,我们首次展示了ITO薄膜中ENZ完美吸收的制造后调整。由于束缚和辐射ENZ模式的激发,我们将讨论在深亚波长($λ$ / 100)ITO纳米层中的完美吸收。为每个ENZ模式计算出模式临界耦合和理想吸收所需的纳米层厚度,并用于评估理想吸收调谐的最佳厚度。谐振吸收波长可通过场效应在金属氧化物半导体(MOS)电容器中进行调节。由于ENZ完美吸收体的亚波长厚度(至少8纳米),可以直接调节完美吸收,这与电子累积区域的德拜长度(埃西替尼1纳米)相当。对于所研究的器件,制造后相对于吸收峰半峰全宽的约20 {%}的理想吸收实现了调谐。

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