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外延TiMgN(001)层的可调谐红外等离子体特性

Tunable Infrared Plasmonic Properties of Epitaxial TiMgN(001) Layers.

作者信息

Wang Baiwei, Nawarat Poomirat, Lewis Kim Michelle, Patsalas Panos, Gall Daniel

机构信息

Department of Materials Science and Engineering, Rensselaer Polytechnic Institute, Troy, New York 12180, United States.

Department of Physics, Applied Physics, and Astronomy, Rensselaer Polytechnic Institute, Troy, New York 12180, United States.

出版信息

ACS Appl Mater Interfaces. 2021 May 19;13(19):22738-22748. doi: 10.1021/acsami.1c03667. Epub 2021 May 5.

DOI:10.1021/acsami.1c03667
PMID:33949846
Abstract

Optical transmission and reflection spectra in combination with ellipsometry and transport measurements on epitaxial rocksalt structure TiMgN(001) layers with 0.00 ≤ ≤ 0.49 are employed to explore their potential as refractory infrared plasmonic materials. A red shift in the reflection edge ℏω from 2.0 to 0.8 eV and the corresponding unscreened plasma energy ℏω from 7.6 to 4.7 eV indicate a linear reduction in the free carrier density with increasing . However, nitrogen vacancies in Mg-rich samples act as donors, resulting in a minimum = 1.6 × 10 cm for = 0.49. Photoelectron valence band spectra confirm the diminishing conduction band density of states and indicate a 0.9 eV decrease in the Fermi level as increases from 0 to 0.49. The dielectric function ε = ε + iε can be divided into a low-energy spectral region where intraband transitions result in large negative and positive ε and ε, respectively, and a higher energy interband transition region with both ε and ε > 0. The screened plasma energy that separates these two regions red-shifts from 2.6 to 1.3 eV for = 0-0.39, indicating a tunable plasmonic activity that extends from the visible to the infrared (470-930 nm). Electron transport measurements indicate a metallic temperature coefficient of resistivity (TCR) for TiN-rich alloys with ≤ 0.26 but weak carrier localization and a negative TCR <60 K for = 0.39 and <300 K for = 0.49, attributed to Mg alloying-induced disorder. The plasmonic quality factor is approximately an order of magnitude larger than what was previously reported for polycrystalline TiMgN, making TiMgN(001) layers competitive with TiScN(001).

摘要

采用光透射和反射光谱,结合椭圆偏振光谱法以及对0.00≤x≤0.49的外延岩盐结构TiMgN(001)层进行的输运测量,来探究它们作为难熔红外等离子体材料的潜力。反射边ħω从2.0 eV红移至0.8 eV,相应的未屏蔽等离子体能量ħω从7.6 eV降至4.7 eV,这表明随着x增加,自由载流子密度n呈线性降低。然而,富镁样品中的氮空位充当施主,导致x = 0.49时n的最小值为1.6×10²¹ cm⁻³。光电子价带光谱证实了导带态密度的减小,并表明随着x从0增加到0.49,费米能级降低了0.9 eV。介电函数ε = ε₁ + iε₂可分为一个低能光谱区域,其中带内跃迁分别导致ε₁为大的负值和ε₂为大的正值,以及一个高能带间跃迁区域,其中ε₁和ε₂均大于0。分隔这两个区域的屏蔽等离子体能量ħωₚ从2.6 eV红移至1.3 eV(x = 0 - 0.39),表明等离子体活性可调,范围从可见光延伸至红外光(470 - 930 nm)。电子输运测量表明,x≤0.26的富TiN合金具有金属电阻率温度系数(TCR),但载流子局域化较弱;x = 0.39时TCR为负且小于60 K,x = 0.49时小于300 K,这归因于Mg合金化引起的无序。等离子体品质因数Q比之前报道的多晶TiMgN大约大一个数量级,使得TiMgN(001)层与TiScN(001)具有竞争力。

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