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Microwave Properties of Parallel Plate Capacitors based on (Ba,Sr)TiO_3 Thin Films Grown on SiO_2.Al_2O_3 Substrates

机译:基于(BA,SR)TiO_3薄膜在SiO_2.Al_2O_3基板上生长的平行板电容器微波特性

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Ba_(0.7)Sr_(0.3)TiO_3 (BST) single and quadruple layer capacitors with Pt electrodes were fabricated together on polycrystalline alumina substrates with a SiO_2-based multicomponent amorphous buffer layer (SiO_2/Al_2O_3). This paper presents the results of the characterization of these capacitors, to demonstrate their suitability for application as decoupling (high value) capacitors and as components in tunable RF applications (e.g., phase shifters and filters). BST films of different compositions, (Ba_(0.7)Sr_(0.3))TiO_3 and (Ba_(0.5)Sr_(0.5))TiO_3, were grown by metal-organic decomposition (MOD) and RF magnetron reactive sputtering. The capacitance density of 90-140 nm thick BST films was in the range of 20 to 70 fF/μm~2. Parallel plate capacitors with areas from 16 μm~2 to 2.25 mm~2 were fabricated using photolithography and ion milling techniques. For large capacitors (0.125 to 2.25 mm~2), capacitance and tan5 were measured at low frequencies (1 KHz - 1 MHz) using an LCR meter. Smaller capacitors (16 μm~2 to 3600 μm~2) were additionally characterized in the frequency range of 50 MHz - 20 GHz. In such case, capacitance, tanδ and equivalent series resistance (ESR) were extracted from two port scattering parameters obtained using a vector network analyzer (VNA). The relationship between dielectric loss, tunability and calculated figure of merit vs. BST composition and deposition temperature was outlined. In addition, loss and ESR at high frequencies was investigated. The typical achieved leakage current density of sputtered BST films for 2.25 mm~2 capacitors fabricated on SiO_2/Al_2O_3 was 7.3x10~(-9) A/cm~2 at 300 kV/cm (65 fF/μm~2), about 2 times lower than for (Ba_(0.7)Sr_(0.3))TiO_3 films deposited by MOD (1.4x10~(-8)A/cm~2 at 300 kV/cm, 34.5 fF/μm~2). Furthermore, the tunability of (Ba_(0.7)Sr_(0.3))TiO_3 deposited by both methods on SiO_2/Al_2O_3 was ~60% at 350 kV/cm.
机译:Ba_(0.7)SR_(0.3)TiO_3(BST)单晶层电容器在具有Pt电极的与基于SiO_2的多组分无定形缓冲层(SiO_2 / Al_2O_3)的多晶氧化铝底物上一起制造。本文介绍了这些电容器的表征的结果,以证明其适用于应用作为解耦(高值)电容器和可调RF应用中的组件(例如,相移器和滤波器)。 BST膜的不同组合物(Ba_(0.7)Sr_(0.3))TiO_3和(Ba_(0.5)Sr_(0.5))TiO_3被金属 - 有机分解(MOD)和RF磁控溅射溅射生长。 90-140nm厚的BST膜的电容密度在20至70ff /μm〜2的范围内。使用光刻和离子铣削技术制造具有16μm〜2至2.25mm〜2的平行板电容器。对于大电容器(0.125至2.25mm〜2),使用LCR表以低频(1 kHz - 1MHz)测量电容和TAN5。较小的电容器(16μm〜2至3600μm〜2)另外表征为50 MHz - 20 GHz的频率范围。在这种情况下,从使用矢量网络分析器(VNA)获得的两个端口散射参数中提取电容,TANδ和等效串联电阻(ESR)。概述了介电损耗,可调节性和计算值与BST组合物和沉积温度的关系。此外,研究了高频下的损失和ESR。在SiO_2 / Al_2O_3上制造的2.25mm〜2电容器的诸如溅射的BST薄膜的典型泄漏电流密度为300kV / cm(65ff /μm〜2),约为7.3x10〜(-9)a / cm〜2。时间低于(BA_(0.7)SR_(0.3))TiO_3沉积的薄膜(1.4×10〜(-8)A / cm〜2,300kV / cm,34.5ff /μm〜2)。此外,通过两种方法在SiO_2 / Al_2O_3上沉积的(Ba_(0.7)Sr_(0.3))TiO_3的可调节性为350kV / cm的60%。

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