用宽频带反射声显微镜完全表征薄膜和厚膜材料

C. Lee, C. Tsai, Xin Cheng
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引用次数: 30

摘要

本文介绍了一种利用宽手反射声学显微镜对沉积在衬底上的薄膜和厚膜材料进行完整表征的方法。搭建了频率范围为50 ~ 175 MHz的宽带反射声显微镜进行实验验证。测量薄膜-衬底复合材料反射系数的振幅与声波频率的关系,以确定当薄膜厚度等于声波波长的四分之一时试样的共振频率。然后测量了谐振频率处反射系数的幅值和相位。利用这三个测量量,薄膜材料的厚度、声速和质量密度可以在没有任何先验知识的情况下同时确定。使用该方法表征了两种类型的薄膜材料,即溅射在蓝宝石衬底上的耐热玻璃薄膜和涂覆在耐热玻璃衬底上的正光刻胶。测得的三个声学参数,即膜厚、声速和质量密度,与已发表的数值吻合较好。在显微镜的频率范围内,大多数无机材料的可测膜厚度范围为30pm至5pm,大多数有机材料的可测膜厚度范围为10pm至2pm。在显微镜最高工作频率下,当膜厚小于声波波长的四分之一时,无法识别共振频率。然而。三个声学参数中的一个或两个仍然可以通过测量反射系数在固定声频下的振幅和相位来确定。这种能力已经通过在熔融石英上沉积的金fdm和在x切割LiNbOj衬底上蒸发的铝膜来证明。另外三个中心频率交错的换能器/透镜组也正在组装中,以覆盖从175 MHz到1000 MHz的整个频率范围,以便薄膜厚度的可测量范围可以扩展到亚微米区域。结果表明,该表征方法对微电子中薄膜和厚膜材料的无损研究具有重要的实用价值。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Complete Characterization of Thin- And Thick-Film Materials Using Wideband Reflection Acoustic Microscopy
Abslmcf-A methodology for complete characterization of thinand thick-film materials deposited on a substrate using widehand reflection acoustic microscopy is presented. A wideband reflection acoustic microscope that covers the frequency range of 50 to 175 MHz was constructed to carry out the experimental verification. The amplitude of the reflection coefficient of the film-substrate composite was measured versus the acoustic frequency to identify the resonant frequency of the specimen at which the film thickness is equal to one quarter of the acoustic wavelength. Then both the amplitude and the phase of the reflection coefficient at the resonant frequency were measured. Using the three measured quantities, thickness, acoustic velocity, and mass density of the film material are simultaneously determined without any prior knowledge. Two types of film materials, namely Pyrex glass film sputtered on a sapphire substrate and positive photoresist coated on a Pyrex glass substrate have been characterized using the methodology. The three measured acoustic parameters, film thickness, acoustic velocity, and mass density, agree well with the published values. For the frequency range of the microscope utilized the corresponding range of measurable film thickness is 30 pm to 5 pm for most inorganic materials, and 10 pm to 2 pm for most organic materials. For the case in which the film thickness is less than one quarter of the acoustic wavelength at the highest operation frequency of the microscope, the resonant frequency cannot be identified. However. one or two of the three acoustic parameters can still be determined by measuring the amplitude and the phase of the reflection coefficient a t a fixed acoustic frequency. This capability has been demonstrated using a gold fdm deposited on fused quartz and an aluminum film evaporated on X-cut LiNbOj substrate. Three additional transducer/lens sets with staggered center frequencies are also being assembled to cover the entire frequency range from 175 MHz t o 1000 MHz so that the measurable range of the film thickness can be extended to the submicron region. Consequently, it is concluded that this characterization methodology should he highly useful For nondestructive study of thinand thick-film materials in microelectronics.
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