首页> 外国专利> Method and Instrument for Measuring Complex Dielectric Constant of a Sample by Optical Spectral Measurement

Method and Instrument for Measuring Complex Dielectric Constant of a Sample by Optical Spectral Measurement

机译:用光谱测量法测量样品复介电常数的方法和仪器

摘要

A substrate in a parallelepiped plate form satisfies an interference condition when incident light has a wavelength (λ) fallen under the following (d: thickness, n: refractive index, θ: incident angle, N: integer). ; <math overflow="scroll"><mtable><mtr><mtd><mrow><mfrac><mrow><mn>2</mn><mo></mo><mi>nd</mi><mo></mo><msqrt><mrow><mn>1</mn><mo>-</mo><msup><mrow><mo>(</mo><mrow><mi>sin</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mrow><mi>θ</mi><mo>/</mo><mi>n</mi></mrow></mrow><mo>)</mo></mrow><mn>2</mn></msup></mrow></msqrt></mrow><mi>λ</mi></mfrac><mo>=</mo><mi>N</mi></mrow></mtd><mtd><mrow><mo>[</mo><mrow><mi>Equation</mi><mo></mo><mstyle><mspace width="0.8em" height="0.8ex" /></mstyle><mo></mo><mn>7</mn></mrow><mo>]</mo></mrow></mtd></mtr></mtable></math> ;At this time, the light in a transmission spectrum is intensified to cause a fringe peak to appear, whereas the light in a reflection spectrum is weakened to provide a fringe valley. At around the wavelength (frequency), as the incident angle is increased, the transmittance nears zero while reflectance increases nearing 1. Increasing the thickness of the substrate by placing a thin film thereon is similar to the increase in the substrate thickness in [Equation 7], whereby the wavelength satisfying the interference condition shifts toward the longer wavelength (lower frequency) Due to the three effects, at a great incident angle, a ratio of an optical (transmission or reflection) spectrum of a system having a substrate and thin film to an optical spectrum of a substrate only becomes a spectrum having a structure wherein maximum and minimum values are adjacent to each other. By analyzing this relative transmission spectrum or relative reflection spectrum, a complex dielectric constant of the thin film can be determined.
机译:当入射光的波长(λ)低于以下(d:厚度,n:折射率,θ:入射角,N:整数)时,平行六面体板状的基板满足干涉条件。 ; <![CDATA [<数学溢出=“ scroll”> 2 nd 1 - sin θ / n < mn> 2 λ = N [ 方程式 7 ] ]]> ;这时,透射光谱中的光被增强以导致出现条纹峰,而反射光谱中的光被减弱以提供条纹谷。在波长(频率)附近,随着入射角的增加,透射率接近于零,而反射率则接近于1。通过在其上放置薄膜来增加基板的厚度类似于[等式7]中基板厚度的增加。 ],从而满足干涉条件的波长向长波长(低频)移动。由于这三种作用,在大入射角下,具有基板和薄膜的系统的光学(透射或反射)光谱之比基板的光谱仅变为具有最大值和最小值彼此相邻的结构的光谱。通过分析该相对透射光谱或相对反射光谱,可以确定薄膜的复介电常数。

著录项

  • 公开/公告号US2008013070A1

    专利类型

  • 公开/公告日2008-01-17

    原文格式PDF

  • 申请/专利权人 ETSUO KAWATE;

    申请/专利号US20040579781

  • 发明设计人 ETSUO KAWATE;

    申请日2004-11-22

  • 分类号G01J3/00;G01J4/00;G01N21/00;

  • 国家 US

  • 入库时间 2022-08-21 20:15:59

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