S=tanΨAcosΔAtanΨBcosΔBtan2ΨAsin2ΔAtan2ΨBsin2ΔB ]]>are calculated and- the refractive index n2 of the substrate (1) is calculated according to the following formula: <mrow><mi>n</mi><mo>=</mo><mfrac><mn>1</mn><mrow><msqrt><mn>2</mn></msqrt></mrow></mfrac><msqrt><mrow><mfrac><mrow><mrow><mo>(</mo><mrow><msubsup><mi>n</mi><mn>1</mn><mn>2</mn></msubsup><mo>+</mo><msubsup><mi>n</mi><mn>2</mn><mn>2</mn></msubsup></mrow><mo>)</mo></mrow><mfrac><mrow><msub><mi>E</mi><mn>2</mn></msub></mrow><mrow><msub><mi>E</mi><mn>1</mn></msub></mrow></mfrac><mo>−</mo><msubsup><mi>n</mi><mn>2</mn><mn>2</mn></msubsup><mrow><mo>(</mo><mrow><msubsup><mi>n</mi><mn>2</mn><mn>2</mn></msubsup><mo>−</mo><msubsup><mi>n</mi><mn>1</mn><mn>2</mn></msubsup></mrow><mo>)</mo></mrow><mo>+</mo><msqrt><mrow><msup><mrow><mrow><mo>(</mo><mrow><mfrac><mrow><msub><mi>E</mi><mn>2</mn></msub></mrow><mrow><msub><mi>E</mi><mn>1</mn></msub></mrow></mfrac><mo>−</mo><msubsup><mi>n</mi><mn>2</mn><mn>2</mn></msubsup></mrow><mo>)</mo></mrow></mrow><mn>2</mn></msup><msup><mrow><mrow><mo>(</mo><mrow><msubsup><mi>n</mi><mn>2</mn><mn>2</mn></msubsup><mo>−</mo><msubsup><mi>n</mi><mn>1</mn><mn>2</mn></msubsup></mrow><mo>)</mo></mrow></mrow><mn>2</mn></msup><mo>+</mo><mn>4</mn><msup><mrow><mrow><mo>(</mo><mrow><msub><mi>n</mi><mn>1</mn></msub><msub><mi>n</mi><mn>2</mn></msub></mrow><mo>)</mo></mrow></mrow><mn>4</mn></msup></mrow></msqrt></mrow><mrow><mfrac><mrow><msub><mi>E</mi><mn>2</mn></msub></mrow><mrow><msub><mi>E</mi><mn>1</mn></msub></mrow></mfrac><mo>+</mo><msubsup><mi>n</mi><mn>1</mn><mn>2</mn></msubsup></mrow></mfrac></mrow></msqrt></mrow> wherein <mrow><mfrac><mrow><msub><mi>E</mi><mn>2</mn></msub></mrow><mrow><msub><mi>E</mi><mn>1</mn></msub></mrow></mfrac><mo>=</mo><mfrac><mrow><msubsup><mi>n</mi><mn>2</mn><mn>2</mn></msubsup><mtext> cos</mtext><msub><mi mathvariant="normal">α</mi><mn>1</mn></msub></mrow><mrow><mtext>cos</mtext><msub><mi mathvariant="normal">α</mi><mn>2</mn></msub><mo>⋅</mo><mtext>cos</mtext><mrow><mo>(</mo><mrow><msub><mi mathvariant="normal">α</mi><mn>1</mn></msub><mo>−</mo><msub><mi mathvariant="normal">α</mi><mn>2</mn></msub></mrow><mo>)</mo></mrow></mrow></mfrac><mo>⋅</mo><mrow><mo>(</mo><mrow><mn>2</mn><mi>S</mi><mfrac><mrow><msub><mi>n</mi><mn>1</mn></msub></mrow><mrow><msub><mi>n</mi><mn>2</mn></msub></mrow></mfrac><mfrac><mrow><msup><mrow><mtext>sin</mtext></mrow><mn>2</mn></msup><msub><mi mathvariant="normal">α</mi><mn>1</mn></msub></mrow><mrow><mtext>cos</mtext><mrow><mo>(</mo><mrow><msub><mi mathvariant="normal">α</mi><mn>1</mn></msub><mo>−</mo><msub><mi mathvariant="normal">α</mi><mn>2</mn></msub></mrow><mo>)</mo></mrow></mrow></mfrac><mo>+</mo><mn>1</mn></mrow><mo>)</mo></mrow></mrow> andn="11"n1 the refractive index of the ambient medium,n2 the refractive index of the substrate (1),α1 the angle of incidence of the light andα2 = arcsin (sine α1 × n1/n2) are."/> Method for the determination of the index of refraction of a transparent layer by ellipsometry
首页> 外国专利> Method for the determination of the index of refraction of a transparent layer by ellipsometry

Method for the determination of the index of refraction of a transparent layer by ellipsometry

机译:椭偏法测定透明层折射率的方法

摘要

Method for the determination of the index of refraction of a transparent layer (2) which, mounted on a substrate (1) is applied, with the help of a ellipsometric method, with the following process steps:- it is a pair of the ellipsometric angle psi (ψA) and delta (δA) on the layer to be investigated, (2) in the case of a first, higher layer thickness is measured,- it is a pair of the ellipsometric angle psi (ψB) and delta (δB) on the layer to be investigated, (2) with the same angle of incidence (a) in the case of a second, lower layer thickness or an uncoated surface of the substrate (1) is measured,- from the four measured ellipsometric angles (ψA, ΨB, ΔA, ΔB) an intermediate value is <mrow><mi>S</mi><mo>=</mo><mfrac><mrow><mtext>tan</mtext><msub><mi mathvariant="normal">Ψ</mi><mi>A</mi></msub><mo>⋅</mo><mtext>cos</mtext><msub><mi>Δ</mi><mi>A</mi></msub><mo>−</mo><mtext>tan</mtext><msub><mi mathvariant="normal">Ψ</mi><mi>B</mi></msub><mo>⋅</mo><mtext>cos</mtext><msub><mi>Δ</mi><mi>B</mi></msub></mrow><mrow><msup><mrow><mtext>tan</mtext></mrow><mn>2</mn></msup><msub><mi mathvariant="normal">Ψ</mi><mi>A</mi></msub><mo>⋅</mo><msup><mrow><mtext>sin</mtext></mrow><mn>2</mn></msup><msub><mi>Δ</mi><mi>A</mi></msub><mo>−</mo><msup><mrow><mtext>tan</mtext></mrow><mn>2</mn></msup><msub><mi mathvariant="normal">Ψ</mi><mi>B</mi></msub><mo>⋅</mo><msup><mrow><mtext>sin</mtext></mrow><mn>2</mn></msup><msub><mi>Δ</mi><mi>B</mi></msub></mrow></mfrac></mrow> are calculated and- the refractive index n2 of the substrate (1) is calculated according to the following formula: <mrow><mi>n</mi><mo>=</mo><mfrac><mn>1</mn><mrow><msqrt><mn>2</mn></msqrt></mrow></mfrac><msqrt><mrow><mfrac><mrow><mrow><mo>(</mo><mrow><msubsup><mi>n</mi><mn>1</mn><mn>2</mn></msubsup><mo>+</mo><msubsup><mi>n</mi><mn>2</mn><mn>2</mn></msubsup></mrow><mo>)</mo></mrow><mfrac><mrow><msub><mi>E</mi><mn>2</mn></msub></mrow><mrow><msub><mi>E</mi><mn>1</mn></msub></mrow></mfrac><mo>−</mo><msubsup><mi>n</mi><mn>2</mn><mn>2</mn></msubsup><mrow><mo>(</mo><mrow><msubsup><mi>n</mi><mn>2</mn><mn>2</mn></msubsup><mo>−</mo><msubsup><mi>n</mi><mn>1</mn><mn>2</mn></msubsup></mrow><mo>)</mo></mrow><mo>+</mo><msqrt><mrow><msup><mrow><mrow><mo>(</mo><mrow><mfrac><mrow><msub><mi>E</mi><mn>2</mn></msub></mrow><mrow><msub><mi>E</mi><mn>1</mn></msub></mrow></mfrac><mo>−</mo><msubsup><mi>n</mi><mn>2</mn><mn>2</mn></msubsup></mrow><mo>)</mo></mrow></mrow><mn>2</mn></msup><msup><mrow><mrow><mo>(</mo><mrow><msubsup><mi>n</mi><mn>2</mn><mn>2</mn></msubsup><mo>−</mo><msubsup><mi>n</mi><mn>1</mn><mn>2</mn></msubsup></mrow><mo>)</mo></mrow></mrow><mn>2</mn></msup><mo>+</mo><mn>4</mn><msup><mrow><mrow><mo>(</mo><mrow><msub><mi>n</mi><mn>1</mn></msub><msub><mi>n</mi><mn>2</mn></msub></mrow><mo>)</mo></mrow></mrow><mn>4</mn></msup></mrow></msqrt></mrow><mrow><mfrac><mrow><msub><mi>E</mi><mn>2</mn></msub></mrow><mrow><msub><mi>E</mi><mn>1</mn></msub></mrow></mfrac><mo>+</mo><msubsup><mi>n</mi><mn>1</mn><mn>2</mn></msubsup></mrow></mfrac></mrow></msqrt></mrow> wherein <mrow><mfrac><mrow><msub><mi>E</mi><mn>2</mn></msub></mrow><mrow><msub><mi>E</mi><mn>1</mn></msub></mrow></mfrac><mo>=</mo><mfrac><mrow><msubsup><mi>n</mi><mn>2</mn><mn>2</mn></msubsup><mtext> cos</mtext><msub><mi mathvariant="normal">α</mi><mn>1</mn></msub></mrow><mrow><mtext>cos</mtext><msub><mi mathvariant="normal">α</mi><mn>2</mn></msub><mo>⋅</mo><mtext>cos</mtext><mrow><mo>(</mo><mrow><msub><mi mathvariant="normal">α</mi><mn>1</mn></msub><mo>−</mo><msub><mi mathvariant="normal">α</mi><mn>2</mn></msub></mrow><mo>)</mo></mrow></mrow></mfrac><mo>⋅</mo><mrow><mo>(</mo><mrow><mn>2</mn><mi>S</mi><mfrac><mrow><msub><mi>n</mi><mn>1</mn></msub></mrow><mrow><msub><mi>n</mi><mn>2</mn></msub></mrow></mfrac><mfrac><mrow><msup><mrow><mtext>sin</mtext></mrow><mn>2</mn></msup><msub><mi mathvariant="normal">α</mi><mn>1</mn></msub></mrow><mrow><mtext>cos</mtext><mrow><mo>(</mo><mrow><msub><mi mathvariant="normal">α</mi><mn>1</mn></msub><mo>−</mo><msub><mi mathvariant="normal">α</mi><mn>2</mn></msub></mrow><mo>)</mo></mrow></mrow></mfrac><mo>+</mo><mn>1</mn></mrow><mo>)</mo></mrow></mrow> andn="11"n1 the refractive index of the ambient medium,n2 the refractive index of the substrate (1),α1 the angle of incidence of the light andα2 = arcsin (sine α1 × n1/n2) are.
机译:用于确定安装在基板(1)上的透明层(2)的折射率的方法,借助于椭圆光度法,其步骤如下:-这是一对椭圆光度法在要研究的层上的角度psi(ψ A )和增量(δ A ),(2)在第一个较高的层厚的情况下,它是要研究的层上的一对椭圆角psi(ψ B )和增量(δ B ),(2)具有相同的入射角( a)在第二个较低的层厚度或基材(1)的未涂层表面的情况下,-从四个测得的椭圆角度(ψ A ,Ψ B ,Δ A ,Δ B )的中间值是 <![CDATA [ S = tan < / mtext> Ψ A cos Δ A tan Ψ B cos Δ B < / msub> tan 2 Ψ A sin 2 Δ A - tan 2 Ψ B ⋅< / mo> sin 2 Δ B ]]> ,并且-基材的折射率n 2 (1 )是根据以下公式计算的: <![CDATA [ n = 1 2 < mrow> n 1 2 + n 2 2 E 2 E 1 n 2 2 n 2 2 - n 1 2 + E 2 < / mn> E 1 -< / mo> n 2 2 2 n 2 2 n 1 2 2 + 4 n 1 n 2 4 E 2 E 1 + n 1 2 ]]> 其中 <![CDATA [ E 2 E 1 = n 2 2 cos α 1 cos α 2 cos α 1 α 2 2 S n 1 < / mrow> n 2 < mtext> sin 2 α 1 cos α 1 α 2 + 1 ]]> andn =“ 11” n 1 的环境介质的折射率,n 2 的基板(1)的折射率,α 1 的入射角光线和α 2 =反正弦(正弦α 1 ×n 1 / n 2 )。

著录项

  • 公开/公告号DE102015105418B4

    专利类型

  • 公开/公告日2018-10-04

    原文格式PDF

  • 申请/专利权人 UNIVERSITÄT GREIFSWALD;

    申请/专利号DE201510105418

  • 发明设计人 PETER NESTLER;CHRISTIANE A. HELM;

    申请日2015-04-09

  • 分类号G01N21/21;G01B11/06;G01N21/41;G01N21/95;

  • 国家 DE

  • 入库时间 2022-08-21 12:35:00

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