• Chinese Optics Letters
  • Vol. 20, Issue 9, 091201 (2022)
Yunlong Zhu1,2, Zhuoran Li1,2, Xu Lu1,2, Yonggui Yuan1,2,*, and Jun Yang2,3,4,**
Author Affiliations
  • 1Key Laboratory of In-fiber Integrated Optics, Ministry of Education of China, Harbin Engineering University, Harbin 150001, China
  • 2College of Physics and Optoelectronic Engineering, Harbin Engineering University, Harbin 150001, China
  • 3Guangdong Provincial Key Laboratory of Information Photonics Technology (Guangdong University of Technology), Guangzhou 510006, China
  • 4School of Information Engineering, Guangdong University of Technology, Guangzhou 510008, China
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    DOI: 10.3788/COL202220.091201 Cite this Article Set citation alerts
    Yunlong Zhu, Zhuoran Li, Xu Lu, Yonggui Yuan, Jun Yang, "White light interferometry with spectral-temporal demodulation for large-range thickness measurement," Chin. Opt. Lett. 20, 091201 (2022) Copy Citation Text show less

    Abstract

    Film thickness measurement can be realized using white light interferometry, but it is challenging to guarantee high precision in a large range of thicknesses. Based on scanning white light interferometry, we propose a spectral-temporal demodulation scheme for large-range thickness measurement. The demodulation process remains unchanged for either coatings or substrate-free films, while some adjustments are made according to the estimated optical thickness. Experiments show that the single-point repeatabilities for 500 nm SiO2 coating and 68 µm substrate-free Si film are no more than 0.70 nm and 1.22 nm, respectively. This method can be further developed for simultaneous measurement of surface profile and film thickness.
    E0(k)=A0(k)eiθ(k),

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    E1(k)=rp(k)E0(k)+(1rp2(k))r(k)E0(k)eikL,

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    R(k)=|r(k)|2,

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    r(k)=r1(k)+r2(k)e2ikn1(k)d1+r1(k)r2(k)e2ikn1(k)d,

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    r1(k)=1n1(k)1+n1(k),

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    r2(k)=n1(k)n2(k)n1(k)+n2(k).

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    Rp(k)=|rp(k)|2=rp2(k),

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    Tp(k)=1Rp(k)=1rp2(k).

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    E(k,S)=q1E1(k)+q2E1(k)eikS=E0(k)(rp+Tp(k)r(k)eikL)(q1+q2eikS),

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    I(S)=k|E(k,S)|2=kA02(k)|rp(k)q1+rp(k)q2eikS+Tp(k)|r(k)|q1eikL+iφ(k)+Tp(k)|r(k)|q2eik(L+S)+iφ(k)|2,

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    If(S)=4q1q2kA02(k)(U1(k)+U2(k)+U3(k)),

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    U1(k)=(Rp(k)+Tp2(k)R(k))coskS,

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    U2(k)=rp(k)Tp(k)|r(k)|cos(k(L+S)+φ(k)),

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    U3(k)=rp(k)Tp(k)|r(k)|cos(k(LS)+φ(k)).

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    F(k)=4q1q2A02(k)(Rp(k)+Tp2(k)R(k)).

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    Fp(k)=4q1q2A02(k)Rp(k).

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    Fref(k)=4q1q2A02(k)(Rp(k)+Tp2(k)Rref(k)),

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    Rref(k)=|rref(k)|2=(1nref(k)1+nref(k))2.

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    R(k)=F(k)Fp(k)Fref(k)Fp(k)Rref(k).

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    W(din)=k|Rth(din,k)R(k)|2,

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    Δdλc2ng(λc),

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    dini=d0±mΔd,

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    α(k)=arg(Hilbert(R(k))).

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    β(k)=cos(α(k)).

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    Yunlong Zhu, Zhuoran Li, Xu Lu, Yonggui Yuan, Jun Yang, "White light interferometry with spectral-temporal demodulation for large-range thickness measurement," Chin. Opt. Lett. 20, 091201 (2022)
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