• Chinese Optics Letters
  • Vol. 19, Issue 3, 031201 (2021)
Shaomin Li and Liqun Sun*
Author Affiliations
  • State Key Laboratory of Precision Measurement Technology and Instruments, Department of Precision Instruments, Tsinghua University, Beijing 100084, China
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    DOI: 10.3788/COL202119.031201 Cite this Article Set citation alerts
    Shaomin Li, Liqun Sun. Natural logarithm wavelength modulation spectroscopy[J]. Chinese Optics Letters, 2021, 19(3): 031201 Copy Citation Text show less

    Abstract

    Natural logarithm wavelength modulation spectroscopy (ln-WMS) is demonstrated in this Letter. Unlike the conventional wavelength modulation spectroscopy (WMS)-2f technique, it is a linear method even for large absorbance, which is the core advantage of ln-WMS. The treating method used in ln-WMS is to take the natural logarithm of the transmitted intensity. In order to determine the proper demodulation phase, the η-seeking algorithm is introduced, which minimizes the absolute value of the first harmonic within the non-absorbing region. Subsequently, the second harmonic of the absorption signal is extracted by setting the demodulating phase as 2η. To illustrate the validity of ln-WMS, it was applied to water vapor experimentally. The result shows that even if the absorbance (base-e) is between 1.60 and 6.26, the linearity between ln-WMS-2f and volume fraction is still established. For comparison, measurement with conventional WMS-2f was also done, whose response no longer kept linearity. The η values retrieved in continuous measurements and the residuals were shown so as to evaluate the performance of the η-seeking algorithm. Time consumed by this algorithm was roughly 0.28 s per measurement. As an alternative WMS strategy, ln-WMS has a wide range of potential applications, especially where the absorbance is large or varies over a wide area.
    FM:v(t)=v¯+acos(ωt+ψ+ϕ),

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    AM:I0(t)=I¯0[1+i1cos(ωt+ψ)],

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    It(t)=I0(t)exp[α(ν)CL],

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    lnIt(t)=lnI0(t)α(ν)CL=lnI¯0+ln[1+i1cos(ωt+ψ)]α(ν)CL.

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    ln(1+x)=n=1(1)n+1nxn,x1,

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    ln[1+i1cos(ωt+ψ)]=n=1(1)n+1ni1n[cos(ωt+ψ)]n=n=0pncos[n(ωt+ψ)].

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    α[ν¯+acos(ωt+ψ+ϕ)]CL=k=0Hkcos[k(ωt+ψ+ϕ)],

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    H0(v¯,a)=CL2πππα(v¯+acosθ)dθ,

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    Hk(v¯,a)=CLπππα(v¯+acosθ)coskθdθ,k1.

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    lnIt=lnI¯0+n=0pncos[n(ωt+ψ)]k=0Hkcos[k(ωt+ψ+ϕ)].

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    lnItNA=lnI¯0+n=0pncos[n(ωt+ψ)].

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    R1fNA=[lnItNA×cos(ωt+η)]lowpass=12p1cos(ψη),

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    ψη=π2+jπ,j=0,±1,±2,.

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    R2f=[lnIt×cos(2ωt+2η)]lowpass=12p2cos(2ψ2η)12H2cos(2ψ+2ϕ2η).

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    R2f=12p2+12H2cos(2ϕ).

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    Shaomin Li, Liqun Sun. Natural logarithm wavelength modulation spectroscopy[J]. Chinese Optics Letters, 2021, 19(3): 031201
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