Theory - 版の履歴

2022年3月4日 (金) 02:07にLwangによる

2022-03-04T02:07:51Z

← 古い版		2022年3月4日 (金) 02:07時点における版
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	The initial value of <math> \nu_1 </math>, <math> \Gamma_1 </math> and <math> A_1 </math> are set to be the optimized value in the last fitting procedure.		The initial value of <math> \nu_1 </math>, <math> \Gamma_1 </math> and <math> A_1 </math> are set to be the optimized value in the last fitting procedure.
	The initial value of <math> \nu_2 </math> is set to the wavenumber of minimum (or maximum) value of difference reflectance spectra.		The initial value of <math> \nu_2 </math> is set to the wavenumber of minimum (or maximum) value of difference reflectance spectra.
	The initial parameter for <math> \Gamma_2 </math> and <math> A_2 </math> is set to be 15 <math> \text{cm}^{-1} </math> and <math> A_1/2 \text{cm}^{-1} </math>, respectively.		The initial parameter for <math> \Gamma_2 </math> and <math> A_2 </math> is set to be 15 <math> \text{cm}^{-1} </math> and <math> 0.5 A_1 \text{cm}^{-1} </math>, respectively.
	A smaller initial value of <math> A_2 </math> suggests that the second Lorentz function is a minor adsorption band in ATR-IR spectra.		A smaller initial value of <math> A_2 </math> suggests that the second Lorentz function is a minor adsorption band in ATR-IR spectra.
	Then all parameters are again optimized using the same fitting procedure.		Then all parameters are again optimized using the same fitting procedure.

2022年2月17日 (木) 09:02にLwangによる

2022-02-17T09:02:13Z

← 古い版		2022年2月17日 (木) 09:02時点における版
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	The first Lorentz function is used to fit the strongest adsorption band in the target region.		The first Lorentz function is used to fit the strongest adsorption band in the target region.
	Thus, the initial parameter for <math> \nu_1 </math> is set to the wavenumber of minimum value of reflectance in the experimental data.		Thus, the initial parameter for <math> \nu_1 </math> is set to the wavenumber of minimum value of reflectance in the experimental data.
	The initial parameter for <math> \Gamma_1 </math> and <math> A_1 </math> is set according to the ~~linesharp~~ of strongest adsorption band in ATR-IR spectra.		The initial parameter for <math> \Gamma_1 </math> and <math> A_1 </math> are set according to the lineshape of strongest adsorption band in ATR-IR spectra.

	After the first fitting procedure, the strongest adsorption band is expected to be well represented.		After the first fitting procedure, the strongest adsorption band is expected to be well represented.

2022年2月17日 (木) 08:59にLwangによる

2022-02-17T08:59:11Z

2022年2月15日 (火) 02:05にLwangによる

2022-02-15T02:05:10Z

← 古い版		2022年2月15日 (火) 02:05時点における版
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	: <math>n_j^0(\lambda) = A + \frac{B}{{\lambda}^2} + \frac{C}{{\lambda}^4}</math>		: <math>n_j^0(\lambda) = A + \frac{B}{{\lambda}^2} + \frac{C}{{\lambda}^4}</math>
	The obtained parameters <math>A, B, C</math> were used to evaluate the nonresnant refractive index at 5000 <math> \text{cm}^{-1} </math>.		The obtained parameters <math>A, B, C</math> were used to evaluate the nonresnant refractive index at 5000 <math> \text{cm}^{-1} </math>.
	It is also possible to directly use the refractive index in the visible region, which may involve ~~some~~ deviation in <math> n_j^0 </math>. <ref name = "ref2" />		It is also possible to directly use the refractive index in the visible region, which may involve a slightly deviation in <math> n_j^0 </math>. <ref name = "ref2" />

	After the determination of <math> n_j^0 </math>, other parameters related to the Lorentz functions are determined by minimizing the least-squares residual (LSR) between the experimental reflectance spectra and those of the analytical formulas over the whole wavenumber region of the target vibrational band. The residual is defined by		After the determination of <math> n_j^0 </math>, other parameters related to the Lorentz functions are determined by minimizing the least-squares residual (LSR) between the experimental reflectance spectra and those of the analytical formulas over the whole wavenumber region of the target vibrational band. The residual is defined by

2022年2月14日 (月) 05:09にLwangによる

2022-02-14T05:09:25Z

← 古い版		2022年2月14日 (月) 05:09時点における版
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	<div id="ATR-IR data" style="font-size: 200%;"> Calculated reflectance of ATR-IR from complex refractive index </div>		----

			<div id="ATR-IR data" style="font-size: 200%;font-style:bold;"> Calculated reflectance of ATR-IR from complex refractive index </div>

	~~----~~
	[[File:Light.png\|500px]]		[[File:Light.png\|500px]]

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	The number of Lorentz functions keeps increasing and the whole procedure is repeated until the final LSR reaches the set tolerance.		The number of Lorentz functions keeps increasing and the whole procedure is repeated until the final LSR reaches the set tolerance.

			----

	<div style="font-size: 200%;"> References </div>		<div style="font-size: 200%;"> References </div>

2022年1月25日 (火) 01:15にLwangによる

2022-01-25T01:15:53Z

← 古い版		2022年1月25日 (火) 01:15時点における版
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	In the beginning, <math> n_j^0 </math> should be determined before the fitting procedure. <math> n_j^0 </math> is the nonresonant refractive index in the IR wavenumber region.		In the beginning, <math> n_j^0 </math> should be determined before the fitting procedure. <math> n_j^0 </math> is the nonresonant refractive index in the IR wavenumber region.
	In the reference paper ~~cite{wang}~~, we use the refractive index values in the visible regions to fit Cauchy's equation.		In the reference paper <ref name = "ref2" />, we use the refractive index values in the visible regions to fit Cauchy's equation.
	: <math>n_j^0(\lambda) = A + \frac{B}{{\lambda}^2} + \frac{C}{{\lambda}^4}</math>		: <math>n_j^0(\lambda) = A + \frac{B}{{\lambda}^2} + \frac{C}{{\lambda}^4}</math>
	The obtained parameters <math>A, B, C</math> were used to evaluate the nonresnant refractive index at 5000 <math> \text{cm}^{-1} </math>.		The obtained parameters <math>A, B, C</math> were used to evaluate the nonresnant refractive index at 5000 <math> \text{cm}^{-1} </math>.

2022年1月21日 (金) 02:08にLwangによる

2022-01-21T02:08:41Z

← 古い版		2022年1月21日 (金) 02:08時点における版
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	The number of Lorentz functions keeps increasing and the whole procedure is repeated until the final LSR reaches the set tolerance.		The number of Lorentz functions keeps increasing and the whole procedure is repeated until the final LSR reaches the set tolerance.


			<div style="font-size: 200%;"> References </div>

	<references>		<references>

2022年1月21日 (金) 02:02にLwangによる

2022-01-21T02:02:16Z

← 古い版		2022年1月21日 (金) 02:02時点における版
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	The number of Lorentz functions keeps increasing and the whole procedure is repeated until the final LSR reaches the set tolerance.		The number of Lorentz functions keeps increasing and the whole procedure is repeated until the final LSR reaches the set tolerance.


	<references>		<references>

	<ref name = "ref1">"Theory of Sum Frequency Generation Spectroscopy"		<ref name = "ref1">"Theory of Sum Frequency Generation Spectroscopy"
	Akihiro Morita. Springer Nature Singapore Pte Ltd: 2018 </ref>		Akihiro Morita. Springer Nature Singapore Pte Ltd: 2018 </ref>
	<ref name = "ref2">"Dispersion of Complex Refractive Indices for Intense Vibrational Bands. I Quantitative Spectra"		<ref name = "ref2">"Dispersion of Complex Refractive Indices for Intense Vibrational Bands. I Quantitative Spectra"
	Ryo Murata, Ken-ichi Inoue, Lin Wang, Shen Ye, and Akihiro Morita, J. Phys. Chem. B, 125(34), 9794-9803 (2021).</ref>		Ryo Murata, Ken-ichi Inoue, Lin Wang, Shen Ye, and Akihiro Morita, J. Phys. Chem. B, 125(34), 9794-9803 (2021).</ref>

			</references>

2022年1月21日 (金) 01:59にLwangによる

2022-01-21T01:59:19Z

← 古い版		2022年1月21日 (金) 01:59時点における版
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	<math>\theta_i</math> and <math>\theta_j</math> denote the angles of incidence and transmission of IR light, respectively.		<math>\theta_i</math> and <math>\theta_j</math> denote the angles of incidence and transmission of IR light, respectively.

	The reflectance of <math>p</math>- and <math>s</math>-polarized lights can be represented as the ratio of reflected to incident light intensities by ~~cite{rf:morita2018b}~~		The reflectance of <math>p</math>- and <math>s</math>-polarized lights can be represented as the ratio of reflected to incident light intensities by <ref name = "ref1" />

	: <math> \| r_{ij}^p\|^2 = \left\| \frac{n_j \cos \theta_i - n_i \cos \theta_j}{n_j \cos \theta_i + n_i \cos \theta_j} \right\|^2 </math>		: <math> \| r_{ij}^p\|^2 = \left\| \frac{n_j \cos \theta_i - n_i \cos \theta_j}{n_j \cos \theta_i + n_i \cos \theta_j} \right\|^2 </math>
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	: <math>n_j^0(\lambda) = A + \frac{B}{{\lambda}^2} + \frac{C}{{\lambda}^4}</math>		: <math>n_j^0(\lambda) = A + \frac{B}{{\lambda}^2} + \frac{C}{{\lambda}^4}</math>
	The obtained parameters <math>A, B, C</math> were used to evaluate the nonresnant refractive index at 5000 <math> \text{cm}^{-1} </math>.		The obtained parameters <math>A, B, C</math> were used to evaluate the nonresnant refractive index at 5000 <math> \text{cm}^{-1} </math>.
	It is also possible to directly use the refractive index in the visible region, which may involve some deviation in <math> n_j^0 </math>.		It is also possible to directly use the refractive index in the visible region, which may involve some deviation in <math> n_j^0 </math>. <ref name = "ref2" />

	After the determination of <math> n_j^0 </math>, other parameters related to the Lorentz functions are determined by minimizing the least-squares residual (LSR) between the experimental reflectance spectra and those of the analytical formulas over the whole wavenumber region of the target vibrational band. The residual is defined by		After the determination of <math> n_j^0 </math>, other parameters related to the Lorentz functions are determined by minimizing the least-squares residual (LSR) between the experimental reflectance spectra and those of the analytical formulas over the whole wavenumber region of the target vibrational band. The residual is defined by
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	The minimization is numerically done in the program, thus the initial parameter of <math> l_\text{max} </math>, <math> A_l </math>, <math> \nu_l</math> and <math>\Gamma_l</math> should be determined.		The minimization is numerically done in the program, thus the initial parameter of <math> l_\text{max} </math>, <math> A_l </math>, <math> \nu_l</math> and <math>\Gamma_l</math> should be determined.
	And the initial parameters also have a large effect on whether the minimization can reach the tolerance and how long the minimization procedure is taken.		And the initial parameters also have a large effect on whether the minimization can reach the tolerance and how long the minimization procedure is taken.
	All of them can be set manually ~~according to user's experiences~~.		All of them can be set manually.
	In the following, we will introduce a method to automatically determine the initial parameters.		In the following, we will introduce a method to automatically determine the initial parameters.

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	Thus, the initial parameter for <math> \nu_1 </math> is set to the wavenumber of minimum value of reflectance in the experimental data.		Thus, the initial parameter for <math> \nu_1 </math> is set to the wavenumber of minimum value of reflectance in the experimental data.
	The initial parameter for <math> \Gamma_1 </math> and <math> A_1 </math> is set to be 15 <math> \text{cm}^{-1} </math> and 7.5 <math> \text{cm}^{-1} </math>, respectively.		The initial parameter for <math> \Gamma_1 </math> and <math> A_1 </math> is set to be 15 <math> \text{cm}^{-1} </math> and 7.5 <math> \text{cm}^{-1} </math>, respectively.
	These parameters are estimated from the parameters of very strong adsorption bands of commonly used liquids. ~~cite{wang}~~		These parameters are estimated from the parameters of very strong adsorption bands of commonly used liquids. <ref name = "ref2" />

	After the first fitting procedure, the strongest adsorption band is expected to be well represented.		After the first fitting procedure, the strongest adsorption band is expected to be well represented.
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	The number of Lorentz functions keeps increasing and the whole procedure is repeated until the final LSR reaches the set tolerance.		The number of Lorentz functions keeps increasing and the whole procedure is repeated until the final LSR reaches the set tolerance.

			<references>
			<ref name = "ref1">"Theory of Sum Frequency Generation Spectroscopy"
			Akihiro Morita. Springer Nature Singapore Pte Ltd: 2018 </ref>
			<ref name = "ref2">"Dispersion of Complex Refractive Indices for Intense Vibrational Bands. I Quantitative Spectra"
			Ryo Murata, Ken-ichi Inoue, Lin Wang, Shen Ye, and Akihiro Morita, J. Phys. Chem. B, 125(34), 9794-9803 (2021).</ref>

2022年1月20日 (木) 08:55にLwangによる

2022-01-20T08:55:53Z

← 古い版		2022年1月20日 (木) 08:55時点における版
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	The experimental geometry is described by the two-layer model in the above Figure, where phase <math>i</math> and phase <math>j</math> represent the substrate and sample, respectively.		The experimental geometry is described by the two-layer model in the above Figure, where phase <math>i</math> and phase <math>j</math> represent the substrate and sample, respectively.
	The incident light in phase <math>i</math> and transmitted light in phase <math>j</math> are related by Snell's law		The incident light in phase <math>i</math> and transmitted light in phase <math>j</math> are related by Snell's law
	: <math> n_i \sin \theta_i = n_j \sin \theta_j </math>		: <math> n_i \sin \theta_i = n_j \sin \theta_j </math>

			where <math>n_i</math> and <math>n_j</math> are the complex refractive index of substrate and sample.
			<math>\theta_i</math> and <math>\theta_j</math> denote the angles of incidence and transmission of IR light, respectively.

			The reflectance of <math>p</math>- and <math>s</math>-polarized lights can be represented as the ratio of reflected to incident light intensities by cite{rf:morita2018b}

			: <math> \| r_{ij}^p\|^2 = \left\| \frac{n_j \cos \theta_i - n_i \cos \theta_j}{n_j \cos \theta_i + n_i \cos \theta_j} \right\|^2 </math>
			: <math> \| r_{ij}^s\|^2 = \left\| \frac{n_i \cos \theta_i - n_j \cos \theta_j}{n_i \cos \theta_i + n_j \cos \theta_j} \right\|^2 </math>

			The angle of transmission <math>\theta_j</math> is derived from Snell's law to be
			: <math> \cos \theta_j = \sqrt{1-\frac{n_i^2}{n_j^2} \sin^2 \theta_i} </math>
			which can be imaginary in the ATR condition.

			In the experiment, the incident angle <math>\theta_i</math> is often fixed, for example, to 45 degree.
			Take substate diamond as example, <math>n_i </math> is also known as 2.38.
			Therefore, the ATR condition is satisfied in most cases where <math>n_j </math> is smaller than <math> n_i \sin \theta_i = 1.68 </math>.
			This situation is held for most liquid samples.
			In the total reflection condition, the calculated <math> \| r_{ij}^p\|^2 </math> and <math> \| r_{ij}^s\|^2 </math> are unity when <math>n_j </math> is real.
			However, <math> \| r_{ij}^p\|^2 </math> and <math> \| r_{ij}^s\|^2 </math> become less than unity when the refractive index of the liquid <math>n_j = \eta_j + i \kappa_j </math> is complex.
			The reduced reflectance is a consequence of the absorption of evanescent light in the liquid sample.
			Therefore, by fitting the experimental reflectance data in ATR-IR spectra, it is able to obtain the complex refractive index of the liquid sample.

	----		----

	<div id="Fitting procedure" style="font-size: 200%;"> ~~Fitting procedure\|~~ How to Fit the ATR-IR spectra </div>		<div id="Fitting procedure" style="font-size: 200%;"> How to Fit the ATR-IR spectra </div>

			The purpose of fitting is to determine the frequency-dependent complex refractive index <math>n_j(\nu) </math>.
			The complex refractive index of sample is represented with a set of Lorentz functions
			: <math> n_j (\nu) = \eta_j (\nu) + i \kappa_j (\nu) = n_j^0 + \sum_{l=1}^{l_\text{max}} \frac{A_l}{\nu_l - \nu - i \Gamma_l} </math>
			where <math> n_j^0 </math> is the nonresonant refractive index.
			<math> A_l </math>, <math> \nu_l</math> and <math>\Gamma_l</math> are the amplitude, peak wavenumber and bandwidth of each Lorentz function,
			respectively. <math> l_\text{max} </math> is the number of Lorentz functions to be used.
			Therefore, the parameters <math> n_j^0 </math>, <math> A_l </math>, <math> \nu_l</math> and <math>\Gamma_l</math> and <math> l_\text{max} </math> were determined from the experimental spectra.

			In the beginning, <math> n_j^0 </math> should be determined before the fitting procedure. <math> n_j^0 </math> is the nonresonant refractive index in the IR wavenumber region.
			In the reference paper cite{wang}, we use the refractive index values in the visible regions to fit Cauchy's equation.
			: <math>n_j^0(\lambda) = A + \frac{B}{{\lambda}^2} + \frac{C}{{\lambda}^4}</math>
			The obtained parameters <math>A, B, C</math> were used to evaluate the nonresnant refractive index at 5000 <math> \text{cm}^{-1} </math>.
			It is also possible to directly use the refractive index in the visible region, which may involve some deviation in <math> n_j^0 </math>.

			After the determination of <math> n_j^0 </math>, other parameters related to the Lorentz functions are determined by minimizing the least-squares residual (LSR) between the experimental reflectance spectra and those of the analytical formulas over the whole wavenumber region of the target vibrational band. The residual is defined by
			: <math> \text{LSR} ( \{ A_l, \nu_l, \Gamma_l \} ) = \frac{1}{n} \sum_{\nu_n \in [\nu_\text{min}, \nu_\text{max}]} \left[ \|r_{ij}^p (\nu_n)\|^2 + \|r_{ij}^s (\nu_n)\|^2 - 2\|r_{ij} (\nu_n)\|^2_\mathrm{exp} \right]^2 </math>
			where <math> \| r_{ij}^p\|^2 </math> and <math> \| r_{ij}^s\|^2 </math> are the calculated reflectances in the above section.
			<math> \|r_{ij} (\nu_n)\|^2_\mathrm{exp} </math> is the experimental reflectance of unpolarized light at wavenumber <math> \nu_n </math>. The summation of <math> n </math> is taken for all observed wavenumber points in the target vibrational band.
			By minimizing the LSR, the parameters of each Lorentz functions, <math> A_l </math>, <math> \nu_l</math> and <math>\Gamma_l</math>, were obtained.
			The minimization is numerically done in the program, thus the initial parameter of <math> l_\text{max} </math>, <math> A_l </math>, <math> \nu_l</math> and <math>\Gamma_l</math> should be determined.
			And the initial parameters also have a large effect on whether the minimization can reach the tolerance and how long the minimization procedure is taken.
			All of them can be set manually according to user's experiences.
			In the following, we will introduce a method to automatically determine the initial parameters.

	----		----

	<div id="Auto Fitting" style="font-size: 200%;"> Automatically determine the initial parameters in fitting procedure </div>		<div id="Auto Fitting" style="font-size: 200%;"> Automatically determine the initial parameters in fitting procedure </div>

			In order to determine the number of Lorentz functions to be used, we first start with only one Lorentz function and represent the complex refractive index as
			: <math> n_j (\nu) = n_j^0 + \frac{A_1}{\nu_1 - \nu - i \Gamma_1} </math>
			The first Lorentz function is used to fit the strongest adsorption band in the target region.
			Thus, the initial parameter for <math> \nu_1 </math> is set to the wavenumber of minimum value of reflectance in the experimental data.
			The initial parameter for <math> \Gamma_1 </math> and <math> A_1 </math> is set to be 15 <math> \text{cm}^{-1} </math> and 7.5 <math> \text{cm}^{-1} </math>, respectively.
			These parameters are estimated from the parameters of very strong adsorption bands of commonly used liquids. cite{wang}

			After the first fitting procedure, the strongest adsorption band is expected to be well represented.
			Here if the LSR is less than the tolerance, the fitting is finished and no more Lorentz functions are required.
			If not, another Lorentz function is added and the complex refractive index become
			: <math> n_j (\nu) = n_j^0 + \frac{A_1}{\nu_1 - \nu - i \Gamma_1} + \frac{A_2}{\nu_2 - \nu - i \Gamma_2} </math>
			The second Lorentz funtion is used to represent major adsorption band in the difference reflectance spectra between the first fitting results and experimental results.
			The initial value of <math> \nu_1 </math>, <math> \Gamma_1 </math> and <math> A_1 </math> are set to be the optimized value in the last fitting procedure.
			The initial value of <math> \nu_2 </math> is set to the wavenumber of minimum (or maximum) value of difference reflectance spectra.
			The initial parameter for <math> \Gamma_2 </math> and <math> A_2 </math> is set to be 15 <math> \text{cm}^{-1} </math> and 3.75 <math> \text{cm}^{-1} </math>, respectively.
			A smaller initial value of <math> A_2 </math> suggests that the second Lorentz function is a minor adsorption band in ATR-IR spectra.
			Then all parameters are again optimized using the same fitting procedure.

			The number of Lorentz functions keeps increasing and the whole procedure is repeated until the final LSR reaches the set tolerance.

← 古い版		2022年2月17日 (木) 08:59時点における版
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	: <math>n_j^0(\lambda) = A + \frac{B}{{\lambda}^2} + \frac{C}{{\lambda}^4}</math>		: <math>n_j^0(\lambda) = A + \frac{B}{{\lambda}^2} + \frac{C}{{\lambda}^4}</math>
	The obtained parameters <math>A, B, C</math> were used to evaluate the nonresnant refractive index at 5000 <math> \text{cm}^{-1} </math>.		The obtained parameters <math>A, B, C</math> were used to evaluate the nonresnant refractive index at 5000 <math> \text{cm}^{-1} </math>.
	It is also possible to directly use the refractive index in the visible region, which may involve a ~~slightly~~ deviation in <math> n_j^0 </math>. <ref name = "ref2" />
			It is also possible to directly use the refractive index in the visible region, which may involve a very slight deviation in <math> n_j^0 </math>. <ref name = "ref2" />

	After the determination of <math> n_j^0 </math>, other parameters related to the Lorentz functions are determined by minimizing the least-squares residual (LSR) between the experimental reflectance spectra and those of the analytical formulas over the whole wavenumber region of the target vibrational band. The residual is defined by		After the determination of <math> n_j^0 </math>, other parameters related to the Lorentz functions are determined by minimizing the least-squares residual (LSR) between the experimental reflectance spectra and those of the analytical formulas over the whole wavenumber region of the target vibrational band. The residual is defined by
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	The first Lorentz function is used to fit the strongest adsorption band in the target region.		The first Lorentz function is used to fit the strongest adsorption band in the target region.
	Thus, the initial parameter for <math> \nu_1 </math> is set to the wavenumber of minimum value of reflectance in the experimental data.		Thus, the initial parameter for <math> \nu_1 </math> is set to the wavenumber of minimum value of reflectance in the experimental data.
	The initial parameter for <math> \Gamma_1 </math> and <math> A_1 </math> is set to ~~be 15 <math> \text{cm}^{-1} </math> and 7.5 <math> \text{cm}^{-1} </math>, respectively.~~		The initial parameter for <math> \Gamma_1 </math> and <math> A_1 </math> is set according to the linesharp of strongest adsorption band in ATR-IR spectra.
	~~These parameters are estimated from~~ the ~~parameters~~ of ~~very strong~~ adsorption ~~bands of commonly used liquids~~. ~~<ref name = "ref2" />~~

	After the first fitting procedure, the strongest adsorption band is expected to be well represented.		After the first fitting procedure, the strongest adsorption band is expected to be well represented.
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	The initial value of <math> \nu_1 </math>, <math> \Gamma_1 </math> and <math> A_1 </math> are set to be the optimized value in the last fitting procedure.		The initial value of <math> \nu_1 </math>, <math> \Gamma_1 </math> and <math> A_1 </math> are set to be the optimized value in the last fitting procedure.
	The initial value of <math> \nu_2 </math> is set to the wavenumber of minimum (or maximum) value of difference reflectance spectra.		The initial value of <math> \nu_2 </math> is set to the wavenumber of minimum (or maximum) value of difference reflectance spectra.
	The initial parameter for <math> \Gamma_2 </math> and <math> A_2 </math> is set to be 15 <math> \text{cm}^{-1} </math> and ~~3.75~~ <math> \text{cm}^{-1} </math>, respectively.		The initial parameter for <math> \Gamma_2 </math> and <math> A_2 </math> is set to be 15 <math> \text{cm}^{-1} </math> and <math> A_1/2 \text{cm}^{-1} </math>, respectively.
	A smaller initial value of <math> A_2 </math> suggests that the second Lorentz function is a minor adsorption band in ATR-IR spectra.		A smaller initial value of <math> A_2 </math> suggests that the second Lorentz function is a minor adsorption band in ATR-IR spectra.
	Then all parameters are again optimized using the same fitting procedure.		Then all parameters are again optimized using the same fitting procedure.