CN112595673A - Method for measuring optical constant of single crystal diamond substrate - Google Patents
Method for measuring optical constant of single crystal diamond substrate Download PDFInfo
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- CN112595673A CN112595673A CN202011296318.0A CN202011296318A CN112595673A CN 112595673 A CN112595673 A CN 112595673A CN 202011296318 A CN202011296318 A CN 202011296318A CN 112595673 A CN112595673 A CN 112595673A
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- 230000003287 optical effect Effects 0.000 title claims abstract description 52
- 239000000758 substrate Substances 0.000 title claims abstract description 44
- 229910003460 diamond Inorganic materials 0.000 title claims abstract description 26
- 239000010432 diamond Substances 0.000 title claims abstract description 26
- 239000013078 crystal Substances 0.000 title claims abstract description 19
- 238000000034 method Methods 0.000 title claims abstract description 15
- 238000005259 measurement Methods 0.000 claims abstract description 24
- 238000001228 spectrum Methods 0.000 claims abstract description 17
- 238000000572 ellipsometry Methods 0.000 claims abstract description 15
- 230000005540 biological transmission Effects 0.000 claims abstract description 12
- 238000000411 transmission spectrum Methods 0.000 claims abstract description 10
- 230000008033 biological extinction Effects 0.000 claims abstract description 7
- 230000003595 spectral effect Effects 0.000 claims abstract description 7
- 230000010287 polarization Effects 0.000 claims description 9
- 238000004364 calculation method Methods 0.000 claims description 7
- 238000000691 measurement method Methods 0.000 claims description 7
- 239000000463 material Substances 0.000 claims description 4
- 238000012821 model calculation Methods 0.000 claims 1
- 239000010408 film Substances 0.000 description 8
- 239000012788 optical film Substances 0.000 description 5
- 239000011159 matrix material Substances 0.000 description 3
- 238000005516 engineering process Methods 0.000 description 2
- 238000011156 evaluation Methods 0.000 description 2
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 1
- 238000010521 absorption reaction Methods 0.000 description 1
- 238000000862 absorption spectrum Methods 0.000 description 1
- 238000004458 analytical method Methods 0.000 description 1
- 239000002131 composite material Substances 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 238000013461 design Methods 0.000 description 1
- 238000000985 reflectance spectrum Methods 0.000 description 1
- 229910052710 silicon Inorganic materials 0.000 description 1
- 239000010703 silicon Substances 0.000 description 1
- 238000012360 testing method Methods 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
Classifications
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/21—Polarisation-affecting properties
- G01N21/211—Ellipsometry
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/21—Polarisation-affecting properties
- G01N21/211—Ellipsometry
- G01N2021/213—Spectrometric ellipsometry
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- Physics & Mathematics (AREA)
- Biochemistry (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Length Measuring Devices By Optical Means (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Abstract
The invention discloses a method for measuring optical constants of a monocrystalline diamond substrate, which comprises the following steps: respectively measuring the single crystal diamond substrate by adopting a transmission type ellipsometry measurement mode and a reflection type ellipsometry measurement mode; the transmission spectra (ψ) were obtained by the above measurements, respectivelyt、Δt) And reflection spectrum (psi)r、Δr) (ii) a Obtaining spectral data according to the measurement, and respectively calculating by adopting a Cauchy model to obtain substrate optical constants at least comprising a substrate refractive index n and an extinction coefficient k; evaluating the fitting error sigma, and optimizing the optical model or the dielectric function when the fitting error exceeds a preset condition; and comparing the fitting errors of the optimized models, and selecting a model and a measurement mode to determine the optical constant of the diamond substrate. It has the following advantages: the optical constant measurement is more accurate.
Description
Technical Field
The invention relates to the technical field of optical constant measurement, in particular to a method for measuring an optical constant of a monocrystalline diamond substrate.
Background
The existing method for testing the ultra-wideband optical constant of the optical film, such as CN106706521A, includes: s1, firstly, depositing an optical film with a preset thickness on a silicon substrate; s2, measuring the ultraviolet to near infrared band elliptical polarization spectrum and infrared band transmission spectrum of the deposited optical film; s3, selecting a transparent area of a section of film according to the spectral data of the optical film, and calculating by adopting a Cauchy model to obtain the refractive index n and the thickness d1 of the film within the waveband range; s4, establishing an optical constant model with an optical constant ranging from ultraviolet to infrared wide spectrum, adding a dielectric constant vibrator model in an absorption spectrum area, wherein the center frequency of a vibrator is the absorption position, and the amplitude and the width of the vibrator are adjusted according to spectrum data; s5, taking an ultraviolet to near-infrared waveband elliptical polarization spectrum and an infrared waveband transmission spectrum as a composite target, performing inversion operation on the optical constant of the film in an ultraviolet to infrared full spectrum range, wherein the initial value of the thickness is set as d1, an evaluation function MSE is preset, the MSE is the mean square error of a measured value and a theoretical model calculated value, and fitting the MSE to make the MSE smaller and better; and S6, obtaining each parameter of the dielectric constant model according to the MSE fitting result, and further obtaining the optical constant of the film in the ultraviolet-infrared ultra-wideband spectrum range, wherein the optical constant comprises the refractive index n, the extinction coefficient k and the physical thickness d of the film. The measurement method only obtains the result according to the measurement of the elliptical polarization measurement mode, so the accuracy of obtaining the constant is to be enhanced.
Disclosure of Invention
The invention provides a method for measuring an optical constant of a monocrystalline diamond substrate, which overcomes the defects of an optical film ultra-wideband optical constant measuring method in the background technology.
In order to solve the technical problem, the invention provides a method for measuring optical constants of a single crystal diamond substrate, which comprises the following steps:
s1, respectively measuring the single crystal diamond substrate by adopting a transmission type ellipsometry measuring method and a reflection type ellipsometry measuring method;
s2, respectively obtained by the above measurementTransmission spectrum (psi, delta)t) And reflection spectrum (psi)r、Δr) Phi represents the amplitude ratio of the emergent light to the incident light, delta represents the phase difference between the emergent light and the incident light, the lower corner mark t represents the transmission ellipsometry, and the lower corner mark r represents the reflection ellipsometry;
s3, obtaining spectral data according to the measurement, and respectively calculating by adopting a Cauchy model to obtain substrate optical constants, wherein the optical constants at least comprise a substrate refractive index n and an extinction coefficient k;
s4, evaluating the fitting error sigma, and optimizing the optical model or the dielectric function when the fitting error exceeds a preset condition;
s5, comparing the fitting error of the optimized model, selecting a model and a measuring mode to determine the optical constant of the diamond substrate.
In one embodiment: in this step S2, the transmission spectrum (ψ)t、Δt) Is defined as:
t represents the polarization amplitude transmission coefficient, r represents the polarization amplitude reflection coefficient, and the lower indices p and s represent p-polarized light and s-polarized light, respectively, resolved from a natural light beam.
In one embodiment: in step S3, the calculation formula of the Cauchy model is:
wherein n is the refractive index, An、BnAnd CnIs Cauchy model parameter, lambda is wavelength, extinction coefficient k is from Ak、BkAnd EbDescription of three parameters, Eb=1240/λb,EbAssociated with the substrate material. .
In one embodiment: in step S4, the fitting error σ is calculated by the following formula:
ρ ═ tan Φ exp (i Δ), M is the number of measurement points, P is the number of parameters, the lower subscript ex indicates experimental data, and the lower subscript cal indicates calculated data of the fit.
In one embodiment: in step S3, obtaining spectral data according to the above measurements, and calculating with a Cauchy model to obtain optical constants of the substrate in the wavelength range, wherein the optical constants further include the thickness d of the substratet、 dr。
In one embodiment: the wave band range is 210 nm-1650 nm.
In one embodiment: in step S4, the optimized optical model includes a multilayer structure.
In one embodiment: the multilayer structure includes a roughness layer calculated using Bruggeman Effective Medium Approximation (EMA) theory.
Compared with the background technology, the technical scheme has the following advantages:
1. through two measurement modes of a transmission type and a reflection type of an ellipsometer, the single crystal diamond substrate is respectively measured to obtain a transmission spectrum and a reflection spectrum, then calculation is carried out according to an optical model established by combining the transmission spectrum and the reflection spectrum, fitting analysis is carried out to obtain a final optical constant of the single crystal diamond substrate, more information can be extracted, and the obtained optical constant is more accurate.
Detailed Description
In order to further explain the objects, technical solutions and features of the present invention, a method for measuring optical constants of a single crystal diamond substrate is described in detail with reference to specific embodiments.
A method for measuring optical constants of a single crystal diamond substrate, comprising:
s1, respectively measuring the single crystal diamond substrate by adopting a transmission type ellipsometry measuring mode and a reflection type ellipsometry measuring mode, wherein the measuring mode can adopt an ellipsometer for measuring, and the ellipsometer is an optical measuring instrument for detecting the thickness, the optical constant and the material microstructure of the thin film;
s2, obtaining transmission spectra (psi) by the above measurementt、Δt) And reflection spectrum (psi)r、Δr) Phi represents the amplitude ratio of the emergent light to the incident light, delta represents the phase difference between the emergent light and the incident light, the lower corner mark t represents the transmission ellipsometry, and the lower corner mark r represents the reflection ellipsometry; wherein:
transmission spectrum (psi)t、Δt) Is defined as:
the reflection spectrum (ψ r, Δ r) is defined as:
in equations (1) and (2): t represents a polarization amplitude transmission coefficient, r represents a polarization amplitude reflection coefficient, and lower corner marks p and s respectively represent p-polarized light and s-polarized light decomposed by a beam of natural light;
s3, obtaining spectrum data according to the above measurement, and calculating respectively by Cauchy model (Cauchy model) to obtain substrate optical constants including at least substrate refractive index nt、nr;
The Cauchy model has the calculation formula as follows:
in equation (3): n is the refractive index, An、BnAnd CnIs Cauchy model parameter, lambda is wavelength,
in equation (4): extinction coefficient k is represented by Ak、BkAnd EbDescription of three parameters, Eb=1240/λbAssociated with the substrate material;
s4, evaluating the fitting error sigma, and optimizing the optical model or the dielectric function when the fitting error exceeds a preset condition;
the fitting error σ is calculated as:
in equation (5): ρ ═ tan ψ exp (i Δ), M is the number of measurement points, P is the number of parameters (one point is measured multiple times, the number of measurements corresponds to the number of P), the lower subscript ex represents experimental data, and the lower subscript cal represents fitting calculation data; wherein: in ellipsometry, corresponding parameters are characterized and analyzed by means of a matrix, the number of measurements is related to the number of matrix elements, for example, if the mueller matrix is 4 x 4, at least 16 measurements are performed to solve the parameters;
s5, comparing the fitting error of the optimized model, selecting a model and a measuring mode to determine the optical constant of the diamond substrate.
Optionally, in step S4, the optimized optical model comprises a multilayer structure including a roughness layer calculated using Bruggeman' S Effective Medium Approximation (EMA) theory.
In this embodiment: whether the error exceeds a predetermined condition such as: judging the goodness of fit of the fitting curve and the measuring curve, wherein if the goodness of fit is large, the error is large, and if the goodness of fit is small, the error is small; or, calculating an evaluation index MSE value, and then judging whether the MSE value is larger than a preset value, wherein if the MSE value is larger than the preset value, the error is large, and if the MSE value is smaller than the preset value, the error is small.
According to the requirement, in step S3, spectral data are obtained according to the above measurement, and the optical constants of the substrate in the waveband range are obtained by respectively calculating with a Cauchy model, and if the substrate surface has other film layers, the thickness d of the surface film layer can be obtained by fitting. The wave band ranges from 210nm to 1650nm, and the thickness d of the film layer is used as a variable parameter to be fitted with A, B, C of a Cauchy model.
The above description is only a preferred embodiment of the present invention, but the design concept of the present invention is not limited thereto, and any person skilled in the art can make insubstantial changes in the technical scope of the present invention within the technical scope of the present invention, and the actions infringe the protection scope of the present invention are included in the present invention.
Claims (8)
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Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN113267454A (en) * | 2021-05-26 | 2021-08-17 | 中国工程物理研究院激光聚变研究中心 | Thin film quality detection method, thin film quality detection device, electronic device, and storage medium |
| CN113654995A (en) * | 2021-07-08 | 2021-11-16 | 南京大学 | A method for measuring ellipsometry spectrum under package condition |
| CN114324184A (en) * | 2021-12-30 | 2022-04-12 | 广州粤芯半导体技术有限公司 | Spectroscopic floating model of ellipsometer and establishing method |
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| CN102680410A (en) * | 2012-05-03 | 2012-09-19 | 中国科学院宁波材料技术与工程研究所 | Method for non-destructively, quickly and accurately characterizing bonding structure of tetrahedral amorphous carbon film |
| CN103743349A (en) * | 2013-12-30 | 2014-04-23 | 中国科学技术大学 | Method and device for measuring nano film |
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2020
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| CN113267454A (en) * | 2021-05-26 | 2021-08-17 | 中国工程物理研究院激光聚变研究中心 | Thin film quality detection method, thin film quality detection device, electronic device, and storage medium |
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