CN112729543A - Background correction method, equipment and medium for narrow-band absorption in optical detection - Google Patents
Background correction method, equipment and medium for narrow-band absorption in optical detection Download PDFInfo
- Publication number
- CN112729543A CN112729543A CN202011501092.3A CN202011501092A CN112729543A CN 112729543 A CN112729543 A CN 112729543A CN 202011501092 A CN202011501092 A CN 202011501092A CN 112729543 A CN112729543 A CN 112729543A
- Authority
- CN
- China
- Prior art keywords
- background correction
- optical detection
- detection system
- background
- light source
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 238000003705 background correction Methods 0.000 title claims abstract description 63
- 238000001514 detection method Methods 0.000 title claims abstract description 60
- 238000000034 method Methods 0.000 title claims abstract description 38
- 230000003287 optical effect Effects 0.000 title claims abstract description 35
- 238000010521 absorption reaction Methods 0.000 title claims abstract description 22
- 238000012937 correction Methods 0.000 claims abstract description 10
- 238000012795 verification Methods 0.000 claims abstract description 5
- 238000002834 transmittance Methods 0.000 claims description 12
- 238000002835 absorbance Methods 0.000 claims description 8
- 239000002131 composite material Substances 0.000 claims description 5
- 238000002474 experimental method Methods 0.000 claims description 5
- 238000004847 absorption spectroscopy Methods 0.000 claims description 4
- 230000001154 acute effect Effects 0.000 claims description 4
- 238000012545 processing Methods 0.000 claims 1
- 239000007789 gas Substances 0.000 description 13
- 230000003595 spectral effect Effects 0.000 description 5
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 4
- MWUXSHHQAYIFBG-UHFFFAOYSA-N Nitric oxide Chemical compound O=[N] MWUXSHHQAYIFBG-UHFFFAOYSA-N 0.000 description 4
- 239000000523 sample Substances 0.000 description 4
- JVMRPSJZNHXORP-UHFFFAOYSA-N ON=O.ON=O.ON=O.N Chemical compound ON=O.ON=O.ON=O.N JVMRPSJZNHXORP-UHFFFAOYSA-N 0.000 description 3
- MMDJDBSEMBIJBB-UHFFFAOYSA-N [O-][N+]([O-])=O.[O-][N+]([O-])=O.[O-][N+]([O-])=O.[NH6+3] Chemical compound [O-][N+]([O-])=O.[O-][N+]([O-])=O.[O-][N+]([O-])=O.[NH6+3] MMDJDBSEMBIJBB-UHFFFAOYSA-N 0.000 description 3
- 235000013405 beer Nutrition 0.000 description 3
- 239000000126 substance Substances 0.000 description 3
- 238000012360 testing method Methods 0.000 description 3
- XKMRRTOUMJRJIA-UHFFFAOYSA-N ammonia nh3 Chemical compound N.N XKMRRTOUMJRJIA-UHFFFAOYSA-N 0.000 description 2
- 238000004458 analytical method Methods 0.000 description 2
- 238000000559 atomic spectroscopy Methods 0.000 description 2
- 238000013461 design Methods 0.000 description 2
- 230000008030 elimination Effects 0.000 description 2
- 238000003379 elimination reaction Methods 0.000 description 2
- 239000012535 impurity Substances 0.000 description 2
- 230000031700 light absorption Effects 0.000 description 2
- 238000012417 linear regression Methods 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 229910052757 nitrogen Inorganic materials 0.000 description 2
- 238000003672 processing method Methods 0.000 description 2
- MGWGWNFMUOTEHG-UHFFFAOYSA-N 4-(3,5-dimethylphenyl)-1,3-thiazol-2-amine Chemical compound CC1=CC(C)=CC(C=2N=C(N)SC=2)=C1 MGWGWNFMUOTEHG-UHFFFAOYSA-N 0.000 description 1
- YZCKVEUIGOORGS-OUBTZVSYSA-N Deuterium Chemical compound [2H] YZCKVEUIGOORGS-OUBTZVSYSA-N 0.000 description 1
- RWSOTUBLDIXVET-UHFFFAOYSA-N Dihydrogen sulfide Chemical compound S RWSOTUBLDIXVET-UHFFFAOYSA-N 0.000 description 1
- UCKMPCXJQFINFW-UHFFFAOYSA-N Sulphide Chemical compound [S-2] UCKMPCXJQFINFW-UHFFFAOYSA-N 0.000 description 1
- 230000009286 beneficial effect Effects 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 229910052805 deuterium Inorganic materials 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000006870 function Effects 0.000 description 1
- 229910000037 hydrogen sulfide Inorganic materials 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000010905 molecular spectroscopy Methods 0.000 description 1
- JCXJVPUVTGWSNB-UHFFFAOYSA-N nitrogen dioxide Inorganic materials O=[N]=O JCXJVPUVTGWSNB-UHFFFAOYSA-N 0.000 description 1
- 238000004451 qualitative analysis Methods 0.000 description 1
- 239000013062 quality control Sample Substances 0.000 description 1
- 238000004611 spectroscopical analysis Methods 0.000 description 1
- 238000001228 spectrum Methods 0.000 description 1
- 150000003568 thioethers Chemical class 0.000 description 1
Images
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
- G01J3/02—Details
- G01J3/10—Arrangements of light sources specially adapted for spectrometry or colorimetry
Landscapes
- Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- General Physics & Mathematics (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Abstract
The invention relates to a background correction method, equipment and medium for narrow-band absorption in optical detection, wherein the background correction method is used for carrying out error correction on an optical detection system and comprises the following steps: acquiring original detection data of an optical detection system of the optical detection system; performing background correction on the original detection data based on a background correction coefficient obtained in advance; wherein the background correction coefficient is obtained by: and acquiring a group of detection data of the optical detection system, and acquiring the optimal background correction coefficient in a reverse deduction and verification mode. Compared with the prior art, the method has the advantages of effectively reducing errors, improving the precision, needing no hardware change and the like.
Description
Technical Field
The present invention relates to a photoelectric detection system, and more particularly, to a method, an apparatus, and a medium for background correction of narrow-band absorption in optical detection.
Background
Photoelectric detection systems such as molecular absorption spectrometers and atomic absorption spectrometers are important instruments in spectroscopy. The gas phase molecular absorption spectrometer carries out quantitative determination based on the principle that the relation between the absorption intensity of gas decomposed into measured components to light and the concentration of the measured components complies with the light absorption law; depending on the absorption wavelength, the component to be measured can be identified and qualitative analysis can be performed. The gas phase molecular absorption spectrometer can comprise a light source, a collimating and focusing lens group, an absorption cell, a monochromator and a photoelectric detection device, and system errors are caused by factors such as background interference in the detection process. How to reduce background interference and improve the detection accuracy of a photoelectric detection system is a technical problem to be solved urgently in the field.
Disclosure of Invention
The present invention is directed to overcome the above-mentioned drawbacks of the prior art and provide a background correction method, apparatus and medium for effectively reducing background interference and improving narrow-band absorption in optical detection.
The purpose of the invention can be realized by the following technical scheme:
a background correction method for narrow-band absorption in optical detection, for background error correction of an optical detection system, the method comprising the steps of:
acquiring original detection data of an optical detection system of the optical detection system;
performing background correction on the original detection data based on a background correction coefficient obtained in advance;
wherein the background correction coefficient is obtained by: and acquiring a group of detection data of the optical detection system, and acquiring the optimal background correction coefficient in a reverse deduction and verification mode.
Further, the background correction factor is used for characterizing the background stray light of the optical detection system.
Further, the optical detection system is a spectral detection system and device based on the lambert-beer law, and comprises a molecular absorption spectrometer or an atomic absorption spectrometer and the like.
Further, the light source of the optical detection system is a continuous light source or an acute line light source containing background interference.
Further, when the light source is a continuous light source, the background correction coefficient is the ratio of the composite light intensity to the incident light intensity.
Further, the data for background correction includes transmittance, and the relationship between the corrected transmittance and the original transmittance is:
wherein T' is the corrected transmittance, T is the original transmittance, and C is the background correction coefficient.
Further, the value range of the background correction coefficient is 0-1.
The invention also provides a sample concentration gradient experimental data processing method of the gas phase molecular absorption spectrometry, which is characterized in that the experimental data is subjected to background correction by adopting the background correction method, and fitting curves of different concentrations and absorbances are obtained according to the corrected data.
The present invention also provides an electronic device comprising: one or more processors; a memory; and one or more programs stored in the memory, the one or more programs including instructions for performing the background correction method as described above.
The present invention also provides a computer readable storage medium comprising one or more programs for execution by one or more processors of an electronic device, the one or more programs including instructions for performing the background correction method as described above.
Compared with the prior art, the invention has the following beneficial effects:
1. the invention can effectively carry out background correction on the detection data according to the correction carried out by the optical absorption characteristic theory, reduce background errors and improve the linear range and the test precision.
2. The background correction coefficient is obtained when each optical detection system is individually factory-set, the pertinence is strong, the reliability is high, the coefficient is a fixed coefficient, the real-time correction of the test result through software is facilitated, and the user experience is improved.
3. The curve quality is improved after the correction of the invention, the concentration test of the sample to be detected and the quality control sample is also corrected according to the background correction coefficient, the good linear relation is satisfied, and the result accuracy completely meets the requirement.
4. The correction method can reduce the dependence of the hardware structure on the light splitting system to the maximum extent by using users and equipment manufacturers, and reduce the technical difficulty and cost of hardware design and production.
5. The method has wide applicability, can be applied to the measurement background correction of the narrow-band absorption sample in the molecular spectrum to ensure that the result is more accurate, can also be applied to the atomic spectroscopy, and is convenient to be applied to the background correction of a continuous light source and the interference elimination of adjacent spectral lines generated by impurity elements in an acute line light source.
Drawings
FIG. 1 is a schematic flow diagram of the present invention;
FIG. 2 is a graph of a curve fit before background correction in an example;
FIG. 3 is a graph of a curve fit after background correction in an example.
Detailed Description
The invention is described in detail below with reference to the figures and specific embodiments. The present embodiment is implemented on the premise of the technical solution of the present invention, and a detailed implementation manner and a specific operation process are given, but the scope of the present invention is not limited to the following embodiments.
Example 1
The embodiment provides a background correction method of narrow-band absorption in optical detection, which is used for performing error correction on an optical detection system, and the method comprises the following steps: acquiring original detection data of an optical detection system of the optical detection system; and performing background correction on the original detection data based on a background correction coefficient obtained in advance. The background correction coefficient is obtained by: and acquiring a group of detection data of the optical detection system, and acquiring the optimal background correction coefficient in a reverse deduction and verification mode. The background correction factor is used to characterize background stray light of the optical detection system. The different instruments may have differences in the light splitting system in mass production, and the coefficient may be slightly different because each instrument needs to be set up one by one.
The method is suitable for molecular spectroscopy or atomic spectroscopy, and is conveniently applied to background correction of a continuous light source and adjacent spectral line interference elimination generated by impurity elements in an acute line light source. This example is illustrated by a gas phase molecular absorption spectrometer with a continuous light source as an optical detection system, and the components used are a deuterium lamp (kohamamatsu type L6309-50), a collimating and focusing lens set, a long-range absorption cell, a C-T type monochromator (spectral bandwidth 2nm, spectroscopic system), and a photomultiplier (kohamamatsu type R928).
Gas phase molecular absorption spectroscopy measures mainly 5 items, including: nitrite nitrogen, ammonia nitrogen, nitrate nitrogen, total nitrogen, and sulfides. The ammonia nitrogen is chemically oxidized and then converted into nitrite nitrogen, the total nitrogen is chemically digested at high temperature and then converted into nitrate nitrogen, the nitrite nitrogen chemically reacts to generate nitrogen dioxide of the gas to be detected, the nitrate nitrogen chemically reacts to generate nitric oxide of the gas to be detected, and the sulfide chemically reacts to generate hydrogen sulfide of the gas to be detected. Aiming at the three detection gases, the photoelectric detection system is adopted for detection, samples to be detected with different contents are used for reaction to generate the detection gases with different concentrations, a concentration gradient experiment is carried out, and unitary linear regression straight line fitting is carried out on the experiment result. The linear regression of nitric oxide gas without correction for a single element fit is poor (γ <0.999) with large errors, as shown in table 1 and fig. 2.
TABLE 1 items of data before background correction
| | Absorbance | 1/ | T | ||
| 1 | 0.0281 | 1.066842 | 0.937346 | ||
| 2 | 0.06 | 1.148154 | 0.870964 | ||
| 3 | 0.0916 | 1.23481 | 0.809841 | ||
| 4 | 0.1189 | 1.314922 | 0.760501 | ||
| 5 | 0.1441 | 1.393478 | 0.717629 |
The inventor conducts extensive analysis, creatively finds that the error is caused by strong background stray light existing in the spectroscopic system due to the fact that the absorption band of the measured substance is smaller than the spectral bandwidth of the spectroscopic system when the spectroscopic system measures the substance, and designs a method for carrying out background correction on the detection data based on the creatively found result.
Consider lambert beer's law:
A＝lg(1/T)
T＝I/I0
where A is absorbance and T is transmittance (transmittance).
The Lambert beer's law is defined under the condition that the relation between the absorbance and the concentration of a substance is on the premise that incident light is monochromatic light, and light emitted by a continuous light source after passing through a light splitting system is composite light which has composite light intensity. The part of light is present in I0In the method, the light passes through the light absorption cell without being absorbed and becomes a part of I, and the part of light is used as a system error, so that the whole light splitting detection system has stronger background stray light.
Therefore, consider that0And the composite intensity I in IxDeduction, T' thus obtained and Abs calculated from T(NEW)The real absorbance value really accords with the lambert beer law, and the process is a background correction technology:
wherein: 0< C <1
Abs(NEW)＝lg(1/T′)
Background subtraction can be achieved by the above background correction.
The optimal background correction coefficient is obtained through a reverse deduction and verification mode, specifically, a background correction coefficient is initialized through an enumeration method based on a dichotomy thought, and whether the current background correction coefficient is adjusted or not is judged based on the relation between a corrected fitting curve and a fitted curve before correction until the optimal background correction coefficient is obtained.
Fig. 2 and fig. 3 show the corrected data and the fitting curve, where in this embodiment, C is 0.44. As can be seen from the implementation results, the problem of the deterioration of the correlation coefficient (curve curvature, narrowing of the linear range) caused by correcting the stray light is effectively solved.
Table 2 background corrected data items
| Concentration c | T-C | (1-C)/(T-C) | Absorbance (new) |
| 1 | 0.937346 | 1.066841742 | 0.0281 |
| 2 | 0.870964 | 1.148153621 | 0.06 |
| 3 | 0.809841 | 1.234809608 | 0.0916 |
| 4 | 0.760501 | 1.314922025 | 0.1189 |
| 5 | 0.717629 | 1.393477626 | 0.1441 |
The above functions, if implemented in the form of software functional units and sold or used as a separate product, may be stored in a computer-readable storage medium. Based on such understanding, the technical solution of the present invention may be embodied in the form of a software product, which is stored in a storage medium and includes instructions for causing a computer device (which may be a personal computer, a server, or a network device) to execute all or part of the steps of the method according to the embodiments of the present invention. And the aforementioned storage medium includes: a U-disk, a removable hard disk, a Read-Only Memory (ROM), a Random Access Memory (RAM), a magnetic disk or an optical disk, and other various media capable of storing program codes.
Example 2
The embodiment provides a sample concentration gradient experimental data processing method for gas phase molecular absorption spectrometry, which is implemented by performing background correction on experimental data by using the background correction method described in embodiment 1, and obtaining fitted curves of different concentrations and absorbances according to the corrected data.
Example 3
The present embodiments provide an electronic device comprising one or more processors, memory, and one or more programs stored in the memory, the one or more programs including instructions for performing the background correction method as described above.
The foregoing detailed description of the preferred embodiments of the invention has been presented. It should be understood that numerous modifications and variations could be devised by those skilled in the art in light of the present teachings without departing from the inventive concepts. Therefore, the technical solutions available to those skilled in the art through logic analysis, reasoning and limited experiments based on the prior art according to the concept of the present invention should be within the scope of protection defined by the claims.
Claims (10)
1. A background correction method for narrow-band absorption in optical detection, for background error correction of an optical detection system, the method comprising the steps of:
acquiring original detection data of an optical detection system of the optical detection system;
performing background correction on the original detection data based on a background correction coefficient obtained in advance;
wherein the background correction coefficient is obtained by: and acquiring a group of detection data of the optical detection system, and acquiring the optimal background correction coefficient in a reverse deduction and verification mode.
2. The method of claim 1, wherein the background correction factor is used to characterize background stray light of the optical detection system.
3. The method of claim 1, wherein the optical detection system is a spectroscopic detection system and apparatus based on the lambert-beer law.
4. The method of claim 1, wherein the light source of the optical detection system is a continuous light source or an acute line light source with background interference.
5. The method of claim 4, wherein the background correction factor is a ratio of a composite intensity to an incident intensity when the light source is a continuous light source.
6. A method as claimed in claim 1, wherein the data for background correction comprises transmittance, and the relationship between the corrected transmittance and the original transmittance is:
wherein T' is the corrected transmittance, T is the original transmittance, and C is the background correction coefficient.
7. The method of claim 1, wherein the background correction factor is in a range of 0 to 1.
8. A method for processing sample concentration gradient experiment data of gas phase molecular absorption spectrometry, which is characterized in that the background correction method of any one of claims 1 to 7 is adopted to carry out background correction on the experiment data, and fitting curves of different concentrations and absorbances are obtained according to the corrected data.
9. An electronic device, comprising: one or more processors; a memory; and one or more programs stored in the memory, the one or more programs including instructions for performing the background correction method of any of claims 1-7.
10. A computer-readable storage medium comprising one or more programs for execution by one or more processors of an electronic device, the one or more programs including instructions for performing the background correction method of any of claims 1-7.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202011501092.3A CN112729543B (en) | 2020-12-18 | 2020-12-18 | Background correction method, equipment and medium for narrow-band absorption in optical detection |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202011501092.3A CN112729543B (en) | 2020-12-18 | 2020-12-18 | Background correction method, equipment and medium for narrow-band absorption in optical detection |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CN112729543A true CN112729543A (en) | 2021-04-30 |
| CN112729543B CN112729543B (en) | 2023-01-03 |
Family
ID=75603284
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN202011501092.3A Active CN112729543B (en) | 2020-12-18 | 2020-12-18 | Background correction method, equipment and medium for narrow-band absorption in optical detection |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN112729543B (en) |
Citations (11)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CA1213446A (en) * | 1981-02-23 | 1986-11-04 | Walter Bohler | Atomic absorption spectrophotometer providing simply derived background absorbance measurement |
| CN87106256A (en) * | 1986-08-13 | 1988-03-23 | 生命扫描有限公司 | The minimum operation steps system of determination and analysis thing |
| US5818048A (en) * | 1992-07-15 | 1998-10-06 | Optix Lp | Rapid non-invasive optical analysis using broad bandpass spectral processing |
| US5910838A (en) * | 1996-04-19 | 1999-06-08 | Bodenseewerk Perkin-Elmer Gmbh | Method of determining concentrations by means of continuous-spectrum atomic absorption spectroscopy |
| CN101408503A (en) * | 2007-10-11 | 2009-04-15 | 上海光谱仪器有限公司 | Method for automatically detecting and dynamically substracting stray light of spectrometer and spectrometer |
| CN102721654A (en) * | 2011-11-16 | 2012-10-10 | 深圳市世纪天源环保技术有限公司 | Background absorption correction method for CODcr measurement |
| WO2013133008A1 (en) * | 2012-03-08 | 2013-09-12 | 株式会社日立ハイテクノロジーズ | Spectrophotometer and absorption photometry method |
| CN104316480A (en) * | 2014-11-06 | 2015-01-28 | 中国科学院合肥物质科学研究院 | Laser in-situ detection system for oxygen concentration in arsenic-bearing gold concentrate roasting furnace |
| CN104422684A (en) * | 2013-08-28 | 2015-03-18 | 赛默电子制造有限公司 | Background correction in emission spectra |
| US20160054275A1 (en) * | 2013-03-26 | 2016-02-25 | Waters Technologies Corporation | Method for extending the dynamic range of absorbance detectors |
| CN206300893U (en) * | 2016-11-29 | 2017-07-04 | 上海安杰环保科技股份有限公司 | A kind of multiple light courcess gas phase adsorption spectrometer |
-
2020
- 2020-12-18 CN CN202011501092.3A patent/CN112729543B/en active Active
Patent Citations (11)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CA1213446A (en) * | 1981-02-23 | 1986-11-04 | Walter Bohler | Atomic absorption spectrophotometer providing simply derived background absorbance measurement |
| CN87106256A (en) * | 1986-08-13 | 1988-03-23 | 生命扫描有限公司 | The minimum operation steps system of determination and analysis thing |
| US5818048A (en) * | 1992-07-15 | 1998-10-06 | Optix Lp | Rapid non-invasive optical analysis using broad bandpass spectral processing |
| US5910838A (en) * | 1996-04-19 | 1999-06-08 | Bodenseewerk Perkin-Elmer Gmbh | Method of determining concentrations by means of continuous-spectrum atomic absorption spectroscopy |
| CN101408503A (en) * | 2007-10-11 | 2009-04-15 | 上海光谱仪器有限公司 | Method for automatically detecting and dynamically substracting stray light of spectrometer and spectrometer |
| CN102721654A (en) * | 2011-11-16 | 2012-10-10 | 深圳市世纪天源环保技术有限公司 | Background absorption correction method for CODcr measurement |
| WO2013133008A1 (en) * | 2012-03-08 | 2013-09-12 | 株式会社日立ハイテクノロジーズ | Spectrophotometer and absorption photometry method |
| US20160054275A1 (en) * | 2013-03-26 | 2016-02-25 | Waters Technologies Corporation | Method for extending the dynamic range of absorbance detectors |
| CN104422684A (en) * | 2013-08-28 | 2015-03-18 | 赛默电子制造有限公司 | Background correction in emission spectra |
| CN104316480A (en) * | 2014-11-06 | 2015-01-28 | 中国科学院合肥物质科学研究院 | Laser in-situ detection system for oxygen concentration in arsenic-bearing gold concentrate roasting furnace |
| CN206300893U (en) * | 2016-11-29 | 2017-07-04 | 上海安杰环保科技股份有限公司 | A kind of multiple light courcess gas phase adsorption spectrometer |
Also Published As
| Publication number | Publication date |
|---|---|
| CN112729543B (en) | 2023-01-03 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN109799203B (en) | Wide-range high-precision spectrum detection method for COD concentration in water body | |
| Vogel et al. | Evaluation of a cavity ring-down spectrometer for in situ observations of 13 CO 2 | |
| Fan et al. | Direct calibration transfer to principal components via canonical correlation analysis | |
| EP3428620B1 (en) | Gas analysis apparatus, program for gas analysis apparatus, and gas analysis method | |
| US20170191929A1 (en) | Spectral modeling for complex absorption spectrum interpretation | |
| US6894297B1 (en) | Multi-component gas analyzing method using FTIR | |
| GB2561879A (en) | Spectroscopic analysis | |
| Millar et al. | Organic contamination detection for isotopic analysis of water by laser spectroscopy | |
| Geiger et al. | Trace analysis of specialty and electronic gases | |
| CN112729543B (en) | Background correction method, equipment and medium for narrow-band absorption in optical detection | |
| Mansouri et al. | Methane detection to 1 ppm using machine learning analysis of atmospheric pressure plasma optical emission spectra | |
| Debus et al. | Long-term strategy for assessing carbonaceous particulate matter concentrations from multiple fourier transform infrared (FT-IR) instruments: influence of spectral dissimilarities on multivariate calibration performance | |
| Leone et al. | The importance of a correct abundance assumption in determining the effective temperature and gravity of stars. A spectroscopic study of the helium weak stars HD 5737, HD 175362 and HD 202671. | |
| JP5424636B2 (en) | Gas analyzer using FTIR method and program used therefor | |
| Thompson et al. | An interactive spectral analysis tool for chemical identification and quantification of gas-phase species in complex spectra | |
| Fabian et al. | N2, O2, and air broadening of NH3 in ν2 band measured by FTIR spectroscopy | |
| JP2023033398A (en) | Component identification device for spectrum analysis device, method therefor and computer program | |
| US11360020B2 (en) | Gas analysis device, program for gas analysis device, and gas analysis method | |
| CN114660008A (en) | Method for correcting flame atomic absorption method interference | |
| Bradshaw | Influence of spectral interferences on the reliability of data when using analyte addition techniques with ICP-OES | |
| CN110398488B (en) | Nonlinear quantitative analysis method applied to laser-induced breakdown spectroscopy | |
| CN111912805B (en) | Ultraviolet spectrum detection method and device for monitoring trace hydrogen sulfide in blast furnace flue gas | |
| CN114397262A (en) | Method and system for correcting wave number drift of Fourier transform infrared spectrometer | |
| Lobo et al. | Calibration models for routine analysis of cider by mid-infrared spectroscopy | |
| CN111912804A (en) | Ultraviolet spectrum detection method and device for monitoring trace sulfur dioxide in blast furnace flue gas |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| PB01 | Publication | ||
| PB01 | Publication | ||
| SE01 | Entry into force of request for substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| CB02 | Change of applicant information | ||
| CB02 | Change of applicant information |
Address after: 201906 Shanghai Baoshan District Fu Lian two road 177 Lane 13 Building Applicant after: Shanghai Anjie Zhichuang Technology Co.,Ltd. Address before: 201906 Shanghai Baoshan District Fu Lian two road 177 Lane 13 Building Applicant before: SHANGHAI ANJIE ENVIRONMENTAL PROTECTION SCIENCE & TECHNOLOGY Co.,Ltd. |
|
| GR01 | Patent grant | ||
| GR01 | Patent grant |