KR20160091187A - laser-induced plazma spectroscopy and laser induced plazma spectroscopic analyzer - Google Patents
laser-induced plazma spectroscopy and laser induced plazma spectroscopic analyzer Download PDFInfo
- Publication number
- KR20160091187A KR20160091187A KR1020150011522A KR20150011522A KR20160091187A KR 20160091187 A KR20160091187 A KR 20160091187A KR 1020150011522 A KR1020150011522 A KR 1020150011522A KR 20150011522 A KR20150011522 A KR 20150011522A KR 20160091187 A KR20160091187 A KR 20160091187A
- Authority
- KR
- South Korea
- Prior art keywords
- light
- laser
- sample
- focusing
- plasma
- Prior art date
Links
- 238000004611 spectroscopical analysis Methods 0.000 title description 3
- 238000004458 analytical method Methods 0.000 claims abstract description 15
- 238000000034 method Methods 0.000 claims abstract description 15
- 238000001228 spectrum Methods 0.000 claims abstract description 15
- 238000002536 laser-induced breakdown spectroscopy Methods 0.000 claims abstract description 12
- 230000001678 irradiating effect Effects 0.000 claims abstract description 5
- 239000013307 optical fiber Substances 0.000 claims description 34
- 230000003287 optical effect Effects 0.000 claims description 10
- 230000003595 spectral effect Effects 0.000 claims description 6
- 239000013077 target material Substances 0.000 abstract description 12
- 238000010183 spectrum analysis Methods 0.000 abstract description 2
- 229910001385 heavy metal Inorganic materials 0.000 description 8
- 239000002689 soil Substances 0.000 description 7
- 239000000126 substance Substances 0.000 description 7
- 238000003780 insertion Methods 0.000 description 4
- 230000037431 insertion Effects 0.000 description 4
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 3
- HCHKCACWOHOZIP-UHFFFAOYSA-N Zinc Chemical compound [Zn] HCHKCACWOHOZIP-UHFFFAOYSA-N 0.000 description 3
- 229910052793 cadmium Inorganic materials 0.000 description 3
- BDOSMKKIYDKNTQ-UHFFFAOYSA-N cadmium atom Chemical compound [Cd] BDOSMKKIYDKNTQ-UHFFFAOYSA-N 0.000 description 3
- 230000000052 comparative effect Effects 0.000 description 3
- 229910052802 copper Inorganic materials 0.000 description 3
- 239000010949 copper Substances 0.000 description 3
- 229910052725 zinc Inorganic materials 0.000 description 3
- 239000011701 zinc Substances 0.000 description 3
- 238000001479 atomic absorption spectroscopy Methods 0.000 description 2
- 239000000356 contaminant Substances 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 238000001095 inductively coupled plasma mass spectrometry Methods 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 230000010355 oscillation Effects 0.000 description 2
- 238000012545 processing Methods 0.000 description 2
- 238000009614 chemical analysis method Methods 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 238000000605 extraction Methods 0.000 description 1
- 239000000383 hazardous chemical Substances 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000012544 monitoring process Methods 0.000 description 1
- 238000007670 refining Methods 0.000 description 1
- 230000000452 restraining effect Effects 0.000 description 1
- 238000005070 sampling Methods 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
- 238000002798 spectrophotometry method Methods 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
- G01J3/28—Investigating the spectrum
-
- 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
- G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
- G01N21/71—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light thermally excited
- G01N21/718—Laser microanalysis, i.e. with formation of sample plasma
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2201/00—Features of devices classified in G01N21/00
- G01N2201/06—Illumination; Optics
- G01N2201/061—Sources
- G01N2201/06113—Coherent sources; lasers
Abstract
The present invention relates to a laser induced plasma spectrometry capable of securing data with high reliability by analyzing a spectrum of ambient light including more emission lines generated from a target material after focusing light emitted from the plasma, And a spectral analysis apparatus.
The laser induced plasma spectrometry improved the light receiving method of the present invention includes a laser irradiation step of irradiating a sample with a laser to generate a plasma, a focusing step of focusing the light emitted from the plasma in a predetermined direction, A light receiving step of excluding ambient light, and an analysis step of analyzing the spectrum of ambient light.
Description
[0001] The present invention relates to a laser induced plasma spectrometer and a laser induced plasma spectrometer using the same. More particularly, the present invention relates to a laser induced plasma spectrometer which improves the light receiving method and more specifically, And more particularly, to a laser induced plasma spectrometry capable of securing reliable data by analyzing a spectrum of ambient light.
Environmentally hazardous substances in soil have a wide range of species, and most of them are present in trace amounts in the environment and therefore involve considerable difficulty in the analysis process.
Chemical analysis methods such as Inductively Coupled Plasma Mass Spectrometry (ICP-MS) or Atomic Absorption Spectrometry (AAS) are used as methods for analyzing trace amounts of environmentally harmful substances such as heavy metals in soil Respectively.
The above methods require a lot of time, effort, and high cost through sampling, extraction, and complicated refining processes that are representative of the area to be contaminated. They also require expensive analytical instruments and skilled personnel. Therefore, there is a need for a technique capable of real-time monitoring of heavy metal substances harmful to the environment in a simple and quick manner while overcoming such shortcomings and ensuring analysis accuracy and rapid analysis speed.
One such technique is laser-induced breakdown spectroscopy (LIBS) or laser-induced plasma spectroscopy (LIPS), which focuses a laser beam onto a sample to excite a plasma generated by light energy, It is a spectrophotometric method used as a circle.
In this method, a laser pulse is irradiated onto a soil sample, and light emitted from the laser induced plasma, which is generated when intense pulse energy is transmitted to the material, is detected from the spectrum shape measured through the optical measuring system and the spectral unit, And the amount or type of a specific substance is analyzed. At high temperature, an emission line is generated from a specific material (the target material to be analyzed), and this emission line forms a peak in the intrinsic wavelength region in the spectrum analysis.
When analyzing using a spectrum, as shown in FIG. 1, a peak corresponding to a wavelength range of a target material such as a heavy metal, and a base continuous line base not corresponding to the wavelength range of the target material Can exist. Such basecontinuous lines may be light scattered by the nature of the soil medium itself, rather than by heavy metals. Thus, these background continuous bands can cause the reliability of the analysis to be reduced.
Korean Patent Registration No. 10-1084766 discloses a method of obtaining data including peaks and background continuous lines corresponding to a wavelength range of a target material in order to minimize influence of a medium and improve reliability of analysis Discloses a heavy metal analysis method capable of securing only a peak corresponding to a wavelength range of a target material by removing continuous bases from the background.
However, the above-mentioned patent has a problem in that data must be additionally processed in that data including only a background continuous line is first acquired and then processed to secure only a peak corresponding to a wavelength range of a target material.
The present invention has been made in order to solve the above problems, and it is an object of the present invention to provide a laser induced plasma spectrometry method capable of directly obtaining data in which a background continuous line is removed without processing additional data by improving the light receiving method of light emitted from the plasma And an object of the present invention is to provide a laser induced plasma spectrometer using the same.
According to an aspect of the present invention, there is provided a laser-induced plasma spectrometry including: a laser irradiation step of irradiating a sample with a laser to generate a plasma; A focusing step of focusing the light emitted from the plasma in a predetermined direction; A light receiving step of excluding the central portion of the focused light to obtain ambient light; And analyzing the spectrum of the ambient light.
Wherein the light receiving step is performed by disposing an optical fiber outside the central portion of the focused light to obtain the ambient light.
The spectral data obtained in the analysis step is characterized in that the background base line is reduced or eliminated.
In order to accomplish the above object, the present invention provides a laser induced plasma spectrometer comprising: a laser generator for emitting a laser toward a sample; A light focusing unit for focusing the light emitted from the plasma derived from the sample in a predetermined direction; A light receiving unit which excludes a central portion of the light focused by the light focusing unit to obtain ambient light; And an analysis unit for analyzing the spectrum of the ambient light obtained through the light receiving unit.
The light-receiving unit includes a light-receiving case having an irradiation surface to which the light converged by the light focusing unit is irradiated, and an optical fiber supported at the light-receiving case and having an end located in an area off the center of the irradiation surface.
As described above, according to the present invention, only the ambient light including more emission lines generated from the target material after focusing the light emitted from the plasma is received and analyzed. Thus, the background continuous line is removed Data can be obtained.
Therefore, the present invention has an advantage of securing data with enhanced reliability of analysis.
1 is a graph of spectroscopic data obtained by a conventional laser induced plasma spectrometry,
2 is a perspective view schematically showing a laser induced plasma spectrometer according to an embodiment of the present invention,
FIG. 3 is a diagram showing the operation of the laser induced plasma spectrometer of FIG. 2,
FIG. 4 is a perspective view showing a principal part of a light receiving unit applied to FIG. 2,
5 is a view for showing ambient light in the light focused by the light focusing unit,
FIG. 6 is a view showing an arrangement state of the optical fiber seen from the front of the light receiving portion of FIG. 4,
FIG. 7 is a view showing an arrangement state of the optical fiber seen from the rear side of the light receiving portion of FIG. 4,
8 is a view showing an arrangement state of the optical fiber seen from the front face of the light receiving unit applied to another embodiment,
FIG. 9 is a view showing an arrangement state of the optical fiber seen from the rear side of the light receiving portion of FIG. 8,
10 is a view showing an arrangement state of the optical fiber seen from the front face of the light receiving unit applied to another embodiment,
FIG. 11 is a view showing an arrangement state of the optical fiber seen from the rear side of the light receiving portion of FIG. 10,
12 is a photograph of light emitted from a plasma generated by irradiating a sample with a laser,
13 and 14 are comparative data and experimental data of copper, zinc and cadmium,
15 and 16 are lead comparison data and experimental data.
Hereinafter, a laser induced plasma spectrometry method and a laser induced plasma spectrometer using the same according to a preferred embodiment of the present invention will be described in detail with reference to the accompanying drawings.
2 to 4, a laser induced plasma spectrometer according to an embodiment of the present invention includes a laser generating unit for emitting a
The
The
The
The
The
The
The pressurizing
The upper portion of the
The
The
The engaging portion is provided on the
The
The rotary drive unit rotates the
The
As an example of the sample, soil may be applied. In this case, contaminants such as heavy metals contained in the soil are quantitatively or qualitatively analyzed using the present invention. Here, a contaminant such as heavy metals means a target material to be analyzed.
The
A first
The
The
The second
The
In the present invention, the
The present invention excludes the central light A through the
As shown in FIG. 12, the central portion of the light emitted from the plasma is white, but the edge portions are red and blue. This seems to be due to the concentration of the emission line generated from the target material at the edge portion of the light emitted from the plasma. Accordingly, the central portion of the light emitted from the plasma is excluded, only the ambient light is obtained, and the spectral data is analyzed from the central portion, thereby obtaining the spectral data from which the background continuous line is removed.
The
The
A plurality of
The end of the
The other end of the
8 and 9 illustrate a light receiving unit that can be applied to another embodiment of the present invention. FIG. 8 is a view schematically showing the arrangement state of the optical fibers viewed from the front of the light receiving unit, and FIG. 9 is a view showing the arrangement state of the optical fibers viewed from the rear side of the light receiving unit.
Fig. 8 shows that the
10 and 11 illustrate a light-receiving portion that can be applied to another embodiment of the present invention. FIG. 10 is a view schematically showing the arrangement state of the optical fibers viewed from the front of the light receiving unit, and FIG. 11 is a view showing an arrangement state of the optical fibers viewed from the rear side of the light receiving unit.
Fig. 10 shows that the
With the structure of the light receiving portion as described above, the center light is excluded from the light focused by the light focusing portion, and only the surrounding light corresponding to the end portion of the optical fiber is transmitted through the optical fiber.
Referring to FIG. 2, the
The
Hereinafter, an analysis method using the laser induced plasma spectrometer shown in FIG. 2 to FIG. 4 will be described.
First, a laser is irradiated to the
After the
Power is supplied to the
Next, the light emitted from the plasma is focused in a predetermined direction.
The light emitted from the plasma is reflected in a direction set by the
The light reflected by the
Next, the
The ambient light transmitted through the
As described above, according to the present invention, only the ambient light including more emission lines generated from the target material after focusing the light emitted from the plasma is received and analyzed, so that the background continuous line is reduced or eliminated without processing additional data Spectral data can be obtained. Therefore, it is possible to secure data that increases the reliability of the analysis.
<Experimental Example>
The comparison data obtained by transmitting all of the collected light to the analyzer using the same soil sample and the experimental data obtained after receiving only the ambient light among the collected light using the light receiving unit as shown in FIG.
FIG. 6 shows comparative data of copper, zinc and cadmium, and FIG. 7 shows experimental data of copper, zinc and cadmium.
FIG. 7 shows that the background continuous lines are removed much in comparison with FIG. Therefore, FIG. 7 shows that the shape of the peak is clear and the intensity is higher.
In FIG. 6, the area of the peak is about 2.43, whereas in FIG. 7, the area of the peak is about 6.86, which is about 2.8 times that of the peak.
Fig. 8 is comparative data of lead, and Fig. 9 is experimental data of lead.
Comparing FIG. 8 and FIG. 9, it can be seen that FIG. 9 shows that the base line is removed much more than in FIG. 8, and the shape and strength of the peak are more pronounced and higher.
In FIG. 8, the peak area value is about 0.94, whereas in FIG. 9, the peak area value is about 4.22, which is quantitatively increased by about 4.5 times.
From these experimental results, it was confirmed that the reliability of the analysis can be improved by extracting and analyzing only the ambient light after focusing the light emitted from the plasma.
While the present invention has been particularly shown and described with reference to exemplary embodiments thereof, it will be understood by those skilled in the art that various changes and modifications may be made without departing from the scope of the invention. . Accordingly, the true scope of protection of the present invention should be determined only by the appended claims.
10: Sample
20: frame part 30: sample mounting part
40: laser generating unit 50: light focusing unit
60: light receiving section 70:
80: Analytical Department
Claims (5)
A focusing step of focusing the light emitted from the plasma in a predetermined direction;
A light receiving step of excluding the central portion of the focused light to obtain ambient light;
And analyzing the spectrum of the ambient light by using a laser beam.
A light focusing unit for focusing the light emitted from the plasma derived from the sample in a predetermined direction;
A light receiving unit which excludes a central portion of the light focused by the light focusing unit to obtain ambient light;
And an analyzer for analyzing the spectrum of the ambient light obtained through the light receiving unit.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
KR1020150011522A KR20160091187A (en) | 2015-01-23 | 2015-01-23 | laser-induced plazma spectroscopy and laser induced plazma spectroscopic analyzer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
KR1020150011522A KR20160091187A (en) | 2015-01-23 | 2015-01-23 | laser-induced plazma spectroscopy and laser induced plazma spectroscopic analyzer |
Publications (1)
Publication Number | Publication Date |
---|---|
KR20160091187A true KR20160091187A (en) | 2016-08-02 |
Family
ID=56708277
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
KR1020150011522A KR20160091187A (en) | 2015-01-23 | 2015-01-23 | laser-induced plazma spectroscopy and laser induced plazma spectroscopic analyzer |
Country Status (1)
Country | Link |
---|---|
KR (1) | KR20160091187A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR20190083455A (en) * | 2018-01-04 | 2019-07-12 | 목포대학교산학협력단 | Apparatus and method for optimization and monitoring of sample surface height in a laser induced plasma spectrometer |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR101084766B1 (en) | 2009-12-30 | 2011-11-22 | 광주과학기술원 | Method for analyzing of heavy metals |
-
2015
- 2015-01-23 KR KR1020150011522A patent/KR20160091187A/en not_active Application Discontinuation
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR101084766B1 (en) | 2009-12-30 | 2011-11-22 | 광주과학기술원 | Method for analyzing of heavy metals |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR20190083455A (en) * | 2018-01-04 | 2019-07-12 | 목포대학교산학협력단 | Apparatus and method for optimization and monitoring of sample surface height in a laser induced plasma spectrometer |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US11248961B2 (en) | Methods and systems for analyzing samples | |
US5617205A (en) | Spectral measuring method and spectral measuring apparatus | |
CN108872075B (en) | Detection system and method for heavy metals in water | |
US7692789B1 (en) | High resolution analysis of soil elements with laser-induced breakdown | |
US20170234800A1 (en) | Laser Induced Breakdown Spectroscopy (LIBS) Apparatus for the Detection of Mineral and Metal Contamination in Liquid Samples | |
EP1792166A1 (en) | Apparatus and method for producing a calibrated raman spectrum | |
US9304086B2 (en) | Raman spectrometry method and Raman spectrometry apparatus | |
KR101084766B1 (en) | Method for analyzing of heavy metals | |
US20160169805A1 (en) | Combined raman spectroscopy and laser-induced breakdown spectroscopy | |
KR20150051579A (en) | Laser induced plazma spectroscopic analyzer | |
JP2009288068A (en) | Analyzing method and analyzer | |
US20160116334A1 (en) | Multi-well plate for use in raman spectroscopy | |
JP2010276361A (en) | Abnormal state inspecting device | |
KR20160091187A (en) | laser-induced plazma spectroscopy and laser induced plazma spectroscopic analyzer | |
CN108303410B (en) | Trace element and isotope automatic detection system thereof | |
JP2016142556A (en) | Resin identification device | |
JP2012207935A (en) | Raman spectrometer and identification device using the same | |
JP2011226821A (en) | Identification device and identification method | |
KR101674395B1 (en) | method for analyzing soil using laser-induced plazma spectroscopy | |
JP2009288067A (en) | Analyzing method and analyzer | |
JP5980653B2 (en) | Deposit analysis method and deposit analysis apparatus | |
JP2005201762A (en) | Lithium leak detector and lithium leak detection method | |
JP2002005835A (en) | Raman spectroscopic measuring apparatus and analytical method for living body sample using the same | |
JP6027459B2 (en) | Deposit analyzer | |
CN107402196B (en) | X-ray fluorescence analysis instrument and sample container therefor |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
A201 | Request for examination | ||
E902 | Notification of reason for refusal | ||
E601 | Decision to refuse application |