CN201449373U - Photoelectric double-pulse laser induced breakdown spectrometer - Google Patents
Photoelectric double-pulse laser induced breakdown spectrometer Download PDFInfo
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- CN201449373U CN201449373U CN2009200613240U CN200920061324U CN201449373U CN 201449373 U CN201449373 U CN 201449373U CN 2009200613240 U CN2009200613240 U CN 2009200613240U CN 200920061324 U CN200920061324 U CN 200920061324U CN 201449373 U CN201449373 U CN 201449373U
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Abstract
The utility model discloses a photoelectric double-pulse laser induced breakdown spectrometer, which comprises a pulse laser, a focusing lens, a moving platform, a discharge electrode, a photodiode, a pulse time-delay controller, a high-voltage pulse power source, an optical collection system of optical radiation, a monochrometer or a spectrometer, a photoelectric converting element, a data acquisition unit and an electronic computer. The photoelectric double-pulse laser induced breakdown spectrometer is capable of substantially improving sensitivity of spectral analysis.
Description
Technical field
The utility model belongs to technical fields such as application of spectral technology, spectral analysis, detection and metering, is specifically related to a kind of photoelectric double-pulse laser induced breakdown spectrograph.
Background technology
Laser-induced Breakdown Spectroscopy (Laser-induced Breakdown Spectroscopy, LIBS) technology is with the surface generation high-temperature plasma of a branch of high-octane pulse laser focusing to a certain material to be analyzed, the small amount of matter that is come out by laser lift-off in high-temperature plasma by atomization and ionization, and the characteristic spectrum radiation of sending atom or ion.Realize analysis by analyzing spectral intensity to concentration of element in the sample (perhaps content).This technology has the complicated sample of need not pre-treatment process, can realize fast, industry is online and characteristics such as remote analysis.Yet the LIBS analysis of technology sensitivity of monopulse is not high, thereby has restricted it in trace element express-analysis Application for Field.Develop in the world at present and dipulse LIBS technology, its sensitivity for analysis can exceed 1-2 the order of magnitude than monopulse LIBS technology.Dipulse LIBS needs two pulsed lasers, and shortcoming one is its system complex, cost height, and shortcoming two is that the pulse width of light pulse can't regulated at will, and wavelength also is restricted, thereby can't be from essence these physical parameters being carried out optimization.
In a lot of occasions, need carry out content analysis to the trace element in the sample: can be the analysis (such as the toxic heavy metal element in the various industrial and agricultural products) of objectionable impurities, also can be the functional composition of key or the analysis (such as functional trace element in the specific alloy) of material.Existing spectroscopic analysis methods or need complicated sample pre-treatment process, time-consuming and can't realize fast detecting (as atomic absorption spectrum, inductively coupled plasma----atom generation spectrum, inductively coupled plasma----analytical technique of mass spectrum); Though can realize express-analysis, sensitivity not high (as x-ray fluorescence, monopulse LIBS technology etc.).The purpose of this utility model is to solve the existing LIBS technology technical barrier that (comprising monopulse LIBS and dipulse LIBS technology), sensitivity for analysis was not high, thereby realizes the express-analysis to trace element in the various samples.
The utility model content
The utility model provides a kind of photoelectric double-pulse laser induced breakdown spectrograph that increases substantially spectral analysis sensitivity in order to overcome the deficiency that above prior art exists.
The purpose of this utility model realizes by following technical scheme: this photoelectric double-pulse laser induced breakdown spectrograph is characterized in that: collection optical system, monochromator or the spectrometer, photo-electric conversion element, data acquisition unit and the robot calculator that comprise pulsed laser, condenser lens, mobile platform, sparking electrode, optical diode, pulse delay controller, high-voltage pulse power source, optical radiation;
Described mobile platform is placed with sample, the laser that pulsed laser produces focuses on the sample by condenser lens, sparking electrode connects high-voltage pulse power source, and high-voltage pulse power source connects the pulse delay controller, and optical diode connects data acquisition unit and pulse delay controller simultaneously;
The collection optical system of optical radiation arrives the emission collection of the electric spark of arc discharge generation at the entrance slit place of monochromator or spectrometer, monochromator or spectrometer are connected with data acquisition unit by photo-electric conversion element, data acquisition unit connects robot calculator, and robot calculator connects monochromator or spectrometer.
Described pulsed laser is electric-optically Q-switched Nd:YAG laser instrument, pulse recurrence rate 1-10Hz, single pulse energy 30-100mJ; Described condenser lens is common K9 glass lens, focal length 10-15 centimetre.
Described mobile platform is for making the mobile platform of x-y both direction translation, and sample is solid, liquid or gas.
Described sparking electrode is the tungsten pin; The voltage of high-voltage pulse power source is 1000-5000V, and pulse current is 1-50A; The pulse delay controller is controlled by external trigger, produces time-delay and all adjustable TTL pulse signal of pulsewidth.
Described optical diode is silica-based PIN diode.
The collection optical system of described optical radiation is one group of lens or the optical fiber that has lens.
The focal length of described monochromator or spectrometer is 30 centimetres or 50 centimetres; Photo-electric conversion element is the CCD of photomultiplier or linear array; Data acquisition unit is the data transmission set of digital storage oscilloscope, high-speed a/d conversion equipment or CCD, and the sample frequency of data acquisition unit is more than 200MHz.
The spectroscopic analysis methods of above-mentioned photoelectric double-pulse laser induced breakdown spectrograph may further comprise the steps:
The first step: pulsed laser sends high power pulses laser and focuses on and produce the plasma spark on the sample through condenser lens, and sample ceaselessly moves and guarantees that short-pulse laser can not repeat to beat on a certain fixed position of sample;
Second step: pulse signal of generation removed trigger pulse delay controller and data acquisition unit simultaneously after optical diode received short-pulse laser;
The 3rd step: time-delay of output and all adjustable TTL pulse signal of pulsewidth after the pulse delay controller is triggered, the control high-voltage pulse power source, make time-delay of high-voltage pulse power source output and all controlled high-voltage pulse of pulsewidth, and be added in plasma spark upper and lower by sparking electrode, produce arc discharge;
The 4th step: the collection optical system of optical radiation arrives the emission collection of the electric spark of arc discharge generation at the entrance slit place of monochromator or spectrometer;
The 5th step: photo-electric conversion element is converted to electric signal with light signal;
The 6th step: data acquisition unit sends robot calculator to after the electrical signal collection of photo-electric conversion element and does data analysis, and robot calculator is controlled the output wavelength or the wavelength coverage of monochromator or spectrometer simultaneously;
The 7th step: robot calculator is chosen the interior integrated signal of suitable time range (sampling gate) as signal intensity, and this signal intensity is corresponding with the concentration of element in the sample;
The 8th step: the signal intensity of the known known sample of the signal intensity of sample and concentration of element is compared, analyze the concentration of element that draws in the sample.
The pulse delay controller in described second step comprises interconnective external trigger start unit, adjustable time delay unit, pulse-width regulated unit.
Principle of work of the present utility model is:
As shown in Figure 4, laser pulse at first produces laser plasma on sample to be analyzed, send short-life tough relative long atomic radiation of sub-radiation of sending a telegraph in the laser plasma with the life-span. wait tough sending a telegraph after the sub-radiation complete obiteration, a high-voltage pulse is discharged to laser plasma by the pair of metal sparking electrode, at this moment, atom in the plasma is excited once again, and launch the atomic radiation of enhancing, and its relaxation time is relevant with the pulsewidth of electric high-voltage pulse, pulsewidth by the broadening high-voltage pulse, can extend to the level of 60-100 microsecond the launch time of atomic radiation, and tough send a telegraph sub-radiation complete obiteration already this moment, the contribution of its background is zero. the position of the sampling gate by selecting suitable data acquisition, just can obtain the ratio of very high signal and background, thereby significantly strengthening the spectral detection sensitivity of LIBS technology. the utility model had both kept the advantage (because it need not sample pretreatment process) of LIBS technology express-analysis, again on the basis of monopulse LIBS technology, its sensitivity has been improved more than 2 orders of magnitude at least, thereby can realize high-sensitivity rapid detection and analysis various samples.
Because the enhancing of atomic radiation and the prolongation in relaxation time realize by electron collision, so the not homoatomic in its article on plasma body all has similar effect, and this just means that this atomic radiation enhancement techniques is all effective to all atoms.This be with LIF (laser-induced fluorescence (LIF)) technology in laser a certain atom selective excitation is strengthened the mechanism difference in itself of its radiation intensity.
Pulsed laser sends high power pulses laser, and the line focus lens focus is on testing sample and produce the plasma spark.Sparking electrode vertically is placed on the upper and lower of plasma spark.Testing sample is to be fixed on one on all can the mobile platform of translation on x, the y both direction, and in the measuring process, mobile platform ceaselessly moves laser is all beaten in the different position of sample at every turn.
Pulse signal of generation removed trigger pulse delay controller and data acquisition unit simultaneously after optical diode received short-pulse laser; Pulse delay controller output TTL pulse signal control high-voltage pulse power source makes time-delay of high-voltage pulse power source output and all controlled high-voltage pulse of pulsewidth, and is added in plasma spark upper and lower by sparking electrode, produces arc discharge; The collection optical system of optical radiation arrives the emission collection of the electric spark of arc discharge generation at the entrance slit place of monochromator or spectrometer; Photo-electric conversion element is converted to electric signal with light signal; Data acquisition unit sends robot calculator to after the electrical signal collection of photo-electric conversion element and does data analysis, and robot calculator is controlled the output wavelength or the wavelength coverage of monochromator or spectrometer simultaneously.
Last robot calculator is chosen the interior integrated signal of suitable time range (sampling gate) as signal intensity, and the concentration of element in this signal intensity and the sample (sample) (concentration of tested a certain element) has correspondence.The signal intensity of the known known sample of the signal intensity of sample and concentration of element is compared, analyze the concentration of element that draws in the sample.
The utility model has following advantage with respect to prior art:
One, this photoelectric double-pulse laser induced breakdown spectrograph and spectroscopic analysis methods, be on the basis of monopulse LIBS, add second high electric field pulse and strengthen the intensity of the atomic radiation in the laser plasma, and the relaxation time of prolongation atomic radiation is to improve atomic radiation and tough ratio of sending a telegraph the background of sub-radiation formation, (tough to send a telegraph sub-radiation be that the life-span is short, the white light that wavelength is continuous, can't utilize monochromator splitting that it is carried out filtering), thereby the utility model significantly improves spectral detection sensitivity, than the sensitivity of monopulse LIBS technology improve 2 quantity and more than, go out 1 more than the order of magnitude than the sensitivity of dipulse LIBS technology is taller.Thereby the utility model can be realized qualitative and quantitative analysis fast and detection to trace element in the various samples.
Two, the raising of the utility model sensitivity for analysis is the element that can analyze at all, just is not confined to above the single-element.This just means can realize, high-sensitive and fast analyzing and testing simultaneously to multielement.(LIF, laser-inducedfluorescence) technology has in essence progress in conjunction with the technology that realizes the highly sensitive detection of single element for this point and LIBS and laser-induced fluorescence (LIF).
Three, system architecture simple, be easy to realize, cost is low.
Description of drawings
Fig. 1 is the structural representation of photoelectric double-pulse laser induced breakdown spectrograph of the present utility model.
Fig. 2 is the structural representation of collection optical system of the optical radiation of Fig. 1.
Fig. 3 is another structural representation of collection optical system of the optical radiation of Fig. 1.
Fig. 4 is the principle schematic of photoelectric double-pulse laser induced breakdown spectral technique of the present utility model.
Fig. 5 utilizes the photoelectric double-pulse laser two of Fig. 1 to lead the experimental result picture that breakdown spectrograph obtains.
Embodiment
The utility model is described in further detail below in conjunction with drawings and Examples.
Photoelectric double-pulse laser induced breakdown spectrograph as shown in Figure 1 comprises collection optical system 8, monochromator 9 (monochromator also available light spectrometer replaces), photo-electric conversion element 10, data acquisition unit 11 and the robot calculator 12 of pulsed laser 1, condenser lens 2, mobile platform 3, sparking electrode 4, optical diode 5, pulse delay controller 6, high-voltage pulse power source 7, optical radiation;
Described mobile platform 3 is placed with sample, the laser that pulsed laser 1 produces focuses on the sample by condenser lens 2, sparking electrode 4 connects high-voltage pulse power source 7, high-voltage pulse power source 7 connects pulse delay controller 6, and optical diode 5 connects data acquisition unit 11 and pulse delay controller 6 simultaneously;
The collection optical system 8 of optical radiation arrives the emission collection of the electric spark of arc discharge generation at the entrance slit place of monochromator 9, monochromator 9 is connected with data acquisition unit 11 by photo-electric conversion element 10, data acquisition unit 11 connects robot calculator 12, and robot calculator 12 connects monochromator 9.
Described pulsed laser is electric-optically Q-switched Nd:YAG laser instrument, pulse recurrence rate 1-10Hz, single pulse energy 30-100mJ; Described condenser lens is common K9 glass lens, focal length 10-15 centimetre.
Described mobile platform is for making the mobile platform of x-y both direction translation, and sample is solid, liquid or gas.
Described sparking electrode is the tungsten pin; The voltage of high-voltage pulse power source is 1000-5000V, and pulse current is 1-50A; The pulse delay controller is controlled by external trigger, produces time-delay and all adjustable TTL pulse signal of pulsewidth.
Described optical diode is silica-based PIN diode.
As shown in Figure 2, the collection optical system of described optical radiation is that two lens a and b (also can adopt the optical fiber d that has lens c to replace, as shown in Figure 3).
The focal length of described monochromator is 30 centimetres or 50 centimetres; Photo-electric conversion element is photomultiplier (if spectrometer, then photo-electric conversion element adopts the CCD of linear array); Data acquisition unit is the data transmission set of digital storage oscilloscope, high-speed a/d conversion equipment or CCD, and the sample frequency of data acquisition unit is more than 200MHz.
The spectroscopic analysis methods of above-mentioned photoelectric double-pulse laser induced breakdown spectrograph may further comprise the steps:
The first step: pulsed laser sends high power pulses laser and focuses on and produce the plasma spark on the sample through condenser lens, and sample ceaselessly moves and guarantees that short-pulse laser can not repeat to beat on a certain fixed position of sample;
Second step: pulse signal of generation removed trigger pulse delay controller and data acquisition unit simultaneously after optical diode received short-pulse laser;
The 3rd step: time-delay of output and all adjustable TTL pulse signal of pulsewidth after the pulse delay controller is triggered, the control high-voltage pulse power source, make time-delay of high-voltage pulse power source output and all controlled high-voltage pulse of pulsewidth, and be added in plasma spark upper and lower by sparking electrode, produce arc discharge;
The 4th step: the collection optical system of optical radiation arrives the emission collection of the electric spark of arc discharge generation at the entrance slit place of monochromator or spectrometer;
The 5th step: photo-electric conversion element is converted to electric signal with light signal;
The 6th step: data acquisition unit sends robot calculator to after the electrical signal collection of photo-electric conversion element and does data analysis, and robot calculator is controlled the output wavelength or the wavelength coverage of monochromator or spectrometer simultaneously;
The 7th step: robot calculator is chosen the interior integrated signal of suitable time range (sampling gate) as signal intensity, and this signal intensity is corresponding with the concentration of element in the sample;
The 8th step: the signal intensity of the known known sample of the signal intensity of sample and concentration of element is compared, analyze the concentration of element that draws in the sample.
The pulse delay controller in described second step comprises interconnective external trigger start unit, adjustable time delay unit, pulse-width regulated unit.
Fig. 5 is the experimental result picture that utilizes photoelectric double-pulse laser induced breakdown spectrograph of the present utility model to obtain: the time-domain diagram of mercury atom emission in certain paint sample under the photoelectric double-pulse excitation mode.
The sparking voltage of sparking electrode: 4500V, discharge current 3A.Result when wherein the curve signal among the figure 1 is 253.65 nanometers (analysis of line wavelength of mercury atom) for detecting wavelength; 2 is that the detection wavelength is the background wavelength (not observing the radiation of other atom at this) of 252.5 nanometers.The signal (or background) of 0-7 microsecond scope is that laser pulse forms, and (background) small peak of 7-10 microsecond is that arc discharge produces toughly sends a telegraph sub-radiation; It is formed that signal (background) in the 10-55 microsecond scope is that electric pulse excites.The ratio of the signal in the contrast 10-50 microsecond scope and the ratio of background, the signal in the 0-7 microsecond scope and background, the former is obviously greater than the latter as can be seen.Further improve discharge current and can further improve this ratio.
Above-mentioned embodiment is a preferred embodiment of the present utility model; can not limit claim of the present utility model; other any change that does not deviate from the technical solution of the utility model and made or other equivalent substitute mode are included within the protection domain of the present utility model.
Claims (7)
1. photoelectric double-pulse laser induced breakdown spectrograph is characterized in that: collection optical system, monochromator or the spectrometer, photo-electric conversion element, data acquisition unit and the robot calculator that comprise pulsed laser, condenser lens, mobile platform, sparking electrode, optical diode, pulse delay controller, high-voltage pulse power source, optical radiation;
Described mobile platform is placed with sample, the laser that pulsed laser produces focuses on the sample by condenser lens, sparking electrode connects high-voltage pulse power source, and high-voltage pulse power source connects the pulse delay controller, and optical diode connects data acquisition unit and pulse delay controller simultaneously;
The collection optical system of optical radiation arrives the emission collection of the electric spark of arc discharge generation at the entrance slit place of monochromator or spectrometer, monochromator or spectrometer are connected with data acquisition unit by photo-electric conversion element, data acquisition unit connects robot calculator, and robot calculator connects monochromator or spectrometer.
2. photoelectric double-pulse laser induced breakdown spectrograph according to claim 1 is characterized in that: described pulsed laser is electric-optically Q-switched Nd:YAG laser instrument, pulse recurrence rate 1-10Hz, single pulse energy 30-100mJ; Described condenser lens is common K9 glass lens, focal length 10-15 centimetre.
3. photoelectric double-pulse laser induced breakdown spectrograph according to claim 1 is characterized in that: described mobile platform is for making the mobile platform of x-y both direction translation, and sample is solid, liquid or gas.
4. photoelectric double-pulse laser induced breakdown spectrograph according to claim 1 is characterized in that: described sparking electrode is the tungsten pin; The voltage of high-voltage pulse power source is 1000-5000V, and pulse current is 1-50A; The pulse delay controller is controlled by external trigger, produces time-delay and all adjustable TTL pulse signal of pulsewidth.
5. photoelectric double-pulse laser induced breakdown spectrograph according to claim 1 is characterized in that: described optical diode is silica-based PIN diode.
6. photoelectric double-pulse laser induced breakdown spectrograph according to claim 1 is characterized in that: the collection optical system of described optical radiation is one group of lens or the optical fiber that has lens.
7. photoelectric double-pulse laser induced breakdown spectrograph according to claim 1 is characterized in that: the focal length of described monochromator or spectrometer is 30 centimetres or 50 centimetres; Photo-electric conversion element is the CCD of photomultiplier or linear array; Data acquisition unit is the data transmission set of digital storage oscilloscope, high-speed a/d conversion equipment or CCD, and the sample frequency of data acquisition unit is more than 200MHz.
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| CN2009200613240U CN201449373U (en) | 2009-07-28 | 2009-07-28 | Photoelectric double-pulse laser induced breakdown spectrometer |
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Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN103091289A (en) * | 2012-12-21 | 2013-05-08 | 吉林大学 | Automatic experimental platform based on laser-induced breakdown spectroscopy analysis technology |
| CN104181146A (en) * | 2013-05-22 | 2014-12-03 | 中国科学院光电研究院 | Multipulse laser-induced breakdown spectrum on-line detection system |
| CN106680247A (en) * | 2015-11-11 | 2017-05-17 | 以恒激光科技（北京）有限公司 | Heavy metal detection equipment |
| CN107064111A (en) * | 2017-05-15 | 2017-08-18 | 华南理工大学 | Gao Zhongying laser lift-off spark induced breakdown spectroscopy elemental analysis system and method |
| CN107884395A (en) * | 2017-12-27 | 2018-04-06 | 冶金自动化研究设计院 | Diffused with laser ablation point and produce the device and method of spectrometer trigger pulse |
-
2009
- 2009-07-28 CN CN2009200613240U patent/CN201449373U/en not_active Expired - Fee Related
Cited By (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN103091289A (en) * | 2012-12-21 | 2013-05-08 | 吉林大学 | Automatic experimental platform based on laser-induced breakdown spectroscopy analysis technology |
| CN103091289B (en) * | 2012-12-21 | 2014-12-03 | 吉林大学 | Automatic experimental platform based on laser-induced breakdown spectroscopy analysis technology |
| CN104181146A (en) * | 2013-05-22 | 2014-12-03 | 中国科学院光电研究院 | Multipulse laser-induced breakdown spectrum on-line detection system |
| CN106680247A (en) * | 2015-11-11 | 2017-05-17 | 以恒激光科技（北京）有限公司 | Heavy metal detection equipment |
| CN107064111A (en) * | 2017-05-15 | 2017-08-18 | 华南理工大学 | Gao Zhongying laser lift-off spark induced breakdown spectroscopy elemental analysis system and method |
| CN107064111B (en) * | 2017-05-15 | 2023-04-21 | 华南理工大学 | High-repetition-frequency laser stripping-spark induced breakdown spectroscopy element analysis system and method |
| CN107884395A (en) * | 2017-12-27 | 2018-04-06 | 冶金自动化研究设计院 | Diffused with laser ablation point and produce the device and method of spectrometer trigger pulse |
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Granted publication date: 20100505 Termination date: 20120728 |