CN104406942B - A kind of multi-mode laser induced breakdown spectroscopy device - Google Patents

A kind of multi-mode laser induced breakdown spectroscopy device Download PDF

Info

Publication number
CN104406942B
CN104406942B CN201410653808.XA CN201410653808A CN104406942B CN 104406942 B CN104406942 B CN 104406942B CN 201410653808 A CN201410653808 A CN 201410653808A CN 104406942 B CN104406942 B CN 104406942B
Authority
CN
China
Prior art keywords
laser
sample
mode
plasma
light path
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.)
Active
Application number
CN201410653808.XA
Other languages
Chinese (zh)
Other versions
CN104406942A (en
Inventor
何勇
彭继宇
刘飞
余克强
方慧
宋坤林
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Zhejiang University ZJU
Original Assignee
Zhejiang University ZJU
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Zhejiang University ZJU filed Critical Zhejiang University ZJU
Priority to CN201410653808.XA priority Critical patent/CN104406942B/en
Publication of CN104406942A publication Critical patent/CN104406942A/en
Application granted granted Critical
Publication of CN104406942B publication Critical patent/CN104406942B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/62Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
    • G01N21/71Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light thermally excited
    • G01N21/718Laser microanalysis, i.e. with formation of sample plasma

Landscapes

  • Health & Medical Sciences (AREA)
  • Physics & Mathematics (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Plasma & Fusion (AREA)
  • Optics & Photonics (AREA)
  • Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
  • Engineering & Computer Science (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Investigating, Analyzing Materials By Fluorescence Or Luminescence (AREA)

Abstract

The invention discloses a kind of multi-mode laser induced breakdown spectroscopy device, with conllinear, reheating, three kinds of mode of operations of pre-ablation;In conllinear mode of operation:The light path of Double-impulse solid laser is climbed system provided with light path, and the light path of laser is coaxially exported for raising 1064nm/532nm so that laser focuses on sample surfaces directly over sample stage, produces plasma;In reheating and pre-ablation mode of operation:The first laser of Double-impulse solid laser is climbed system, the light path for raising first laser into light path so that first laser focuses on sample surfaces directly over sample stage, produces plasma;Delay time generator controls the triggering sequential of first laser and second laser;The second laser of Double-impulse solid laser directly focuses to plasma;Also include signal acquisition and processing system, the characteristic spectral line sent is cooled down according to plasma and first laser impacts the spatial information of sample, distributed intelligence of the display elements in sample surfaces.

Description

A kind of multi-mode laser induced breakdown spectroscopy device
Technical field
The present invention relates to laser spectrum tech field, more particularly to a kind of multi-mode laser induced breakdown spectroscopy device.
Background technology
LIBS is Laser-Induced Breakdown Spectroscopy (laser induced breakdown spectrograph) abbreviation, Plasma ablation that the technology is produced using pulse laser simultaneously excites material in sample (normally solid), and pass through spectrum Instrument obtains the spectrum that Plasma-Atomic launched that is excited, and recognizes the element constituent in sample with this, and then can be with Carry out identification, classification, the qualitative and quantitative analysis of material.The technology can be realized quickly without being pre-processed to sample Remotely, it is micro- damage sample element (especially metallic element) is detected, available for solid, gas, fluid sample detection.Swash The application field of photoinduction breakdown spectral is also quite varied, heavy metal analysis in such as biomedicine, archaeology, environmental monitoring, water And explosive detection etc..
Compared with single-pulse laser induced breakdown spectroscopy, double-pulse laser induced breakdown spectrum can greatly enhance signal, carry The detection limit of high element.The mode of operation of double-pulse laser induced breakdown spectrum can be divided into conllinear formula and rectilinear.It is rectilinear again Pre-ablation pattern (pre-ablative) and reheat mode (re-heating) can be divided into.These three modes are each have their own excellent Point.However, the domestic and international three kinds of mode of operations that there is no Patents to realize LIBS on same device.
In general, the realization of these three mode of operations needs two systems.Such as patent application CN101620183B and specially Profit application CN102788772B realizes conllinear and non-colinear mode of operation with dual pulse welding and two lasers respectively. Also patent utilization light path realizes a certain working method with a laser, but its effect does not reach making for LIBS technologies With requiring.The induced with laser spectrum detection system that dipulse such as patent application CN103323435A defocuses pre-ablation utilizes 2 tunnels Light path realizes the conllinear dipulse mode of operations of LIBS, but its beam of laser and the sequential of the second beam laser are uncontrollable, Optimal spectral line can not be obtained.Although and the LIBS measurement apparatus described in patent application CN103529000A Vertical operation pattern is realized using the single tunnel light path of laser 2, but is usually Millisecond using the control time of optical shutter, The control requirement of LIBS Microsecond grades can not be realized.
The content of the invention
The integrated of three kinds of mode of operations of LIBS is realized on same device to realize, the invention discloses A kind of multi-mode laser induced breakdown spectroscopy device, reduces system building cost, simple with regulation, and it is excellent that adjustable parameter is more etc. Point.
The concrete technical scheme of the present invention is as follows:
A kind of multi-mode laser induced breakdown spectroscopy device, it is characterised in that including Double-impulse solid laser, sample stage With the delay time generator for controlling Double-impulse solid laser triggering sequential;Double-impulse solid laser has 1064nm coaxial Output, 532nm are coaxially exported, the different axle outputs of 1064nm and the different axle of 1064nm, 532nm export four kinds of way of outputs;
Described multi-mode laser induced breakdown spectroscopy device has conllinear, reheating, three kinds of mode of operations of pre-ablation;
In described conllinear mode of operation:The light path of the Double-impulse solid laser is climbed system provided with light path, should Light path climbs system for raising the light path that 1064nm/532nm coaxially exports laser so that laser is focused on directly over sample stage To sample surfaces, plasma is produced;
In described reheating and pre-ablation mode of operation:The first laser of the Double-impulse solid laser enters described Light path climb system, the light path is climbed the light path that system is used to raise first laser so that first laser by sample stage just on Side focuses on sample surfaces, produces plasma;During the triggering of described delay time generator control first laser and second laser Sequence;The second laser of the Double-impulse solid laser directly focuses to plasma;
Also include signal acquisition and processing system, the characteristic spectral line sent is cooled down according to plasma and first laser is impacted The spatial information of sample, distributed intelligence of the display elements in sample surfaces.
The present invention is built using a kind of Double-impulse solid laser (Lei Bao companies, Vlite200) and subsequent optical path system Realize 3 kinds of mode of operations of LIBS, and a variety of operation wavelengths switching.With pre-ablation, reheat and Conllinear Three models mode, wherein line mode have 2 operation wavelengths (532nm and 1064nm), and pre-ablation and reheating also have 2 Individual operation wavelength (2 tunnels are 1064nm, and 1064nm all the way, another road 532nm).
Energy attenuator is there also is provided on the optical axis of described Double-impulse solid laser and for detecting that record swashs in real time The laser energy real-time monitoring system of light energy;Described first laser enters light after laser energy real-time monitoring system outgoing Road is climbed system;Described second laser focuses to plasma after laser energy real-time monitoring system outgoing.Laser energy Real-time detecting system is mainly used in the energy of detection recording laser in real time, for subsequent data analysis.
When being detected using LIBS, sample properties to be detected are different, the laser energy needed for it Also it is different.To realize the detection of the fragile sample of such as plant leaf blade, animal tissue or reducing damage of the laser to sample, generally need The energy of laser is decayed.However, laser energy can be caused not to energy progress decay by adjusting laser diode voltage It is stable, and then influence testing result.The present invention is decayed using energy attenuator to laser energy, and its attenuation range is 1% ~99%.Laser energy real-time detecting system is mainly used in the energy of detection recording laser in real time, for judging energy of lasers Fluctuation whether there is exception, and carry out subsequent data analysis., can be right according to energy variation when subsequently carrying out data analysis The intensity of spectral line of acquisition is compensated.
Wherein, described signal acquisition and processing system includes:Optical fiber collection system, for collecting plasma cooling hair The characteristic spectral line gone out;Beam splitting system, for carrying out light splitting to characteristic spectral line;ICCD detectors, for the light of beam splitting system to be believed Number be converted to electric signal;Sample surface imaging system, for monitoring first laser impact sample position, obtains the space of sampled point Information;Computer, according to the spatial information of described electric signal and sampled point, distributed intelligence of the display elements in sample surfaces.
It is preferred that, described beam splitting system is echelle spectrometer.
Echelle spectrometer is the spectrometer using echelle grating as dispersion element, can one without raster scanning Secondary property obtains full modal data, is avoided that conventional spectrograph multichannel head and the tail section Bonding Problem.Nothing inside echelle spectrometer Mechanical part, stability is higher, and resolution ratio can reach 0.08nm, can meet spectral line light splitting requirement.
Wherein, described sample surface imaging system includes:LED light source for illuminating for illuminating sample from positive direction, position Beam splitter on LED light source for illuminating optical axis, CCD camera and imaging lens, the sample surfaces figure for gathering beam splitter reflection As information.
It is preferred that, described light path climb system by the first speculum, the second speculum and the 3rd speculum group into described Second speculum is located at the surface of the first speculum, and the 3rd speculum is located at the surface of sample stage;The first described reflection Mirror, the second speculum and the 3rd speculum are Nd:YAG double-frequency laser speculums.
The light path system of climbing is mainly used in lifting light path, and laser will be converted into and vertically propagate in the horizontal direction. Can be prevented effectively from rise laser positions using the light path system of climbing causes the laser factors of instability.Laser is directly over sample Sample surfaces are impacted, are conducive to effectively exciting for plasma, it is ensured that plasma is uniformly and symmetrically distributed.
Described delay time generator control Double-impulse solid laser adjusts Q triggered times and xenon lamp to open the triggered time, prolongs When generator set Double-impulse solid laser adjust Q signal triggered time xenon lamp signal triggering after 150 ± 20 μ s.This when The setting of sequence can at utmost ensure the energy stability of Double-impulse solid laser.
It is preferred that, first laser and the second laser focusing is arranged on along the lens that optical axis is slidably matched with lens and installed On frame;Described first laser light path focusing plates V-arrangement film with lens surface, and its reflectivity at 532nm, 1064nm is less than 0.25%.
The distance of lens and sample is the important parameter of LIBS, directly affects laser in object to be excited Laser parameter.As a rule, the distance of lens and sample should be less than the focal length of lens.When lens and sample distance reduce, The diameter of impact point will increase, and radiancy and fluence can reduce.Therefore, lens are arranged on to slide along optical axis and matched somebody with somebody The Lens mounting carrier of conjunction can be according to sample properties and the distance of actual demand accurate adjustment lens and sample.Due to dipulse solid The optical maser wavelength of laser is 532nm and 1064nm, to reduce loss of the laser energy in light path system, it is ensured that laser energy Effective rate of utilization, described lens surface plating V-arrangement film, its reflectivity 532nm, 1064nm at is less than 0.25%.Described Lens plating V-arrangement film can effectively for selected Double-impulse solid laser wavelength, make its reflection at 532nm, 1064nm Rate is less than 0.25%.
As an improvement, described sample stage includes the electric displacement platform with four-degree-of-freedom, the liter being movably arranged on electric displacement platform Drop plate and the objective table being slidably fitted on electric displacement platform;The lifter plate is provided with transparent constraint window, laser light constraint Sample is impacted after window;The lower section of the lifter plate is provided with restraining plate, and the restraining plate, which is placed on the surface of sample, restraining plate, to be divided Cloth Constrained chamber, the constraint chamber is used for the plasma for constraining sample excitation.
Sample stage limits enhanced line intensity by space, and energy plasma is laterally and row constraint, and root are entered in longitudinal direction The big minor adjustment the intensity of spectral line of constraint space is adjusted according to different sample requirements, the intensity of spectral line enhancing scope is 2~10 times.Constrain window Mouth is mainly used in plasma and longitudinally enters row constraint, and the characteristic spectral line produced to incident laser and plasma has preferably Transmissivity.The transverse direction that restraining plate is mainly used in plasma enters row constraint, and characteristic spectral line is carried out constraint propagation, improves Spectral line collection efficiency and the intensity of spectral line.
It is preferred that, described lifter plate is provided with light-transmitting opening, the light-transmitting opening covered with light-passing board, the light-transmitting opening with thoroughly The described constraint window of tabula rasa composition.
Wherein, light-passing board is poly (methyl methacrylate) plate, and the selection of material is N-BK7, and thickness is 1~5mm, and transmitance is more than 90%, Energy threshold is more than 10J/cm2.Line enhancement effect suffers restraints window from the influence with a distance from sample.By properties of samples and institute The element spectral line intensity to be detected is different, and constraint window of the invention can be moved in vertical direction, as needed regulation spectrum Line strength.To ensure that laser effectively excites effective collection with characteristic spectral line, light-passing board is saturating to optical maser wavelength and characteristic spectral line The rate of mistake should be greater than 90%.Meanwhile, to prevent laser from being caused damage to poly (methyl methacrylate) plate, its energy threshold should be greater than 10J/cm2
Restraining plate is the aluminium sheet of chromium plating, and thickness is 1~3mm.Aluminium sheet constraint intracavitary carry out chromium plating, make inner chamber have compared with High reflectivity, makes characteristic spectral line constraint propagation, improves spectral line collection efficiency.
The Double-impulse solid laser that the present invention is used, its energy hole is realized by energy attenuator, it is to avoid utilize voltage Directly regulation causes energy of lasers unstable.Laser is adjusted using sample stage and the Lens mounting carrier that can be moved along optical axis direction Running parameter.First mode of operation is conllinear mode of operation, and delay time generator control first laser launches sequential in second laser Before transmitting, it is only necessary to control the displacement of sample stage Z-direction to adjust the spot size of Laser Focusing point.Second mode of operation is to add again Thermal technology's operation mode, delay time generator control first laser transmitting sequential controls sample stage, adjusts Z before second laser transmitting Direction displacement height, makes second laser (1064nm) light-emitting window higher than 1 ± 0.5mm above plasma confinement plate, regulation first, Second lens group mounting bracket controls the spot size of Laser Focusing point.3rd mode of operation is pre-ablation mode of operation, delay hair Raw device control first laser transmitting sequential controls sample stage, adjusts Z-direction displacement height after second laser transmitting, makes the Dual-laser (1064nm) light-emitting window adjusts first, second lens group mounting bracket higher than 1 ± 0.5mm above plasma confinement plate Control the spot size of Laser Focusing point.Because the shape and characteristic of sample have differences, sample stage uses 4DOF (X, Y, Z And W) sample stage, including 3 single-degree-of-freedom (X, Y and Z) pulse electric displacement platforms and rotary freedom (W) electronic rotation Platform.When sample is spherical (such as apple, pear and other fruits), from whole frees degree;When sample surfaces are regular planar, select XYZ Three Degree Of Freedoms can meet requirement.
The invention has the advantages that:
(1) three kinds of mode of operations of double-pulse laser induced breakdown spectrum are realized, for selection optimum working mode detection Sample elements content provides condition.
(2) the real-time monitoring to laser energy is realized, is conducive to improving the repeatability of detection technique.
(3) distance and laser energy of lens and object according to different samples, can be adjusted, optimal noise is obtained Than.
(4) sample stage limits enhanced line intensity by space, and energy plasma is laterally and row constraint is entered in longitudinal direction, carries High spectral line collection efficiency and the intensity of spectral line, are avoided that and excite particle to cover sample surfaces again, and smooth sample surfaces are (especially Such as fresh blade out-of-flatness sample), the distance of sample to condenser lens is kept constant repeated so as to improve detection.
Brief description of the drawings
Fig. 1 is the structure chart of multi-mode laser induced breakdown spectroscopy device;
Fig. 2 is the structure chart of sample stage;
Fig. 3 is the top view of sample stage in Fig. 2;
Fig. 4 is the schematic diagram that sample is impacted on sample stage;
Fig. 5 is unconfined plasma figure;
Fig. 6 is the constraints graph with constraint window and constraint chamber plasma.
Embodiment
As shown in figure 1, the multi-mode laser induced breakdown spectroscopy device in the present invention includes:Double-impulse solid laser 1, Delay time generator 2, energy attenuator 3, laser energy real-time monitoring system 4, light path is climbed system 5, ICCD detectors 6, light splitting System 7, the second condenser lens 8, sample stage 9, the first condenser lens 10, optical fiber collection system 11, sample surface imaging system 12.
Double-impulse solid laser 1 has 4 kinds of mode of operations:(1) 1064nm is coaxially exported, and (2) 532nm is coaxially exported, (3) the different axle outputs of 1064nm, the different axle outputs of (4) 1064nm, 532nm.Double-impulse solid laser 1 can be by 2 pulses 1064nm solid state lasers, frequency-doubling crystal and combined beam light road are realized.
The control Double-impulse solid laser 1 of delay time generator 2 adjusts Q triggered times, xenon lamp to open triggered time and ICCD spies Survey the gate duration of device 6.Delay time generator sets Double-impulse solid laser to adjust the triggered time of Q signal to be triggered in xenon lamp signal 150 ± 20 μ s afterwards, detector controls the opening time to be 1.5 μ s (detectors after the second road laser Q-switching switch triggering time The control opening time need to be optimized according to signal to noise ratio).
Variable energy attenuator 2 is made up of 1/2 wave plate 31 and the first beam splitter 32.Laser energy monitors reponse system in real time It is made up of the 41, second beam splitter 42 of thermoelectric pulse probe, USB connecting lines, computer 13.The laser to be monitored is by 3:7 points Shu Jing separates 30% laser energy, is popped one's head in and received by thermoelectric pulse, computer is connected to by USB connecting lines, special soft The energy of recording laser is shown on part in real time, for subsequent data analysis.
Light path system 5 of climbing is made up of the first speculum 52, the second speculum 51 and the 3rd speculum 53.First speculum 52nd, the second speculum 51 and the 3rd speculum 53 are from 1 inch of double frequency Nd:YAG laser mirrors, 532, the reflection at 1064nm Rate is more than 98%.
First condenser lens 10 and the second condenser lens 8 are installed on the Lens mounting carrier for having the free degree along optical axis direction In, for adjusting the distance of sample and lens, so as to control impact to the laser parameter on sample.
Optical fiber collection system 11 is made up of light collector and optical fiber.Sample surface imaging system 12 include CCD camera 124, Imaging lens 123, the 3rd beam splitter 122, LED light source for illuminating 121.
Beam splitting system 7 is echelle spectrometer.First condenser lens 10 and the second condenser lens 8 select N-BK7, plating V-arrangement film, its reflectivity at 532,1064nm is less than 0.25%.
As shown in Figure 2, Figure 3 and Figure 4, sample stage 9 includes gear rack elevating bar 901, gear slider 902, right angle pinboard 903, plasma confinement window 904, cylindrical guide 905, plasma confinement plate 906, V-type sliding block 907 combines electric displacement platform 909, pull bar 910 constrains chamber 911.Electric displacement platform 909 is combined using four-degree-of-freedom (x, y, z, w) combination electric displacement platform, including three lists The free degree (x, y and z) pulse electric displacement platform and rotary freedom (w) electric rotary table.Gear rack elevating bar 901 is pacified vertically On combination electric displacement platform 909, gear slider 902 is engaged with gear rack elevating bar 901, can vertically be moved up and down.Right angle Pinboard 903 is secured by bolts on gear slider 902, and plane is provided with the light-transmitting opening of rectangle, and light-transmitting opening edge is provided with support Light-passing board is provided with step, light-transmitting opening, plasma confinement window 904 is formed.Cylindrical guide 905 is fixed on combination electric displacement platform 909, plasma confinement plate 906 can be slided up and down along cylindrical guide 905.Cylindrical guide 905 and gear rack elevating bar 901 pass through Bolt-connection is on combination electric displacement platform 909.Combination electric displacement platform 909 is provided with V-groove, and V-type sliding block 907 can under the effect of pull bar 910 Horizontally slipped along V-groove, pull bar 910 is threadably secured in V-type sliding block 907.Sample 908 places V-type sliding block 907 (quite In objective table) on, laser is impacted down from above, by plasma confinement window 904, and passes through plasma confinement plate 906, sample surfaces are arrived in impact, excite plasma, and cooling sends characteristic spectral line and collected by optical fiber collection system 11.
The material of plasma confinement window 904 is N-BK7, and thickness is 1~5mm, and transmitance is more than 90%, energy threshold More than 10J/cm2.Plasma confinement window 904 is mainly used in plasma and longitudinally enters row constraint, and to incident laser with The characteristic spectral line that plasma is produced has preferable transmissivity.N-BK7 is a kind of common optical glass, can be passed through The light of 350nm~2000nm wave bands, the transmissivity of its laser is more than 90%, and energy threshold is more than 10J/cm2.Therefore plasma It is N-BK7 to constrain the selection of material of window 904, and thickness is 1~3m.Plasma confinement window 904 can be acted in gear slider 902 Under vertically move.Line enhancement effect suffers restraints window from the influence with a distance from sample.Due to properties of samples and The element spectral line intensity to be detected is different, and plasma confinement window 904 of the invention can be moved in vertical direction, root According to need adjust the intensity of spectral line.
In the present embodiment, the material of plasma confinement plate 906 is the aluminium sheet of chromium plating, and thickness is 1mm, and it is middle uniform Cone constraint chamber 911 is furnished with, upper conical surface diameter and lower conical surface diameter are 2mm and 3mm respectively.Distance should between constraining chamber 911 It is consistent with combining the planning displacement of electric displacement platform 909.The transverse direction that plasma restraining plate 6 is mainly used in plasma enters row constraint, And characteristic spectral line is carried out constraint propagation, spectral line collection efficiency and the intensity of spectral line are improved, the intensity of spectral line enhancing scope is 2~10 Times.Chromium plating is carried out in the constraint chamber 911 of aluminium sheet, makes inner chamber that there is higher reflectivity, makes characteristic spectral line constraint propagation, is improved Spectral line collection efficiency.Constraint chamber uses conical structure, and due to its up-small and down-big structure, the structure compared with cylindrical type can be more preferably Obtain plasma and enter row constraint.In addition, when plasma is projected from cone constraint chamber, because its space constraint is increased, Its electron density can be strengthened with movement velocity, therefore advantageously in the enhancing of spectral line signal.The plasma of the present invention Distance is consistent with combining the planning displacement of electric displacement platform 909 between the constraint chamber of body restraining plate 906, can be suitably used for laser-induced breakdown The working method of spectrum Surface scan.Using plasma restraining plate 906 of the present invention covers sample surfaces, is conducive to smooth sample table Detection repeatability is improved in face, while avoiding exciting the other regions to be measured of particle contamination.When testing sample is the surfaces such as fresh blade During out-of-flatness sample, its region to be measured has differences with lens distance, and then influences the laser parameter of laser arrival sample.Laser The detection stability and the laser parameter in region to be detected of induced breakdown spectroscopy are closely bound up, therefore smooth sample surfaces are conducive to Fixed laser parameter improves the repeatability of detection.In addition, the up-small and down-big conical structure of plasma confinement plate 906 is conducive to Farthest avoid exciting particle contamination by a upper detection zone, it is ensured that detect the element that object is region to be detected.
V-type sliding block 907 can be moved under the effect of pull bar 910 along V-groove, using this V-type sliding block guide track structure, it is to avoid rise The troublesome operation such as plasma confinement window mouthful and plasma restraining plate.Company between plasma confinement plate 906 and cylindrical guide 905 It is connected in be close to and connects, plasma confinement plate 906 can not freely glides under gravity.
So that LIBS system reheats mode of operation as an example, when this sample stage works, control combination electromigration Platform 909 makes the pyramid type constraint chamber 911 of plasma confinement plate 906 corresponding with the position of top laser, sets combination electromigration The work step-length of platform 909 is cone constraint chamber neighbor distance or multiple.Beam of laser B passes through light path system, and line focus is saturating Mirror is propagated down from above, through plasma confinement window 904, and by cone constraint chamber impact sample.Plasma Its laser transmittance for constraining window 904 is more than 90%, and energy threshold is more than 10J/cm2.Second beam laser A vertically leads to Over-focusing lens focus is impacted onto the plasma inspired, enhanced line signal.Plasma cooling sends characteristic spectral line C Collected by the optical fiber collection system 11 of top.The number of times that each position can be impacted according to needed for being selected actual requirement, when completion one After individual position multiple position spectra collections are carried out by combining the movement of electric displacement platform 909.As shown in Figure 5 and Figure 6, when without plasma When body constrains window 904 and plasma confinement plate 906, the plasma D inspired is free excited state;When to exciting After plasma D is limited, plasma D density increase, plasma temperature rise enhances the spectral line of excited atom Intensity.
Double-impulse solid laser 1 sends pulse laser, by the damping capacity of energy attenuator 3, by optical system, hits Get on sample, plasma is formed when energy density is higher than the threshold value excited, plasma cooling sends different wave length Characteristic spectral line, is collected via optical fiber collection system 11, by beam splitting system 7, is detected by ICCD detectors 6, and in computer 13 Upper display processing.The device can realize that 3 kinds of mode of operations and different operating wavelength are cut by adjusting output laser and light path Change.Conllinear (collinear) that tri- kinds of different mode of operations of dipulse LIBS refer to, pre-ablation (pre-ablative), again plus Hot (re-heating).
Mode of operation 1 (conllinear):The mode of operation of Double-impulse solid laser 1 is coaxial 532nm or coaxial 1064nm, electricity Brain control delay time generator 2 gives the modulating signal of Double-impulse solid laser 1 and adjusts Q signal, and Double-impulse solid laser 1 starts work Make.Laser sequentially passes through the first speculum 52 (532nm/1064nm) and second speculum 51 (532nm/1064nm) improving laser Light path;Adjusting the reflector mount of the second speculum 51 makes laser be located above sample, and light path is changed through the 3rd speculum 53, to It is lower to propagate.Laser focuses on sample surfaces via plating the first condenser lens of V film glass 10, when laser energy density is higher than what is excited During threshold value, sample produces plasma, and plasma cooling, atom occurs transition, produces the characteristic spectral line for characterizing element.Spectral line Collected, via beam splitting system 7 (echelle spectrometer) light splitting, converted by ICCD detectors 6 by optical fiber collection system 11 For electric signal, it is connected to by USB in computer 13, carries out data statistics and analysis in computer 13, determine certain in sample The content of material.
Mode of operation 2 (reheating):The mode of operation of Double-impulse solid laser 1 is different axle 532nm/1064nm, 1064nm Output, computer control delay time generator 2 awards the modulating signal of Double-impulse solid laser 1 and adjusts Q signal, Double-impulse solid laser 1 starts working.First laser (532nm/1064nm) sequentially passes through the first speculum 52 (532nm/1064nm) and the second reflection The light path of mirror 51 (532nm/1064nm) improving laser;Adjusting the reflector mount of the second speculum 51 makes laser be located on sample Side, changes light path through the 3rd speculum 53 (532nm/1064nm), propagates downwards.Laser is focused on via plating V film glass first Mirror 10 focuses on sample surfaces, and when laser energy density is higher than the threshold value excited, sample produces plasma.Control sample stage 9, Z-direction displacement height is adjusted, second laser (1064nm) light-emitting window is higher than 9061 ± 0.5mm of plasma confinement plate.The Dual-laser (1064nm) is focused on by the second condenser lens of plating V film glass plano-convex 8, focuses on the plasma signal ejected On, enhanced line signal.Spectral line is collected by optical fiber collection system 11, via beam splitting system 7 (echelle spectrometer) point Light, electric signal is converted into by ICCD detectors 6, is connected to by USB in computer 13, computer 13 carry out data statistics with Analysis, determines the content of the material of certain in sample.
Mode of operation 3 (pre-ablation):The mode of operation of Double-impulse solid laser 1 is different axle 532nm/1064nm, 1064nm Output, computer control delay time generator 2 awards the modulating signal of Double-impulse solid laser 1 and adjusts Q signal, Double-impulse solid laser 1 starts working.Sample stage 9 is controlled, Z-direction displacement height is adjusted, second laser (1064nm) light-emitting window is higher than plasma 9061 ± 0.5mm of restraining plate.Second laser (1064nm) is focused on by the second condenser lens of plating V film glass plano-convex 8, focuses on sample Top, can lead to inert gas.First laser (532nm/1064nm) sequentially pass through the first speculum 52 (532nm/1064nm) and The light path of second speculum 51 (532nm/1064nm) improving laser;Adjusting the reflector mount of the second speculum 51 is located at laser Above sample, change light path through the 3rd speculum 53 (532nm/1064nm), propagate downwards.Laser is via plating V film glass first Condenser lens 10 focuses on sample surfaces, and when laser energy density is higher than the threshold value excited, sample produces plasma.Spectral line Optical fiber collection system 11 is collected, and via beam splitting system 7 (echelle spectrometer) light splitting, electricity is converted into by ICCD detectors 6 Signal, is connected in computer 13 by USB, is carried out data statistics and analysis in computer 13, is determined the material of certain in sample Content.

Claims (8)

1. a kind of multi-mode laser induced breakdown spectroscopy device, it is characterised in that including Double-impulse solid laser, sample stage and For controlling Double-impulse solid laser to trigger the delay time generator of sequential;Double-impulse solid laser has 1064nm coaxially defeated Go out, 532nm is coaxially exported, the different axle outputs of 1064nm and the different axle of 1064nm, 532nm export four kinds of way of outputs;
Described multi-mode laser induced breakdown spectroscopy device has conllinear, reheating, three kinds of mode of operations of pre-ablation;
In described conllinear mode of operation:The light path of the Double-impulse solid laser is climbed system, the light path provided with light path System of climbing is used to raise the light path that 1064nm/532nm coaxially exports laser so that laser focuses on sample directly over sample stage Product surface, produces plasma;
In described reheating and pre-ablation mode of operation:The first laser of the Double-impulse solid laser enters described light Road is climbed system, and the light path is climbed the light path that system is used to raise first laser so that first laser is poly- directly over sample stage Jiao arrives sample surfaces, produces plasma;Described delay time generator control first laser and the triggering sequential of second laser;Institute The second laser for stating Double-impulse solid laser directly focuses to plasma;
Also include signal acquisition and processing system, the characteristic spectral line sent is cooled down according to plasma and first laser impacts sample The spatial information of obtained sampled point, distributed intelligence of the display elements in sample surfaces;
Described light path climb system by the first speculum, the second speculum and the 3rd speculum group into second speculum Positioned at the surface of the first speculum, the 3rd speculum is located at the surface of sample stage;Described the first speculum, the second reflection Mirror and the 3rd speculum are double frequency Nd:YAG laser mirrors;The focusing of the first laser and second laser is installed with lens On the Lens mounting carrier that can be slidably matched along optical axis direction;Focusing in the light path of the first laser plates V with lens surface Shape film, its reflectivity at 532nm, 1064nm is less than 0.25%.
2. multi-mode laser induced breakdown spectroscopy device as claimed in claim 1, it is characterised in that described dipulse solid Energy attenuator is there also is provided on the optical axis of laser and for detecting that the laser energy of recording laser energy is monitored in real time in real time System;
Described first laser is climbed system after laser energy real-time monitoring system outgoing into light path;
Described second laser focuses to plasma after laser energy real-time monitoring system outgoing.
3. multi-mode laser induced breakdown spectroscopy device as claimed in claim 1, it is characterised in that described signal acquisition and Processing system includes:
Optical fiber collection system, for collecting the characteristic spectral line that plasma cooling is sent;
Beam splitting system, for carrying out light splitting to characteristic spectral line;
ICCD detectors, for the optical signal of beam splitting system to be converted into electric signal;
Sample surface imaging system, for monitoring first laser impact sample position, obtains the spatial information of sampled point;
Computer, according to the spatial information of described electric signal and sampled point, distributed intelligence of the display elements in sample surfaces.
4. multi-mode laser induced breakdown spectroscopy device as claimed in claim 3, it is characterised in that described beam splitting system is Echelle spectrometer.
5. multi-mode laser induced breakdown spectroscopy device as claimed in claim 4, it is characterised in that described sample surface into As system includes:
For from surface to illumination sample LED light source for illuminating,
Beam splitter on LED light source for illuminating optical axis,
CCD camera and imaging lens, the sample surfaces image information for gathering beam splitter reflection.
6. multi-mode laser induced breakdown spectroscopy device as claimed in claim 1, it is characterised in that described delay time generator Double-impulse solid laser is controlled to adjust Q triggered times and xenon lamp to open the triggered time, delay time generator sets dipulse solid to swash The triggered time of light device tune Q signal 150 ± 20 μ s after the triggering of xenon lamp signal.
7. multi-mode laser induced breakdown spectroscopy device as claimed in claim 1, it is characterised in that described sample stage includes Electric displacement platform with four-degree-of-freedom, the lifter plate being movably arranged on electric displacement platform and the objective table being slidably fitted on electric displacement platform;
The lifter plate impacts sample after being provided with transparent constraint window, laser light constraint window;
The lower section of the lifter plate is provided with restraining plate, and the restraining plate is placed in distribution Constrained chamber on the surface of sample, restraining plate, The constraint chamber is used for the plasma for constraining sample excitation.
8. multi-mode laser induced breakdown spectroscopy device as claimed in claim 7, it is characterised in that set on described lifter plate There is light-transmitting opening, covered with light-passing board at the light-transmitting opening, the light-transmitting opening constitutes described constraint window with light-passing board.
CN201410653808.XA 2014-11-17 2014-11-17 A kind of multi-mode laser induced breakdown spectroscopy device Active CN104406942B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201410653808.XA CN104406942B (en) 2014-11-17 2014-11-17 A kind of multi-mode laser induced breakdown spectroscopy device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201410653808.XA CN104406942B (en) 2014-11-17 2014-11-17 A kind of multi-mode laser induced breakdown spectroscopy device

Publications (2)

Publication Number Publication Date
CN104406942A CN104406942A (en) 2015-03-11
CN104406942B true CN104406942B (en) 2017-07-21

Family

ID=52644589

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201410653808.XA Active CN104406942B (en) 2014-11-17 2014-11-17 A kind of multi-mode laser induced breakdown spectroscopy device

Country Status (1)

Country Link
CN (1) CN104406942B (en)

Families Citing this family (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP3510376B1 (en) * 2016-09-08 2024-02-14 FOSS Analytical A/S Method for performing laser induced breakdown spectroscopy
CN106841082B (en) * 2017-01-18 2019-09-10 上海朗研光电科技有限公司 Portable terahertz time-domain spectroscopy instrument
CN108344694A (en) * 2018-02-26 2018-07-31 长光禹辰信息技术与装备(青岛)有限公司 A kind of multispectral instrument of multi-mode multiplexing
CN108495246A (en) * 2018-04-28 2018-09-04 苏州静声泰环保科技有限公司 A kind of point sound source sound-producing device and vocal technique
CN109444111B (en) * 2018-12-10 2021-03-09 西安交通大学 Optical fiber LIBS detection system and method capable of selecting double-pulse mode
CN109521000B (en) * 2019-01-24 2023-08-08 中国工程物理研究院流体物理研究所 Grating beam-splitting type simultaneous multi-point laser-induced breakdown spectroscopy measurement system and method
CN113281257A (en) * 2021-06-02 2021-08-20 光谱时代(北京)科技有限公司 Laser-induced breakdown spectroscopy element analysis system
CN113916787B (en) * 2021-10-19 2023-05-26 西安电子科技大学 Multimode laser-induced breakdown spectroscopy device
CN114823406B (en) * 2022-03-31 2023-03-24 上海微崇半导体设备有限公司 Method and device for measuring semiconductor multilayer structure based on second harmonic

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8310671B1 (en) * 2010-09-29 2012-11-13 The United States Of America As Represented By The Administrator Of National Aeronautics And Space Administration Interference-free optical detection for Raman spectroscopy
CN102841078A (en) * 2012-09-10 2012-12-26 北京宝瑞光电科技有限公司 Integrated laser-induced enhanced plasma spectrum acquisition system
CN103529000A (en) * 2013-10-17 2014-01-22 中国科学院西安光学精密机械研究所 Single-light-source dual-wavelength LIBS (laser-induced breakdown spectroscopy) measurement device and method
CN203894165U (en) * 2014-06-09 2014-10-22 江西农业大学 Collinear double-pulse laser-induced breakdown spectroscopy (LIBS) technology-based device for rapidly detecting benzopyrene content in edible oil
CN104142316A (en) * 2014-08-15 2014-11-12 中国科学院上海技术物理研究所 Pre-ablation and reheating combined triple-pulse LIBS (laser-induced breakdown spectroscopy) detection system
CN204214778U (en) * 2014-11-17 2015-03-18 浙江大学 A kind of multi-mode laser induced breakdown spectroscopy device

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8319964B2 (en) * 2009-07-10 2012-11-27 University Of Florida Research Foundation, Inc. Method and apparatus to laser ablation—laser induced breakdown spectroscopy
US20120314214A1 (en) * 2011-06-07 2012-12-13 Alexander Dennis R Laser Induced Breakdown Spectroscopy Having Enhanced Signal-to-Noise Ratio

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8310671B1 (en) * 2010-09-29 2012-11-13 The United States Of America As Represented By The Administrator Of National Aeronautics And Space Administration Interference-free optical detection for Raman spectroscopy
CN102841078A (en) * 2012-09-10 2012-12-26 北京宝瑞光电科技有限公司 Integrated laser-induced enhanced plasma spectrum acquisition system
CN103529000A (en) * 2013-10-17 2014-01-22 中国科学院西安光学精密机械研究所 Single-light-source dual-wavelength LIBS (laser-induced breakdown spectroscopy) measurement device and method
CN203894165U (en) * 2014-06-09 2014-10-22 江西农业大学 Collinear double-pulse laser-induced breakdown spectroscopy (LIBS) technology-based device for rapidly detecting benzopyrene content in edible oil
CN104142316A (en) * 2014-08-15 2014-11-12 中国科学院上海技术物理研究所 Pre-ablation and reheating combined triple-pulse LIBS (laser-induced breakdown spectroscopy) detection system
CN204214778U (en) * 2014-11-17 2015-03-18 浙江大学 A kind of multi-mode laser induced breakdown spectroscopy device

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
Dual-Pulse LIBS Using a Pre-ablation Spark for Enhanced Ablation and Emission;DIMITRA N. STRATIS et al.;《APPLIED SPECTROSCOPY》;20001231;第54卷(第9期);1271 *

Also Published As

Publication number Publication date
CN104406942A (en) 2015-03-11

Similar Documents

Publication Publication Date Title
CN104406942B (en) A kind of multi-mode laser induced breakdown spectroscopy device
CN104374763B (en) Adjustable reheating double pulse laser-induced breakdown spectroscopy device
CN104374759B (en) A kind of atomic fluorescence spectrophotometry device based on laser ablation plume
CN104374752B (en) Rapid detection method for nutrient elements of crops based on collinear laser-induced breakdown spectroscopy
CN104374753B (en) Crop heavy metal based on double-pulse laser induced breakdown spectrum and method for detecting microelements
CN204214783U (en) One is adjustable heats double-pulse laser induced breakdown spectral device again
CN101782517B (en) Laser probe micro-area component analyzer based on double laser light source
US8309883B2 (en) Methods and systems for laser processing of materials
CN109444111B (en) Optical fiber LIBS detection system and method capable of selecting double-pulse mode
CN104374751B (en) Device based on conllinear LIBS crop nutrient quick detection
US11879780B2 (en) Coherent anti-Stokes Raman scattering microscope imaging apparatus
CN107783242B (en) Automatic focusing device and block LIBS online detection device adopting same
CN1839307A (en) Optical path difference compensation mechanism for acquiring time-series signal of time-series conversion pulse spectrometer
AU2019257598A1 (en) Multi-laser systems having modified beam profiles and methods of use thereof
CN108827911A (en) The micro- resonance laser induced breakdown spectroscopy detection method of one kind and system
CN209992396U (en) Microscopic imaging full-spectrum high-voltage module time-resolved fluorescence measurement system
CN204214778U (en) A kind of multi-mode laser induced breakdown spectroscopy device
CN204214779U (en) Based on the device that conllinear Laser-induced Breakdown Spectroscopy crop alimentary element detects fast
US7817270B2 (en) Nanosecond flash photolysis system
CN110955107A (en) Ultra-high-speed time resolution camera shooting device and method based on reflection imaging technology
CN110632038A (en) Light path time-delay double-pulse LIBS device
CN204214781U (en) A kind of atomic fluorescence spectrophotometry device based on laser ablation plume
CN104374698B (en) Sample table for laser-induced breakdown spectroscopy detection
CN104515754B (en) Laser plasma spectrometry device
CN208224086U (en) A kind of micro- resonance laser induced breakdown spectroscopy detection system

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant