[go: up one dir, main page]

CN109682795A - The method and device of thin film damage is differentiated based on the plasma ignition time - Google Patents

The method and device of thin film damage is differentiated based on the plasma ignition time Download PDF

Info

Publication number
CN109682795A
CN109682795A CN201811022571.XA CN201811022571A CN109682795A CN 109682795 A CN109682795 A CN 109682795A CN 201811022571 A CN201811022571 A CN 201811022571A CN 109682795 A CN109682795 A CN 109682795A
Authority
CN
China
Prior art keywords
plasma
film
signal
flash
air
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN201811022571.XA
Other languages
Chinese (zh)
Other versions
CN109682795B (en
Inventor
苏俊宏
汪桂霞
徐均琪
时凯
梁海锋
杨利红
吴慎将
万文博
李建超
黄钉劲
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.)
Xian Technological University
Original Assignee
Xian Technological University
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 Xian Technological University filed Critical Xian Technological University
Publication of CN109682795A publication Critical patent/CN109682795A/en
Application granted granted Critical
Publication of CN109682795B publication Critical patent/CN109682795B/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
    • G01N21/73Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light thermally excited using plasma burners or torches

Landscapes

  • Health & Medical Sciences (AREA)
  • Physics & Mathematics (AREA)
  • Chemical & Material Sciences (AREA)
  • Plasma & Fusion (AREA)
  • Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Engineering & Computer Science (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

本发明公开了一种基于等离子体点燃时间判别薄膜损伤的方法及装置。解决了等离子体闪光法对薄膜损伤识别的误判问题,技术方案是:用至少三个探测器分别获取空气和薄膜等离子体闪光信号及入射激光信号,以后者为基准,得到空气和薄膜等离子体闪光点燃时间,准确分辨出空气和薄膜等离子体闪光,消除误判。实现步骤是分别采集基准和闪光信号;获取基准和闪光信号起始时刻;以基准和闪光信号起始时刻之差作为闪光点燃时间;建模计算闪光点燃时间;比较并得出损伤识别判据。本发明建立的点燃时间计算模型,可针对任意单层薄膜;装置结构简单,测量精度达0.1ns,能准确进行薄膜损伤识别,可靠性好。本发明应用于强激光作用下的光学薄膜损伤判别。

The invention discloses a method and a device for judging damage of thin films based on plasma ignition time. The problem of misjudgment of thin film damage identification by the plasma flash method is solved, and the technical scheme is as follows: at least three detectors are used to obtain the air and thin film plasma flash signals and incident laser signals respectively, and the latter is used as the benchmark to obtain the air and thin film plasma. Flash ignition time, accurately distinguish air and thin-film plasma flashes, and eliminate misjudgment. The realization steps are to collect the reference and the flash signal respectively; obtain the starting time of the reference and the flash signal; take the difference between the reference and the starting time of the flash signal as the flash ignition time; model and calculate the flash ignition time; compare and obtain the damage identification criterion. The ignition time calculation model established by the invention can be aimed at any single-layer film; the device has a simple structure, the measurement accuracy reaches 0.1 ns, and the film damage can be accurately identified, and the reliability is good. The invention is applied to the damage judgment of optical thin films under the action of strong laser.

Description

The method and device of thin film damage is differentiated based on the plasma ignition time
Technical field
The invention belongs to technical field of optical test, relate generally to the fault localization of film, it is specifically a kind of based on it is equal from Daughter burning time differentiates the method and device of thin film damage, for the thin film damage identification under superlaser effect.
Background technique
The optical phenomena of film is just noticed early in the 17th century, after the 1930s, because of vacuum technique Development provide prerequisite to the preparation of various optical thin films, even to this day, optical thin film has been greatly developed, optics Seriation, sequencing and specialization are gradually moved towards in the production of film, and still, there are also many problems in the research of optical thin film Need further to be solved, the existing level of optical thin film is not met by requirement in many work, needs to improve.In theory On, not only the growth mechanism needs of film are got clear, and the optical theory of film, are especially applied to the optics reason of extremely short wave band By also needing to be further improved and improve.In technique, people also lack effective means realization to the essence of thin-film deposition parameter Really control, in this way, the growth of film just has a degree of randomness, the optical constant of film, the thickness of film and thin The performance of film also just has a degree of unstability and blindness, everything all limits the raising of optical thin film quality. For optical thin film itself, in addition to optical property needs to improve, absorb, scatter etc. except light loss need to reduce, its machine Tool intensity, chemical stability and physical property require to be further improved.In laser system, the anti-laser intensity of optical thin film Lower, this is one of sixty-four dollar question in optical thin film research.
The power of the anti-laser action ability of optical thin film commonly uses optical thin film laser damage threshold (LIDT) size to comment The LIDT of valence, optical thin film is bigger, and anti-laser action ability is stronger, and the measurement of laser damage in thin films threshold value (LIDT) with it is thin The judgement whether film damages, the two be it is inseparable, accurately to measure laser damage in thin films threshold value (LIDT), just must be accurate Ground judges whether film is damaged.Therefore, the anti-laser action ability of optical thin film is studied, it just must Study of Laser film Non-destructive tests.The method of differentiation thin film damage respectively has advantage and disadvantage at present: it is intuitive accurate that phasecontrast microscope method determines that damage has Advantage, but it is expensive, it is relatively time-consuming, it is unable to the damage results of given amounts value;He-Ne light intensity scattering method is to miscellaneous in film Matter, defect and working environment are very sensitive, and experimental error is relatively large.Photothermal deflection method is cleverer compared with phasecontrast microscope observation method It is quick, but to test environment it is more demanding, and test build it is more complex;Acousto-optic method measurement sensitivity with higher, still Noise is affected to its result, is easy to produce misjudgment phenomenon.Above-mentioned several method receives in laser film non-destructive tests The extensive concern of optics worker, and also carrying out constantly studying at present.They are detected with different principles respectively The damage from laser degree of film, has their own advantages, but also all have deficiency.So induced with laser thin film damage Study of recognition is one The element task that item needs to adhere to for a long time, only non-destructive tests are reliable, and the accuracy of the LIDT measured could improve.
Traditional plasma flicker method differentiates that the schematic illustration of thin film damage is as shown in Figure 1.Light laser is successively by declining It is focused near the film at detected sample sample platform after subtracting device, focusing system, beam splitter, if laser energy is more than the breakdown institute of film The energy threshold needed, will generate plasma spark, if there is flash of light, be glistened and by detecting element acquisition by flashing signal It is converted to electric signal and sends computer to, thus judge that film has damaged.In fact, laser in transmission process, works as incidence When laser energy density is more than threshold of air breakdown, air plasma flash of light, this air plasma flash of light can be also generated Film plasma spark will be interfered, cause detecting element can not the signal of resolved detection be air or film Plasma spark signal and thin film damage misjudgment phenomenon occurs.This misjudgment phenomenon most directly influence result be exactly cause it is thin The measurement inaccuracy of film laser damage threshold (LIDT), in turn, inaccurate LIDT value influences the anti-laser action energy of optical thin film The evaluation of power.Thin film damage identification is accurately carried out, accurate laser damage in thin films threshold value (LIDT) value is obtained, to optical thin film Anti- laser action ability is correctly evaluated, and this misjudgment phenomenon must be just eliminated.
Optical film technique is widely used in optics and photoelectron technical field, manufactures various optical instruments.Such as: it is high-precision Spend detector, the very high computer chip of integrated level, accurate weapon system etc..Because the thickness of optical thin film is mostly in nanometer To the micron order of magnitude, so the requirement of the links such as thin-film material, thin film preparation process and films test is all very high, for For films test link, sixty-four dollar question is exactly the anti-laser ability of testing film, with traditional plasma flicker method When identifying thin film damage, differed constantly as nanosecond order even more even if air and the plasma spark generated with film are lighted It is small, also it can come wrong judgement and calculated result to the calibration tape of the anti-laser ability of film, currently, either phasecontrast microscope Method, He-Ne light intensity scattering method, photothermal deflection method, acousto-optic method or traditional plasma flicker method, cannot all accurately identify air It glistens with the plasma of film, the indistinguishable of the plasma flash of light of air and film directly results in traditional plasma flash of light Method identifies the frequent erroneous judgement of thin film damage, influences the evaluation of the anti-laser action ability of optical thin film, therefore, conventional plasma therewith Body flicker method is not used widely.
Summary of the invention
Present invention aims in view of the above shortcomings of the prior art, propose one kind can accurately carry out thin film damage knowledge Other method and device that thin film damage is differentiated based on the plasma ignition time.
The present invention is a kind of method that thin film damage is differentiated based on the plasma ignition time, is comprised the following steps that
Step 1 is with different detector acquisition reference signals and flashing signal: being acquired respectively with different photodetectors Incident laser signal, air and film plasmon flashing signal, simultaneously the synchronous feeding signal receiving device of all acquisition signals Show respective signal waveform;
Step 2 obtains reference signal and flashing signal initial time: by signal receiving device incident laser signal, Air and film plasma spark signal data are handled, and using incident laser signal as benchmark signal, obtain incident laser Signal, air plasma flashing signal and the respective initial time of film plasma spark signal;
Step 3 is using reference signal and the difference of flashing signal initial time as plasma spark burning time: to enter The difference of the initial time of laser signal and air plasma flashing signal is penetrated as air plasma flash of light burning time;With The difference of the initial time of incident laser signal and film plasma spark signal is as film plasma spark burning time;
Step 4 modeling and calculating plasma flash of light burning time: lighting time modeling to air plasma flash of light, Utilize the electron density n during air breakdowneThe change rate formula of t obtains air plasma flash of light burning time at any time tb;Film plasma spark burning time is modeled, film plasma ignition time t is calculatedm
Step 5 judgement: comparison air plasmon flash of light burning time tbWith film plasmon flash of light burning time tm, work as tb=tmWhen, illustrate air and the flash of light of film plasmon while generating, this phenomenon occurrence probability very little;Work as tb≠tmWhen, Air and the flash of light of film plasmon do not generate simultaneously, can accurately differentiate;
Step 6 damage identification technique criterion: work as tb< tmWhen, air plasma flash of light is glistened prior to film plasma Occur, is to differentiate thin film damage signal with flashing signal below;Work as tb> tmWhen, film plasma spark prior to air etc. from Son flash of light occurs, and is to differentiate thin film damage signal with front flashing signal, is sent into computer with the thin film damage signal determined The non-destructive tests of film are participated in, more accurate thin film damage data are obtained.
The present invention or a kind of device that thin film damage is differentiated based on the plasma ignition time, are issued strong by laser Laser passes through optical filter, attenuator, and nearby induces film breakdown by the film that focusing system focuses on detected sample sample platform And plasma spark is generated, it is received and is glistened with detector, energy meter reads the reflected light energy of beam splitter in real time, and computer is Operating console, which is characterized in that the detector is at least three, and two of them are respectively placed on horizontal plane along laser emitting The bilateral symmetry position of direction flashing signal, left side are film plasma spark signal sensor, and right side is air plasma Body flashing signal detector, the setting of another incident laser signal sensor are visited in condenser lens side, incident laser signal Attenuator group, detector acquisition incident laser and plasma spark signal are equipped with before surveying device and are converted to electric signal, it is above Signal synchronous transfer obtained by detector is to signal receiving device.
The present invention differentiates misjudgment phenomenon existing for thin film damage for traditional plasma flicker method, in traditional plasma A kind of method and dress that thin film damage is differentiated based on the plasma ignition time is proposed on the basis of flicker method identification thin film damage It sets.
Compared with prior art, technical advantage of the invention:
1, when traditional plasma flicker method identification thin film damage, the reason of because of detecting element setting, easily air and The plasma spark that film generates is obscured and generates erroneous judgement, when light laser acts on film surface, air plasma flash of light It can be generated with film plasma spark, in existing thin film damage determination method, all be not carried out the differentiation to the two, The difference of the burning time of general air plasma flash of light and film plasma spark is nanosecond order, this is thin for high-precision It is that cannot be neglected for the damaging judge of film.Present invention utilizes different detectors, targetedly obtain air plasma Body flash of light and film plasma spark signal, by comparing the air plasma flash of light of nanosecond order and film plasma The burning time of flash of light has carried out accurate resolution to air plasma flash of light and film plasma spark, has made thin film damage It identifies more acurrate;
2, the present invention inhales during modeling and calculating air and film plasma spark burning time according to multi-photon The computation model that theory of electrolytic dissociation establishes air plasmon body burning time is received and cascaded, is only joined with the laser action of incident laser Number is related, and model is simple, and computational accuracy can calculate after air is breakdown under any laser action parameter role up to 0.001ns Air plasma glisten burning time;According to film when breakdown the interaction principle of film and laser establish film etc. The computation model of gas ions burning time, the present invention need not distinguish the material of film, thickness and preparation process, can be directed to any list The plasma spark burning time of layer film directly calculates, and computational accuracy is up to 0.001ns.
3, the present invention is based on the plasma ignition times to differentiate that the device of thin film damage is improved in conventional apparatus , induced with laser thin film damage identification device is improved, reliability, the accuracy of experimental result and data is ensure that, ensure that The accuracy of LIDT value.Synchronous transfer is to oscillograph after the signal of all photodetector acquisitions is converted to electric signal, with incidence Laser signal is benchmark signal, and air and film plasma spark signal initial time difference, respectively air and Film plasma spark burning time has carried out accurate resolution to air plasma flash of light and film plasma spark. Experimental provision structure of the present invention is simple, air ion body flash of light burning time and film plasma spark burning time measurement essence Degree is all up 0.1ns.
Detailed description of the invention
Fig. 1 is conventional apparatus schematic illustration;
Fig. 2 is the device of the invention schematic illustration;
Fig. 3 is the technology of the present invention route map;
Fig. 4 is that present invention damage differentiates flow diagram;
Fig. 5 is air plasma of the present invention flash of light burning time simulation calculation curve graph;
Fig. 6 is film plasma spark burning time simulation calculation curve graph of the present invention.
Specific embodiment
With reference to the accompanying drawings and examples to the detailed description of the invention.
Embodiment 1
Thin film technique is a Disciplinary Frontiers of modern science and technology research, is widely used in detected with high accuracy device, is integrated Spend very high computer chip, accurate weapon system etc..Such as in many of high energy strong laser system optical thin film element, For these optical thin film elements, surface deposit optical film is not required nothing more than to improve light transmission quality, and it is required to have Stronger anti-laser action ability.Therefore it needs to solve there are two realistic problem in this field: first is that how laser film is made It is standby;Second is that whether being damaged under light laser effect, how damage identifies, anti-laser action energy for the film of preparation How power is judged.And the anti-laser action ability of optical thin film is often evaluated with laser damage threshold (LIDT), it refers to optics The energy density of incoming laser beam when film generation Critical Damage.The LIDT of optical thin film is bigger, resisting laser damage ability Better.
It is exactly to cause the measurement of laser damage in thin films threshold value (LIDT) inaccurate that this misjudgment phenomenon, which most directly influences result, Really, inaccurate LIDT value directly affects optical film product and quality and application, and it is anti-sharp also to influence optical thin film certainly The evaluation of light action ability.
For this purpose, the present invention proposes a kind of side for differentiating thin film damage based on the plasma ignition time with innovation after study Method comprises the following steps that referring to fig. 4
Step 1 is with different detector acquisition reference signals and flashing signal: being acquired respectively with different photodetectors Incident laser signal, air and film plasmon flashing signal, simultaneously the synchronous feeding signal receiving device of all acquisition signals Show respective signal waveform;Using incident laser signal as benchmark signal, the air plasma flashing signal of acquisition and film etc. Gas ions flashing signal and reference signal are when the difference on start time is respectively that respective air plasma flash of light is lighted Between and film plasma spark burning time.
Because incident laser, air and the flash of light of film plasmon belong to the optical signal of different spectral bands, this hair It is bright to acquire incident laser signal, air and film plasmon flashing signal respectively using different photodetectors, all letters It is number synchronous to be sent into signal receiving device and show respective signal waveform.
Step 2 obtains reference signal and flashing signal initial time: by signal receiving device incident laser signal, Air and film plasma spark signal data are handled, and using incident laser signal as benchmark signal, obtain incident laser Signal, air plasma flashing signal and the respective initial time of film plasma spark signal.In this example, use Matlab software handles incident laser signal, air and film plasma spark signal data, by processing, respectively The initial time of reference signal, air plasma flashing signal and film plasma spark signal is obtained.
Step 3 is using reference signal and the difference of flashing signal initial time as plasma spark burning time: to enter The difference of the initial time of laser signal and air plasma flashing signal is penetrated as air plasma flash of light burning time;With The difference of the initial time of incident laser signal and film plasma spark signal is as film plasma spark burning time.
In other words, incident laser signal and difference of the air plasma flashing signal on start time are air etc. Gas ions flash of light burning time;Incident laser signal and difference of the film plasma spark signal on start time are film Plasma spark burning time.
Step 4 modeling and calculating plasma flash of light burning time: air plasma flash of light burning time is carried out Modeling, utilizes the electron density n during air breakdowneThe change rate formula of t obtains air plasma shining point at any time Fire time tb;Film plasma spark burning time is modeled, film plasma ignition time t is calculatedm
The present invention is during modeling and calculating air and film plasma spark burning time, according to Multiphoton Absorbtion Establish the computation model of air plasmon body burning time with cascade theory of electrolytic dissociation, only with the laser action parameter of incident laser Correlation, model is simple, and computational accuracy can calculate after air is breakdown under any laser action parameter role up to 0.001ns Air plasma flash of light burning time;According to film when breakdown the interaction principle of film and laser establish film etc. from The computation model of daughter burning time, the present invention need not distinguish the material of film, thickness and preparation process, can be directed to any single layer The plasma spark burning time of film directly calculates, and computational accuracy is up to 0.001ns.
Step 5 judgement: comparison air plasmon flash of light burning time tbWith film plasmon flash of light burning time tm, work as tb=tmWhen, illustrate air and the flash of light of film plasmon while generating, this phenomenon occurrence probability very little;Work as tb≠tmWhen, Air and the flash of light of film plasmon do not generate simultaneously, can accurately differentiate.
Step 6 damage identification technique criterion: work as tb< tmWhen, air plasma flash of light is glistened prior to film plasma Occur, is to differentiate thin film damage signal with flashing signal below;Work as tb> tmWhen, film plasma spark prior to air etc. from Son flash of light occurs, and is to differentiate thin film damage signal with front flashing signal, is sent into computer with the thin film damage signal determined The non-destructive tests of film are participated in, more accurate thin film damage data are obtained.
Referring to Fig. 3, technology path of the invention is to establish model when Irradiation of High optical thin film and calculate air etc. Gas ions flash of light burning time and film plasma spark burning time pass through the actual value of both experimental provision tests.It is right Theoretical calculation and experimental results are analyzed, and the technology criterion of thin film damage erroneous judgement is obtained.
The present invention different detector acquisition reference signals and flashing signal;Obtain reference signal and flashing signal starting Moment;Obtain plasma spark burning time;Model simultaneously calculating plasma flash of light burning time;Judgement;Non-destructive tests skill Art criterion completes the resolution of air and film plasma spark.
Embodiment 2
The method of thin film damage is differentiated with embodiment 1, to air etc. described in step 4 based on the plasma ignition time Time modeling is lighted in gas ions flash of light, specifically
In formula, neFor the electron density during air breakdown, t is time, τpFor laser pulse width, E is incident laser energy Amount, r are laser focal beam spot radius, and N is air molecule density, and k is the number of photons for ionizing an atom and needing while absorbing, σ For the photon absorption cross sections of atom step, h=6.626 × 10-34For Planck's constant.Q is air coefficient, vmFor momentum of electron Transfer collision frequency, c=3 × 108It (m/s) is the light velocity, λ is laser wavelength of incidence, and n=1.0003 is air refraction.
Theoretical foundation according to the present invention has: photonic absorption and cascade ionization when air is by laser breakdown.Multi-photon Absorption process refers to an atom while absorbing k photon, and the gross energy of these photons is not less than the ionization potential of the atom, thus Bring it about ionization.Electron avalanche or cascade ionization refer to that initiating electron obtains energy from the electric field of laser, when this energy is sufficiently large When, and if atomic collision, atom excitation can be made to be ionized, so continuous collision.
The present invention establishes the calculating mould of air plasmon body burning time according to Multiphoton Absorbtion and cascade theory of electrolytic dissociation Type, only related to the laser action parameter of incident laser, model is simple, can calculate air quilt under any laser action parameter role Air plasma flash of light burning time after breakdown.
Embodiment 3
Method based on plasma ignition time differentiation thin film damage is dodged with embodiment 1-2 by air plasma Luminous point combustion time model obtains electron density neThe curve of t variation at any time referring to Fig. 5, then chooses air quilt from the curve Puncture moment point, it is electron density n at the time of air breakdown that selection principle, which is in the air of normal temperature and pressure,eEqual to 1013cm-3 At the time of corresponding, air is breakdown at this time, and air plasma is ignited.
The present invention acts on the breakdown mechanism of lower air to light laser and is studied, according to Multiphoton Absorbtion and cascade electricity From the computation model that theory establishes air plasmon body burning time, computational accuracy is up to 0.001ns.
Embodiment 4
Method based on plasma ignition time differentiation thin film damage acquires incident laser signal with embodiment 1-3 Photodetector service band requires to be 800-1700nm;Acquire the photodetector operating wave of air plasmon flashing signal Duan Yaoqiu is 400-1100nm;The photodetector service band for acquiring film plasmon flashing signal requires to be 150- 550nm。
Embodiment 5:
For method based on plasma ignition time differentiation thin film damage with embodiment 1-4, the present invention provides one specifically The result of calculating:
N=2.7 × 10 are taken respectively in formula (1)19(cm-3), q=1021(cm-1s-1V-2), νm=3.9477 × 1013 (s-1), ν=1015(s-1), σ=10-16(cm-2), λ=1.064 × 10-6(m), τp=10-8(s), r=0.015 (cm).Normal In the air of normal temperature and pressure, air breakdown at the time of, can be defined as electron density equal to 1013cm-3At the time of corresponding, air at this time It is considered having punctured, air plasma has been ignited.If acting on light laser ENERGY E=82.4mJ, t is obtainedbCalculate knot Fruit is as shown in figure 5, tbFor 1.856ns.
Film plasma spark burning time is modeled described in step 4, specifically
In formula, e, m, E, w, υe、tpThe quantity of electric charge, electron mass, laser field field strength, laser angular frequency, electronics is respectively indicated to touch Hit frequency and pulsewidth;E=2P/ (c ε0), P, c, ε0Respectively indicate laser power density, the light velocity, dielectric constant;Nec、Ne、Ne0Point It is not the electron density of breakdown critical value, the electron density of t moment and initiating electron density, vLIndicate the ionization of atom or molecule Rate, ELFor vapor atomic or the ionization energy of molecule, then when film is breakdown, electron density N in steameCritical value must be reached NecIf by tmReach Nec, the plasma ignition time is tm
According to laser and material interaction principle, after strong laser irradiation to film surface, film surface a thin layer is first It is heated to gasifying by laser, which continues to absorb incident laser energy, and temperature continues to rise, and its electricity known to saha equation It is also improved from degree, plasma is formd when reaching a certain level.If from the increased process angle of electronics (ion) density Illustrate the generation of plasma, how many pairs of ionization process of a small amount of free electron, breakdown threshold, film etc. on film surface Gas ions flash of light burning time all has a great impact, referred to as initial free electrons.In the process that film surface gasification layer is formed In, initial free electrons absorb laser energy by reverse drag anticline process, and electron density will increase, and electrons are constantly inhaled Laser energy is received, continues ionization and goes down, reaches the gesture for forming snowslide afterwards to a certain degree, is i.e. film plasma spark is lighted.
It is the single layer Al of λ/4 with optical thickness2O3For film, if effect light laser wavelength X=1064nm, pulsewidth τp= 10ns, ENERGY E=82.4mJ, focal beam spot radius r=0.015cm can be obtained by formula (2), the point of film plasma spark Fire time tmFor 7.843ns, as shown in Figure 6.
The present invention according to film the interaction principle of film and laser establishes film plasma ignition when breakdown when Between computation model, it is not necessary to distinguish the material of film, thickness and preparation process, can for any single thin film plasma dodge Light burning time directly calculates, and computational accuracy is up to 0.001ns.
Embodiment 6
The present invention or a kind of device that thin film damage is differentiated based on the plasma ignition time, with it is above-mentioned based on it is equal from Based on daughter burning time differentiates the method for thin film damage, many devices for differentiating thin film damage can be designed or derive, Here the apparatus structure that thin film damage is differentiated based on the plasma ignition time is provided.
Existing traditional plasma flicker method differentiates that the schematic illustration of thin film damage is as shown in Figure 1.Nd:YAG laser The light laser that device issues nearby is induced after optical filter, attenuator by the film that focusing system focuses on detected sample sample platform It punctures and plasma spark occurs, and energy meter reads the reflected light energy of beam splitter in real time, and computer is operating console. Flashing signal, if there is flash of light, is converted to electric signal and sends meter to by unique detecting element for detecting flashing signal Calculation machine, thus judges whether film damages.
In fact, laser in transmission process, when incident laser fluence is more than threshold of air breakdown, can also generate Air plasma flash of light, will interfere film plasma spark, cause detecting element can not resolved detection Signal is the plasma spark signal of air or film and thin film damage misjudgment phenomenon occurs.
Referring to Fig. 3 the burning time of air and film plasma spark can be calculated separately and measured in order to eliminate erroneous judgement (tbAnd tm), the two is differentiated in time, keeps thin film damage identification more acurrate.In view of the above-mentioned problems, the present invention is specially set Count it is a kind of based on the plasma ignition time differentiate thin film damage device specifically included laser along laser emitting direction 1, optical filter 2, attenuator 3, focusing system 4, beam splitter 5, detected sample sample platform 7, energy meter 6 are connected with beam splitter 5, focusing system 4 are made of at least two condenser lenses, and detector 9 is located at the side rear of 4 first lens of focusing system, pacify in flash of light two sides Equipped with flash of light detector, all signals in 8 reception system of computer realize the control to whole device.
Detected sample is focused on after optical filter 2, attenuator 3, and by focusing system 4 by the light laser that laser 1 issues Film at sample platform 7 nearby induces film breakdown and generates plasma spark, and energy meter 6 reads the anti-of beam splitter 5 in real time Light energy is penetrated, computer 8 is operating console.Detector acquisition plasma spark signal is simultaneously converted to electric signal, referring to figure 2, detector of the invention is at least three, in this example, and detector is three, and two of them are respectively placed on horizontal plane along laser The bilateral symmetry position of exit direction flashing signal, left side are film plasma spark signal sensor 13, and right side is air Plasma spark signal sensor 10, another incident laser signal sensor 9 are arranged in first of focusing system thoroughly Mirror side rear is equipped with attenuator group before being along laser direction of travel on horizontal plane before incident laser signal sensor 9, visit Survey device 13 acquire film plasma spark signal, detector 10 acquire air plasma flashing signal, detector 9 acquire into Laser signal is penetrated, all signals of acquisition are converted to electric signal, and signal synchronous transfer to signal obtained by three above detector connects Receiving apparatus.Signal receiving device is oscillograph in this example, by all signal waveforms of 12 simultaneous display of oscillograph.The present invention utilizes three A high speed free space photodetector replaces a common photodetector in conventional apparatus, eliminates the mistake of conventional apparatus Sentence phenomenon, accurately identified whether film damages, provides guarantee to obtain accurate film LIDT value.
When traditional plasma flicker method identifies thin film damage, the reason of because of detecting element setting, easily air and thin The plasma spark that film generates is obscured and generates erroneous judgement, when light laser acts on film surface, air plasma flash of light meeting It is generated with film plasma spark, in existing thin film damage determination method, is all not carried out the differentiation to the two, one As air plasma flash of light and film plasma spark burning time difference be nanosecond order, this is for nanometer scale height It is that cannot be neglected for the damaging judge of precision film.Present invention utilizes different detectors, targetedly obtain air Plasma spark and film plasma spark signal, by comparing the air plasma flash of light of nanosecond order and film etc. The burning time of gas ions flash of light has carried out accurate resolution to air plasma flash of light and film plasma spark, has made thin Membrane damage identification is more acurrate.
Experimental provision structure of the present invention is simple, and science research input needed for the photodetector used is few, and measurement accuracy can Up to 0.1ns.The comprehensive sex expression of the present invention is that the integrated use of the professional relevant knowledge of more of light, mechanical, electrical and calculation etc., measurement skill The integrated use of art and control technology and the integrated use of hardware and software co-design.The present invention is free using three high speeds Space photodetector replaces a common photodetector in conventional apparatus, eliminates the misjudgment phenomenon of conventional apparatus, quasi- It really identifies whether film damages, provides guarantee to obtain accurate film LIDT value.
Embodiment 7
Differentiate the method and device of thin film damage with embodiment 1-6 based on the plasma ignition time.Photoelectricity of the invention Detector is at least three, this is most basic setting, as needed, can also add photodetector near flash of light, than Such as four or more, or to improve precision, or adjust because of the adjustment of incident light source.
The attenuator group added before incident laser signal sensor in this example, attenuator group are within 10% by transmitance. Attenuator group is combined by two optical filters and is constituted in this example, and the transmitance of the attenuator group of formation is 4%.Two optical filters it is saturating The rate of mistake is respectively 20% and 20%.
Because incident laser energy is very big, in order to which effective protection incident laser detector avoids it from being damaged by light laser, enter Attenuator group has been added before penetrating laser signal detector.
Embodiment 8
Differentiate the method and device of thin film damage with embodiment 1-7 based on the plasma ignition time.Acquire incident laser 9 service band of photodetector of signal requires to be 800-1700nm, and the rise time is less than 70ps;Air plasmon is acquired to dodge 10 service band of photodetector of optical signal requires to be 400-1100nm, and the rise time is less than 150ps;It is in vitro to acquire film etc. 13 service band of photodetector of sub- flashing signal requires to be 150-550nm, and the rise time is less than 5ns.The present invention is different Detector acquisition reference signal and flashing signal;Obtain reference signal and flashing signal initial time;Obtain plasma sudden strain of a muscle Light burning time, waveband selection is with strong points, and the rise time is able to satisfy signal acquisition requirement completely, ensure that measuring accuracy.
In this example attenuator group by transmitance be respectively 20% and 40% filter set at the transmitance of attenuator group is 8%.
Embodiment 9
Differentiate the method and device of thin film damage with embodiment 1-8 based on the plasma ignition time.In this example, letter is received The oscillograph that number device uses, oscillograph at least need triple channel, and sample rate is no less than 10G sample/s, and bandwidth is not less than 300MHz, storage depth are not less than 20M sample.As long as receiving signal device to be able to satisfy while receiving three road signals and show, Time interval between each sampled point is no more than 0.1ns, and the sampling precision of signal receiving device is higher, experiment test knot Fruit error is smaller, and precision is higher.
In this example attenuator group by transmitance be respectively 10% and 20% filter set at the transmitance of attenuator group is 2%.
Embodiment 10
Differentiate the method and device of thin film damage with embodiment 1-9 based on the plasma ignition time.Present invention connection is each The coaxial cable gauge size tolerance length of detector and signal receiving device must it is completely the same, in this example, use it is coaxial Cable is SMA male connector to BNC male connector, 48 inches, guarantees synchronous transfer.
The more specifical example for combining method and apparatus is given below, the present invention is further described.
Embodiment 11
Differentiate the method and device of thin film damage with embodiment 1-10 based on the plasma ignition time.
The present invention differentiates in traditional plasma flicker method to be improved on thin film damage device basic, the principle of the present invention Schematic diagram is as shown in Figure 2.The light laser that Nd:YAG laser 1 issues is gathered after optical filter 2, attenuator 3 by focusing system 4 Film of the coke at detected sample sample platform 7 nearby induces film and film surface air breakdown and plasma spark occurs, energy Meter 6 reads the reflected light energy of beam splitter 5 in real time, and computer 8 is operating console.Detector 9 is the height of THORLABS production Fast free space photodetector DET08CL/M, detector 10 are the high speed free space photodetector of THORLABS production DET025AL/M, detector 13 are the high speed free space photodetector DET25K/M of THORLABS production, they are adopted respectively Collection incident laser, air and film plasma spark signal are simultaneously converted to electric signal, and collected three road electric signal passes through The identical SMA coaxial cable of THORLABS production, the RT01014 four-way oscillography produced by Rohde & Schwarz Representative Office The output display of device 12, obtains the curve that signal voltage changes over time.Using Oringin software to incident laser signal, air It is handled with film plasma spark signal data, has respectively obtained incident laser signal, the air as reference signal The initial time of plasma spark signal and film plasma spark signal.Incident laser signal initial time is incident sharp At the time of light reaches focus, on the basis of incident laser signal, the air plasma flashing signal and incident laser of acquisition are believed Difference number on initial time is that air plasma glistens burning time tbMeasured value, film plasma spark signal with Difference of the incident laser signal on initial time is film plasma spark burning time tmMeasured value.It is inhaled in conjunction with multi-photon Receive and cascade the air plasma flash of light burning time t that theory of electrolytic dissociation Modeling Calculation obtainsbTheoretical value and laser and material The film plasma spark burning time t that interaction theory Modeling Calculation obtainsmTheoretical value, judgement of concluding:
First determine whether air plasma flash of light burning time tbWith film plasma spark burning time tmWhether phase Deng.Work as tb=tmWhen, illustrate air and the flash of light of film plasmon while generating, this phenomenon occurrence probability very little;Work as tb≠tm When, air and the flash of light of film plasmon do not generate simultaneously, can accurately distinguish.
Judge which works as t as thin film damage signal is differentiated in two flashing signals againb< tmWhen, air plasma Body flash of light is glistened prior to film plasma to be occurred, and the flashing signal generated after judgement is differentiation thin film damage signal;Work as tb> tm When, film plasma spark glistens prior to air plasma to be occurred, and is believed with the flashing signal first generated for differentiation thin film damage Number.The present invention obtains differentiating thin film damage signal, which is believed using the burning time of flashing signal as point of penetration Number feeding computer participates in the non-destructive tests of film, obtains accurate thin film damage data.
Since incident laser energy is very big, in order to protect detector 9, attenuator group 11 is placed before it, is decayed in this example Piece group at the transmitance of, attenuator group is 6% by the filter set that transmitance is respectively 20% and 30%.
Technical effect of the invention is explained again below by experiment and its result.
Embodiment 12
Differentiate the method and device of thin film damage with embodiment 1-11 based on the plasma ignition time.
In this example, the laser output wavelength of high power Nd:YAG solid state laser is 1064nm, and output energy is 5mJ- 235mJ is adjustable, and focal beam spot radius is 0.015cm, pulse width 10ns.Referring to fig. 2, the laboratory sample on sample stage 7 is light Learn the single layer Al with a thickness of λ/42O3Film (central wavelength 1064nm), base material are diameter of phi 30mm, the K9 of thickness 2mm Glass.In order to guarantee the stability of laser output energy, the input voltage of laser is remained unchanged in experiment.
Table 1 is that 10 groups of close incident laser energies act on lower air plasma flash of light burning time tbWith film plasma Body flash of light burning time tmExperimental data, in this example, oscillograph 12 obtains three tunnels acquisition signal with 1 μ s sampling time, respectively At the time of recording every road signal from scratch, i.e. CH1, CH2 and CH3, they respectively indicate incident laser signal, air and film At the beginning of plasma flashing signal, i.e. initial time, then air plasma glistens burning time tbIt is that CH2 and CH1 are poor Value, film plasma spark burning time tmFor CH3 and CH1 difference.Being obtained after 10 groups of experimental data average treatments, entering Penetrate laser action light laser energy be 82.4mJ when, air plasma glisten burning time tbAverage value is about 2.7ns, film Plasma spark burning time tmAverage value is about 7.8ns.Table 1 gives air plasma flash of light burning time tbWith it is thin Film plasma spark burning time tmExperimental data.
1 t of tablebAnd tmExperimental data
Result verification
The air plasma flash of light burning time t being calculated respectively with theoretical modelingbWith film plasma spark Burning time tmTheoretical value, and the air plasma flash of light burning time t of experiment testbIt is lighted with film plasma spark Time tmMeasured value, list can obtain the relationship of the two, as shown in table 2.
2 theoretical calculation of table and experiment test tbAnd tmCompare
As shown in Table 2, no matter theoretical calculation or test is tested, t can be obtainedb< tmConclusion, and theoretical calculation and reality The result that test tries meets preferably, illustrates to act on single layer Al when light laser2O3When film surface, air plasma dodges Light occurs prior to film plasma spark, has clearly differentiated air and film plasma spark moment in time, determines The flashing signal generated afterwards is to differentiate thin film damage signal, which is sent into the damage that computer participates in film Wound identification, obtains accurate thin film damage data, and this invention removes differentiating thin film damage with traditional plasma flicker method When caused by judge by accident.
The present invention can obtain high-precision flash of light burning time, moreover it is possible to distinguish to flash of light burning time.The present invention couple Light laser acts on the breakdown mechanism of lower air and is studied, and establishes air according to Multiphoton Absorbtion and cascade theory of electrolytic dissociation The computation model of plasmon body burning time, computational accuracy is up to 0.001ns.According to film film and laser when breakdown Interaction principle establishes the computation model of film plasma ignition time, it is not necessary to distinguish the material of film, thickness and preparation Technique can directly be calculated for the plasma spark burning time of any single thin film, and computational accuracy is also up to 0.001ns. The present invention also demonstrates the feasibility of calculation method with experimental provision, has told air in time and film plasma dodges Light burning time, the measurement accuracy of burning time is up to 0.1ns.For in the case where light laser acts on optical thin film whether damage How wound, damage identify this realistic problem, improve the uncertainty of measurement LIDT according to the technical solution of the present invention, obtain A kind of method and device that thin film damage is differentiated based on plasma ignition time that can accurately identify thin film damage.It is theoretical Thin film damage identification can accurately be carried out by demonstrating the present invention with experiment, and computation model is simple, and computational accuracy is high, experimental provision Structure is simple, and air and film plasma spark burning time measurement accuracy are high, good reliability.
In brief, the method and device disclosed by the invention that thin film damage is differentiated based on the plasma ignition time.Its Technical solution is: with different detector acquisition reference signals and flashing signal;When obtaining reference signal and flashing signal starting It carves;Obtain plasma spark burning time;Model simultaneously calculating plasma flash of light burning time;Judgement;Damage identification technique Criterion completes the resolution of air and film plasma spark, works as tb< tmWhen, air plasma flash of light prior to film etc. from Son flash of light occurs, and is to differentiate thin film damage signal with flashing signal below;Work as tb> tmWhen, film plasma spark is prior to sky The flash of light of gas plasma occurs, and is to differentiate thin film damage signal with front flashing signal.The present invention is obtained using at least three detectors Take air and film plasma spark signal and incident laser signal, on the basis of the latter, obtain air and film etc. from Daughter flash of light burning time, air and film plasma spark are told with this in time, obtain differentiating thin film damage Signal obtains a kind of side that thin film damage is differentiated based on the plasma ignition time to eliminate the misjudgment phenomenon of original device Method and device.The invention proposes a kind of method and device that thin film damage is differentiated based on the plasma ignition time, its masters Want advantage to have: establishing the computation model of air and film plasma spark burning time, can calculate any single thin film etc. Gas ions flash of light burning time;Experimental provision structure is simple, and measurement accuracy is up to 0.1ns.Thin film damage knowledge can accurately be carried out Not.Present invention is mainly applied to the damage differentiations of the optical thin film under light laser effect.

Claims (5)

1.一种基于等离子体点燃时间判别薄膜损伤的方法,其特征在于,包括有如下步骤:1. a method for discriminating film damage based on plasma ignition time, is characterized in that, comprises the steps: 步骤一 用不同的探测器采集基准信号和闪光信号:用不同光电探测器分别采集入射激光信号、空气和薄膜等离体子闪光信号,把所有采集信号同步送入信号接收装置并显示各自信号波形;Step 1: Use different detectors to collect the reference signal and flash signal: use different photodetectors to collect the incident laser signal, air and thin-film plasma flash signals respectively, send all the collected signals to the signal receiving device synchronously and display their respective signal waveforms ; 步骤二 获取基准信号和闪光信号起始时刻:将信号接收装置中的入射激光信号、空气和薄膜等离子体闪光信号数据进行处理,以入射激光信号为基准信号,获取入射激光信号、空气等离子体闪光信号各自的起始时刻;Step 2: Obtain the reference signal and the starting time of the flash signal: process the incident laser signal, air and thin-film plasma flash signal data in the signal receiving device, take the incident laser signal as the reference signal, and obtain the incident laser signal, air plasma flash the respective start times of the signals; 步骤三 以基准信号和闪光信号起始时刻之差作为等离子体闪光点燃时间:以入射激光信号与空气等离子体闪光信号的起始时刻之差作为空气等离子体闪光点燃时间;以入射激光信号与薄膜等离子体闪光信号的起始时刻之差作为薄膜等离子体闪光点燃时间;In step 3, the difference between the starting time of the reference signal and the flash signal is used as the ignition time of the plasma flash; The difference between the initial times of the plasma flash signal is taken as the ignition time of the thin-film plasma flash; 步骤四 建模并计算等离子体闪光点燃时间:对空气等离子体闪光点燃时间建模,利用空气击穿过程中的电子密度ne随时间t的变化率公式得到空气等离子体闪光点燃时间tb;对薄膜等离子体闪光点燃时间建模,计算得到薄膜等离子体点燃时间tmStep 4: Modeling and calculating the plasma flash ignition time: Model the air plasma flash ignition time, and obtain the air plasma flash ignition time t b by using the formula of the rate of change of the electron density ne during the air breakdown process with time t; Model the flash ignition time of the thin film plasma, and calculate the thin film plasma ignition time t m ; 步骤五 判断:对比空气等离体子闪光点燃时间tb和薄膜等离体子闪光点燃时间tm,当tb=tm时,说明空气和薄膜等离体子闪光同时产生,此现象发生几率很小;当tb≠tm时,空气和薄膜等离体子闪光未同时产生,可准确分辨;Step 5: Judgment: Compare the air plasma flash ignition time t b with the thin-film plasma flash ignition time t m , when t b = t m , it means that the air and thin-film plasma flashes are generated at the same time, and this phenomenon occurs The probability is very small; when t b ≠ t m , the air and thin-film plasmon flashes are not generated at the same time, and can be accurately distinguished; 步骤六 损伤识别技术判据:当tb<tm时,空气等离子体闪光先于薄膜等离子闪光发生,以后面闪光信号为判别薄膜损伤信号;当tb>tm时,薄膜等离子体闪光先于空气等离子闪光发生,以前面闪光信号为判别薄膜损伤信号,以判别出的薄膜损伤信号送入计算机参与薄膜的损伤识别,获得更加准确的薄膜损伤数据。Step 6 Criterion of damage identification technology: when t b < t m , the air plasma flash occurs before the thin film plasma flash, and the subsequent flash signal is used as the signal for judging the damage of the thin film; when t b > t m , the thin film plasma flash occurs first. When the air plasma flash occurs, the previous flash signal is used as the film damage signal, and the film damage signal is sent to the computer to participate in the film damage identification, so as to obtain more accurate film damage data. 2.如权利要求1所述的基于等离子体点燃时间判别薄膜损伤的方法,其特征在于:步骤四所述的对空气等离子体闪光点燃时间建模,具体是:2. the method for judging film damage based on plasma ignition time as claimed in claim 1, is characterized in that: the modeling of air plasma flash ignition time described in step 4 is specifically: 式中,ne为空气击穿过程中的电子密度,t为时间,τp为激光脉宽,E为入射激光能量,r为激光聚焦光斑半径,N为空气分子密度,k为电离一个原子需要同时吸收的光子数,σ为原子阶跃的光子吸收截面,h=6.626×10-34为普朗克常数,q为空气系数,vm为电子动量转移碰撞频率,c=3×108(m/s)是光速,λ为入射激光波长,n=1.0003为空气折射率。In the formula, ne is the electron density during air breakdown, t is the time, τ p is the laser pulse width, E is the incident laser energy, r is the laser focus spot radius, N is the air molecular density, and k is the ionized atom. The number of photons to be absorbed at the same time, σ is the photon absorption cross section of the atomic step, h=6.626×10 -34 is Planck's constant, q is the air coefficient, v m is the electron momentum transfer collision frequency, c=3×10 8 (m/s) is the speed of light, λ is the incident laser wavelength, and n=1.0003 is the refractive index of air. 3.如权利要求2所述的基于等离子体点燃时间判别薄膜损伤的方法,其特征在于:通过空气等离子体闪光点燃时间模型得到电子密度ne随时间t变化的曲线,再从该曲线中选取空气被击穿时刻点,选取原则为在常温常压的空气中,空气击穿的时刻为电子密度ne等于1013cm-3对应的时刻。3. the method for discriminating film damage based on plasma ignition time as claimed in claim 2, it is characterized in that: obtain the curve that electron density ne changes with time t by air plasma flash ignition time model, select from this curve again The selection principle of the time point of air breakdown is that in the air at normal temperature and pressure, the time point of air breakdown is the time corresponding to the electron density ne equal to 10 13 cm -3 . 4.一种基于等离子体点燃时间判别薄膜损伤的装置,由激光器发出的强激光经过滤光片、衰减器,并由聚焦系统聚焦于被测样品台处的薄膜附近诱导薄膜被击穿而产生等离子体闪光,用探测器接收闪光,能量计实时读取分束器的反射光能量,计算机为操作控制台,其特征在于,所述探测器至少为三个,其中两个分别置于水平面上沿激光出射方向闪光信号的左右对称位置,左侧为薄膜等离子体闪光信号探测器,右侧为空气等离子体闪光信号探测器,另外一个入射激光信号探测器设置在聚焦系统的第一个透镜侧后方,入射激光信号探测器前加设有衰减片组,探测器采集入射激光和等离子体闪光信号并转换为电信号,以上探测器所得信号同步传输至信号接收装置。4. A device for judging film damage based on plasma ignition time. The strong laser emitted by the laser passes through the filter, the attenuator, and is focused by the focusing system to the vicinity of the film at the sample stage to be tested to induce the film to be broken down. Plasma flash, the detector receives the flash, the energy meter reads the reflected light energy of the beam splitter in real time, the computer is the operation console, and it is characterized in that there are at least three detectors, two of which are placed on the horizontal plane respectively The left and right symmetrical positions of the flash signal along the laser output direction, the left side is the thin-film plasma flash signal detector, the right side is the air plasma flash signal detector, and the other incident laser signal detector is set on the first lens side of the focusing system At the rear, an attenuation plate group is installed in front of the incident laser signal detector. The detector collects the incident laser and plasma flash signals and converts them into electrical signals. The signals obtained by the above detectors are synchronously transmitted to the signal receiving device. 5.根据权利要求4所述的基于等离子体点燃时间判别薄膜损伤的装置,其特征在于,所述入射激光信号探测器前加设的衰减片组,衰减片组由透过率为10%以内。5 . The device for judging film damage based on plasma ignition time according to claim 4 , wherein the attenuating sheet set added before the incident laser signal detector has a transmittance within 10% of the attenuating sheet set. 6 . .
CN201811022571.XA 2018-05-14 2018-09-03 Method for identifying film damage based on plasma ignition time Active CN109682795B (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
CN201810457637 2018-05-14
CN2018104576371 2018-05-14

Publications (2)

Publication Number Publication Date
CN109682795A true CN109682795A (en) 2019-04-26
CN109682795B CN109682795B (en) 2023-09-22

Family

ID=66184487

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201811022571.XA Active CN109682795B (en) 2018-05-14 2018-09-03 Method for identifying film damage based on plasma ignition time

Country Status (1)

Country Link
CN (1) CN109682795B (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110542684A (en) * 2019-08-06 2019-12-06 中国科学院上海光学精密机械研究所 Optical thin film laser damage threshold testing system and method thereof
CN110618143A (en) * 2019-10-25 2019-12-27 中国工程物理研究院上海激光等离子体研究所 Method and system for testing laser damage threshold of wavelength separation film defect
CN114689564A (en) * 2022-03-29 2022-07-01 上海建冶科技股份有限公司 Laser derusting state detection method
CN116818285A (en) * 2023-06-30 2023-09-29 西安工业大学 Method and device for determining duration of air plasma flash
CN116839870A (en) * 2023-06-30 2023-10-03 西安工业大学 Method and device for determining flash duration of film plasma

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101718712A (en) * 2009-12-02 2010-06-02 西安工业大学 Combined testing device and testing method of laser damage thresholds of film and optical element
CN104764747A (en) * 2015-03-05 2015-07-08 江苏大学 A method of determining whether a matrix is damaged or not on line
CN106768889A (en) * 2016-12-19 2017-05-31 中北大学 Optical thin film laser damage threshold test device and method under a kind of vacuum environment
CN208902611U (en) * 2018-05-14 2019-05-24 西安工业大学 A device for discriminating film damage based on plasma ignition time

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101718712A (en) * 2009-12-02 2010-06-02 西安工业大学 Combined testing device and testing method of laser damage thresholds of film and optical element
CN104764747A (en) * 2015-03-05 2015-07-08 江苏大学 A method of determining whether a matrix is damaged or not on line
CN106768889A (en) * 2016-12-19 2017-05-31 中北大学 Optical thin film laser damage threshold test device and method under a kind of vacuum environment
CN208902611U (en) * 2018-05-14 2019-05-24 西安工业大学 A device for discriminating film damage based on plasma ignition time

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
C G MORGAN: "Laser-induced breakdown of gases", REPORTS ON PROGRESS IN PHYSICS, vol. 38, no. 5 *
汪桂霞: "激光诱导薄膜等离子体点燃时间及其影响因素", 《光学学报》, vol. 37, no. 4 *

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110542684A (en) * 2019-08-06 2019-12-06 中国科学院上海光学精密机械研究所 Optical thin film laser damage threshold testing system and method thereof
CN110542684B (en) * 2019-08-06 2022-03-08 中国科学院上海光学精密机械研究所 Optical film laser damage threshold testing system and method
CN110618143A (en) * 2019-10-25 2019-12-27 中国工程物理研究院上海激光等离子体研究所 Method and system for testing laser damage threshold of wavelength separation film defect
CN110618143B (en) * 2019-10-25 2022-05-31 中国工程物理研究院上海激光等离子体研究所 Method and system for testing laser damage threshold of wavelength separation film defect
CN114689564A (en) * 2022-03-29 2022-07-01 上海建冶科技股份有限公司 Laser derusting state detection method
CN116818285A (en) * 2023-06-30 2023-09-29 西安工业大学 Method and device for determining duration of air plasma flash
CN116839870A (en) * 2023-06-30 2023-10-03 西安工业大学 Method and device for determining flash duration of film plasma
CN116818285B (en) * 2023-06-30 2024-04-26 西安工业大学 Method and device for determining duration of air plasma flash
CN116839870B (en) * 2023-06-30 2024-04-26 西安工业大学 Method and device for determining flash duration of film plasma

Also Published As

Publication number Publication date
CN109682795B (en) 2023-09-22

Similar Documents

Publication Publication Date Title
CN109682795A (en) The method and device of thin film damage is differentiated based on the plasma ignition time
CN103175808B (en) Laser-induced breakdown spectroscopy analysis system and method
Rothe et al. Applications of tunable dye lasers to air pollution detection: measurements of atmospheric NO 2 concentrations by differential absorption
CN1316262C (en) Detection method and laser radar of Raman-Mie scattering laser atmospheric signal
CN103983619B (en) A kind of spatial discrimination Laser-induced Breakdown Spectroscopy analytic system and analytical approach thereof
CN103630908B (en) Laser frequency spectrum Measurement and calibration method in molecular scattering anemometry laser radar
CN104034703B (en) The LIBS material composition detection system of the low detection limit of high s/n ratio improved and method
CN102608613B (en) Device and method for accurately calibrating point object detectivity of laser radar
CN109186958A (en) A kind of coaxial laser damage threshold test device of more light and implementation method
CN103954593A (en) Plasma signal acquisition device based on laser-induced-breakdown spectroscopy
CN105891144A (en) Terahertz scanning system and method
CN105115862A (en) Cloud particle detection method and cloud particle detector
CN101196471A (en) Quantitative detection system and detection method of soil heavy metal pollution
CN107144421B (en) Point source transmittance stray light test system and method based on time resolution
CN103308187A (en) High-frequency Shack-Hartmann wave-front measuring device and measuring method thereof
CN110296975A (en) Energetic material macroparameter quickly detects spectroscopic system
CN101122555A (en) High concentration super fine granule measuring device and method based on backward photon related spectrum
CN103149158A (en) Double-prism water quality monitoring optical fiber sensing system
CN103308208B (en) The fast diagnosis method of transient temperature and device in a kind of plasma space field
CN111158011B (en) Pulse laser spot comprehensive test system and spot test method
CN106483531B (en) Atmosphere Raman-Rayleigh scattering thermometric laser radar and inversion method
CN201145663Y (en) High concentration ultrafine grain measuring apparatus based on rear photon correlation spectrum
CN208076382U (en) Water body multi-wavelength optical attenuation coefficient measuring device
CN208902611U (en) A device for discriminating film damage based on plasma ignition time
CN203414408U (en) Laser-induced breakdown spectroscopy analysis system

Legal Events

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