CN103268064B - Analog calculation method of ablating silicon nitride by ultrashort pulse laser - Google Patents

Analog calculation method of ablating silicon nitride by ultrashort pulse laser Download PDF

Info

Publication number
CN103268064B
CN103268064B CN201310086318.1A CN201310086318A CN103268064B CN 103268064 B CN103268064 B CN 103268064B CN 201310086318 A CN201310086318 A CN 201310086318A CN 103268064 B CN103268064 B CN 103268064B
Authority
CN
China
Prior art keywords
ablation
silicon nitride
model
residual altitude
pulse laser
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
CN201310086318.1A
Other languages
Chinese (zh)
Other versions
CN103268064A (en
Inventor
吴东江
姚龙元
马广义
牛方勇
郭东明
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.)
Dalian University of Technology
Original Assignee
Dalian University of Technology
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 Dalian University of Technology filed Critical Dalian University of Technology
Priority to CN201310086318.1A priority Critical patent/CN103268064B/en
Publication of CN103268064A publication Critical patent/CN103268064A/en
Application granted granted Critical
Publication of CN103268064B publication Critical patent/CN103268064B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Laser Beam Processing (AREA)

Abstract

The invention discloses an analog calculation method of ablating silicon nitride by ultrashort pulse laser, and Matlab is utilized to perform analog calculation and analysis on processing parameters. The analog calculation method mainly comprises the following steps that an ablating model of ablating silicon nitride by ultrashort pulse laser is established, and calculating parameters are initialized; boundary conditions of the plasma density are defined, and an ablating threshold, depth and volume with different analog parameters are calculated through the model; and on the basis of calculation results and a residual height model, the laser ablated residual height is analyzed and evaluated, and guiding parameters are given. By using the analog calculation method, the process of obtaining the processing parameters by repeated experiment can be avoided, analog results can be utilized to optimize the processing parameters, thereby shortening the product cycle, reducing the processing cost and increasing the production efficiency, and therefore, the analog calculation method has an important guiding value for the actual manufacturing process of ablating silicon nitride by ultrashort pulse laser.

Description

A kind of simulation method of mechanism of ultrashort-pulse laser ablation silicon nitride
Technical field
The invention belongs to ultra-short pulse laser Micrometer-Nanometer Processing Technology field, particularly a kind of simulation method of mechanism of ultrashort-pulse laser ablation silicon nitride.
Background technology
Along with the high speed development of advanced manufacturing technology and industrial level, the research of silicon nitride material is also received much concern.Because silicon nitride material has high chemical stability, high-heat resistance shock resistant, high rigidity, high temperature resistant, radiation hardness, the characteristic such as corrosion-resistant, thermohardening good, excellent optical performance.Therefore be widely applied in industries such as photoelectron, machinery, atomic energy, Aero-Space, and be widely used in the accurate and ultraprecise fields such as microelectronics along with it, microfabrication is carried out to it and seems particularly important.But silicon nitride belongs to high hard easy crisp material, existing processing method is difficult to carry out Precision Machining to it, therefore will realize then becoming key issue urgently to be resolved hurrily to its controlled fine removal.
Ultra-short pulse laser Micrometer-Nanometer Processing Technology a kind ofly utilizes that femtosecond laser is ultrafast, superpower, unique machining feature of superelevation, cause local microexplosion by producing the plasma of HTHP in very short time, thus realize the micro pipes method of material being carried out to accurately removal.Little owing to having the zone of action when femtosecond laser and matter interaction, without fuel factor, machining accuracy is high, can break through the unique advantages such as diffraction limit, therefore makes Precision Machining silicon nitride become possibility.This not only overcomes the difficulty in the process that its high rigidity characteristic brings, and provides a kind of precision machining method of high hard easy crisp material, thus improves crudy.But because removal precision when femtosecond laser carries out ablation to silicon nitride is wayward, and find optimal procedure parameters separately through repetition test and seem very loaded down with trivial details, working (machining) efficiency also can not get ensureing simultaneously, therefore just in the urgent need to a kind of method that can facilitate precision of prediction and don't lose working (machining) efficiency.Based on this, the present invention proposes a kind of simulation method of mechanism of ultrashort-pulse laser ablation silicon nitride, the evaluation of analog computation result when its key is then foundation and the different parameters of ablating model.About theoretical model and the correlation modeling method of mechanism of ultrashort-pulse laser ablation dielectric substance, all there is report with Publication about Document:
American scholar: M.D.Perry, B.C.Stuart, P.S.Banks, et al.Ultrashort-pulse laser machining of dielectric materials [J] .J Appl Phys, 1999,85 (9): 6803-6810.
France scholar: L.Sudrie, A.Couairon, M.Franco, et al.Femtosecond laser-induced damage and filamentary propagation in fused silica [J] .Phys Rev Lett, 2002,89 (18): 186601.
American scholar: C.H.Fan, J.Sun, J.P.Longtin.Plasma absorption of femtosecond laser pulses in dielectrics [J] .J Heat Transfer, 2002,124 (2): 275-283.
Chinese scholar: Liu Qing, Cheng Guanghua, Wang Yishan etc. the three-dimensional mangement of femtosecond pulse in transparent material and mechanism [J] thereof. photon journal, 2003,32 (3): 276-279.
Chinese scholar: Li Xiaoxi, Jia Tianqing, Feng Donghai etc. ablative mechanism and ultra-fast dynamics research [J] thereof of lower lithium fluoride are irradiated in ultrashort pulse. Acta Optica, 2005,25 (11): 1526-1530.
Analyzed by literature survey, Chinese scholars is when studying induced by ultrashort pulse laser dielectric substance, propose a lot of theoretical model describing avalanche ionization process and photoionization process, and the critical plasma density that conduction band free electron density Evolution and material occur when damaging is described.But these study the discussion that mostly lays particular emphasis on single model and single factors, rarelyr carry out systematically multi-model integrated analysis; And the controling parameters that seldom can relate to the research of ablation threshold and ablation depth in material removal process, lays particular emphasis on experimental analysis to the research of ablation volume then more comprehensively.Domestic scholars research is in this regard mainly for the discussion of interaction mechanism, and carried out lot of experiments, theoretical modeling remains defect, and research object is then in the majority with materials such as quartz glass, analyzes relatively little to the analog computation of silicon nitride material.Due to the weak point of its important application background and at present sunykatuib analysis, therefore find a kind of can the mechanism of accurate characterization ultra-short pulse laser and material, can remove technique to reality again provides the method for guide parameters to seem particularly important.
Summary of the invention
For solving in mechanism of ultrashort-pulse laser ablation silicon nitride process, the present invention removes that the wayward and technological parameter of precision is more difficult the problem such as to determine, for overcoming the deficiency of existing simulation method, study the independent role of unitary variant and the acting in conjunction rule of multiple variable respectively when calculating, its key is:
When 1, pretreatment being carried out to avalanche ionization coefficient and photoionization coefficient, first should determine the relation of ionization rate and electric-field intensity, then determine the relation of itself and energy density, so that follow-up ablation threshold analog computation.
2, laser pulse dimensional energy distribution Gaussian function is described, and Gaussian beam can break through processing diffraction limit, thus improves machining accuracy.
3, accurately should control condition when conduction band electron density reaches critical density, ensure that material calculates ablation depth, volume and residual altitude under the prerequisite that damage occurs.
The object of the present invention is to provide a kind of simulation method of mechanism of ultrashort-pulse laser ablation silicon nitride, not only can realize the optimization of control to ablation precision and technological parameter, and the blindness avoiding repetition test to bring, cut down finished cost, enhance productivity.
For achieving the above object, the present invention adopts following technical scheme:
A, the ablation threshold setting up mechanism of ultrashort-pulse laser ablation silicon nitride, the degree of depth and ablation volume-based model, and parameter initialization is carried out to model constants; Define plasma density boundary condition ρ during silicon nitride generation ablation in institute's established model simultaneously crbe 1.6 × 10 21cm -3, and pretreatment is carried out to the avalanche ionization coefficient of silicon nitride, photoionization coefficient and conduction band free electron density;
B, determine optical maser wavelength, setting pulsewidth computer capacity is 10fs ~ 10ps, calculates silicon nitride ablation threshold.When conduction band electron density exceedes critical plasma density, i.e. ρ c(x, t) > ρ crtime, silicon nitride produces damage, works as ρ c(x, t)≤ρ crtime, assignment must be carried out again to initializaing variable and calculate;
C, setting laser energy density codomain are 1J/cm 2~ 8J/cm 2, based on threshold value result, ablation depth is simulated; Under the modeling volume assumed condition that single pulse ablation pattern is cone shape, and define laser beam waist radius, and then the ablation volume under utilizing ablation depth analog result to obtain corresponding conditions; Described volume-based model is
V = x · πω 0 2 6 ln ( F F th )
In formula: V is ablation volume, x is ablation depth, ω 0for waist radius, F thfor ablation threshold, F is energy density;
D, set up the relational model of sweep speed v, line overlap rate δ and residual altitude Δ x, definition ablation residual altitude boundary condition, and threshold value and depth model result of calculation are loaded in residual altitude model; The relational model of described sweep speed v and residual altitude Δ x is
v = ΔL ( f - 1 ) = ξD ( f - 1 ) = Δx x × 100 % · D ( f - 1 )
In formula: Δ L is two pulse distances on sweep speed direction, and ξ is relative residual altitude, and D is ablation diameter, and f is pulse frequency, and x is ablation depth; Δ x is residual altitude, refers to the distance between ablation profile summit line and profile valley line; The relational model of described line overlap rate δ and residual altitude Δ x is
δ = ( d - Δd ) d × 100 % = ( 1 - ξ ) × 100 %
In formula: Δ d is ablation distance between centers of tracks, Δ d=ξ d; D is ablation line width, d=D;
E, paired pulses frequency carry out assignment, and are 4.0J/cm in energy density 2~ 8.0J/cm 2, sweep speed is calculate residual altitude under 0 ~ 3mm/s condition.If Δ x > Δ x max, do not meet the demands, variable should be re-entered and calculate, if Δ x≤Δ x max, meet machining accuracy, export guide parameters, complete analog computation.
Described avalanche ionization coefficient is:
η ( E ) = v s · α ( E ) = v s eE Δ exp ( - E i E ( 1 + E E P ) + E kT )
In formula: v sfor saturation drift velocity, α (E) is Townsend coefficient, and e is electron charge, and Δ is energy gap.E i, E pand E kTthat carrier overcomes electric-field intensity needed for ionization, optical phonon and thermal scattering effect respectively.
Described photoionization coefficient is:
In formula: ω is laser frequency, m=m em h/ (m e+ m h) be the reduction effective mass of electron hole pair, me, m hbe respectively the effective mass in electronics and hole; N=< Δ/(h ω)+1> represents the number of photons exciting an electron institute to absorb from valence band to conduction band; U=Δ-e 2e 2/ (4m ω 2), Φ (z) is Dawson integration.
Described ablation threshold model is:
&rho; cr ( 0 , &tau; ) = &rho; a 0 [ W th + H th &rho; c 0 ] exp [ ( 2 W th &rho; a 0 + H th ) &tau; ] - W th ( &rho; a 0 - 2 &rho; c 0 ) 2 W th + H th &rho; c 0 exp [ ( 2 W th &rho; a 0 + H th ) &tau; ] + H th ( &rho; a 0 - 2 &rho; c 0 )
In formula: ρ a0, ρ c0be respectively initial valence band, conduction band electron density, ρ crfor critical electron density.H th=η (F th); W th=w pI(F th), F thfor ablation threshold, τ is pulse width.
Described ablation depth model is:
In formula: x is ablation depth, h is Planck's constant; N=(< ε >+ Δ)/h ω, < ε > is averaged electron energy in plasma, W f=[F/F th] nw pI(F th), H f=[F/F th] 1/2η (F th).
Described conduction band free electron density equation is:
&PartialD; &rho; c ( x , t ) &PartialD; t = ( &PartialD; &rho; c ( x , t ) &PartialD; t ) AI + ( &PartialD; &rho; c ( x , t ) &PartialD; t ) PI - ( &PartialD; &rho; c ( x , t ) &PartialD; t ) Los .
In formula: AI item and the conduction band electron variable density that PI item represents avalanche ionization respectively, photoionization causes, Los. item represents the loss of carrier.
Described avalanche ionization coefficient and photoionization coefficient pretreatment refer to the relation by light intensity and electric-field intensity, energy density, finally set up function between ionization coefficient and energy density and to its computational analysis; The pretreatment of conduction band free electron density refers to and utilizes it to characterize equation, and the space-time expression form in conjunction with laser is done to derive further, and carries out analog computation by the parameter such as initial conduction band, valence-band electrons density of silicon nitride.
The pass of described light intensity and electric-field intensity, energy density is:
I = n 0 E 2 2 R 0 = F &tau;
In formula: R 0=c μ 0for vacuum impedance, c is vacuum light speed, μ 0for space permeability, n 0for medium refraction index.
Compared with prior art, the present invention has following beneficial effect:
1, the simulation method adopted in the present invention is compared with the scheme in the past reported, take into full account electron ionization mode when ultra-short pulse laser and silicon nitride interact and electron density Evolution, the removal mechanisms at work of material in ablation process can have been reflected more truly;
2, the simulation method adopted in the present invention is compared with the scheme in the past reported, each machined parameters is determined convenient and is convenient in actual production realize, revise with after analog result comparison, technological parameter database can be listed in, to subsequent technique optimization, there is important guiding and be worth;
3, the simulation method adopted in the present invention, compared with the scheme in the past reported, can be applied in a flexible way in the product of processing different accuracy, size, reduce while designing and developing cost and turn improve efficiency, be easier to ensure crudy.
Accompanying drawing explanation
The present invention has 6, accompanying drawing, wherein:
Fig. 1 is a kind of simulation method flow chart of mechanism of ultrashort-pulse laser ablation silicon nitride;
Fig. 2 is the Changing Pattern of silicon nitride ablation threshold with pulse width;
Fig. 3 is the Changing Pattern of silicon nitride ablation depth with energy density;
Fig. 4 is the Changing Pattern of silicon nitride ablation volume with energy density;
Fig. 5 (a), (b) are that sweep speed and line overlap rate affect schematic diagram to residual altitude respectively;
Fig. 6 is the Changing Pattern of residual altitude with sweep speed, energy density and pulse width.
Detailed description of the invention
Below in conjunction with accompanying drawing 1-6 and embodiment, the present invention is further described: as shown in Figure 1, a kind of simulation method flow chart of mechanism of ultrashort-pulse laser ablation silicon nitride, embodiments of the invention require: under optical maser wavelength is 780nm condition, obtain by analog computation the technological parameter being used to guide actual processing.Mainly comprising pulsewidth is damage threshold under 10fs ~ 10ps condition; Energy density is 1J/cm 2~ 8J/cm 2, ablation depth when pulsewidth is 12fs, 35fs, 220fs and volume and sweep speed are 0 ~ 3mm/s, and energy density is 4.0J/cm 2~ 8.0J/cm 2time residual altitude.Physical simulation calculation procedure is as follows:
A, the ablation threshold setting up mechanism of ultrashort-pulse laser ablation silicon nitride, the degree of depth and ablation volume-based model, and parameter initialization is carried out to model constants.By Matlab software, in electric field strength E=0 ~ 350MV/cm, during energy gap Δ=5.0eV, can be calculated Townsend coefficient; Another by free electron saturation drift velocity v s=2 × 10 7cm/s, vacuum impedance R 0=376.991 Ω, refractive index n0=2.0, can calculate the relation of avalanche ionization speed and energy density; For silicon nitride material, from valence band to conduction band, excite the number of photons n=4 that an electron institute will absorb, and then at electron hole pair reduction effective mass m=0.86m e=7.833 × 10 -31during kg, analog computation goes out photoionization speed.
B, utilize conduction band free electron density EVOLUTION EQUATION ρ c(x, t) is described the electron density in silicon nitride ablation process, wherein: initial valence-band electrons density p a0=1.10 × 10 23cm -3, initial conduction band electron density p c0=10 10cm -3, critical electron density ρ cr=1.6 × 10 21cm -3.Work as ρ c(x, t) > ρ crtime, meet ablation threshold condition, and then under pulsewidth is 10fs ~ 10ps condition, calculate the short pulse ablation threshold value of silicon nitride, result as shown in Figure 2, wherein during τ > 10ps, is long pulse ablation threshold.
C, based on threshold value analog result, obtain damage threshold when pulsewidth is 12fs, 35fs and 220fs, be respectively 2.0J/cm 2, 1.8J/cm 2and 1.4J/cm 2; Setting energy density codomain is 1J/cm 2~ 8J/cm 2, and calculating ablation depth, result is as shown in Figure 3.And then at waist radius ω 0when=30 μm, ablation volume when analyzing distinct pulse widths by volume-based model, as shown in Figure 4; The ablation depth curve utilizing Fig. 3 to obtain, can select the energy density parameter adopted during ablation different depth.
D, set up the relational model of sweep speed v, line overlap rate δ and residual altitude Δ x respectively, modeling schematic diagram is as shown in Fig. 5 (a), (b); Meanwhile, definition ablation residual altitude boundary condition, and the ablation depth result that the ablation threshold result obtained by Fig. 2 and Fig. 3 obtain is loaded in residual altitude model.
E, setting pulse frequency are 1kHz, and energy density is 4.0J/cm 2~ 8.0J/cm 2, sweep speed is 0 ~ 3mm/s, and utilize sweep speed model to carry out analog computation analysis to residual altitude, result as shown in Figure 6.According to residual altitude requirement, can determine to add the technological parameters such as sweep speed, energy density and the pulsewidth adopted man-hour, if Δ x > Δ x max, do not meet the demands, variable should be re-entered and calculate, if Δ x≤Δ x max, meet machining accuracy, export guide parameters, complete analog computation.
Above-described embodiment is the unrestricted method scheme of the present invention in order to explanation only, and any being equal to according to technical scheme of the present invention and inventive concept thereof replaces or change, and all should be encompassed within protection scope of the present invention.

Claims (1)

1. a simulation method for mechanism of ultrashort-pulse laser ablation silicon nitride, is characterized in that the method comprises the following steps:
A, set up the ablating model of mechanism of ultrashort-pulse laser ablation silicon nitride, and parameter initialization is carried out to model constants, define plasma density boundary condition ρ during silicon nitride generation ablation in institute's established model simultaneously crbe 1.6 × 10 21cm -3;
B, determine optical maser wavelength, setting pulsewidth computer capacity is 10fs ~ 10ps, calculates silicon nitride ablation threshold; When conduction band electron density exceedes critical plasma density, i.e. ρ c(x, t) > ρ crtime, silicon nitride produces damage, works as ρ c(x, t)≤ρ crtime, assignment must be carried out again to initializaing variable and calculate;
C, setting laser energy density codomain are 1J/cm 2~ 8J/cm 2, based on threshold value result, ablation depth is simulated; Under the modeling volume assumed condition that single pulse ablation pattern is cone shape, set up ablation volume-based model, and define laser beam waist radius, and then the ablation volume under utilizing ablation depth analog result to obtain corresponding conditions; Described volume-based model is
V = x &CenterDot; &pi; &omega; 0 2 6 ln ( F F th )
In formula: V is ablation volume, x is ablation depth, ω 0for waist radius, F thfor ablation threshold, F is energy density;
D, set up the relational model of sweep speed v, line overlap rate δ and residual altitude Δ x, definition ablation residual altitude boundary condition, and threshold value and depth model result of calculation are loaded in residual altitude model; The relational model of described sweep speed v and residual altitude Δ x is
v = &Delta;L ( f - 1 ) = &xi;D ( f - 1 ) = &Delta;x x &times; 100 % &CenterDot; D ( f - 1 )
In formula: Δ L is two pulse distances on sweep speed direction, and ξ is relative residual altitude, and D is ablation diameter, and f is pulse frequency, and x is ablation depth; Δ x is residual altitude, refers to the distance between ablation profile summit line and profile valley line; The relational model of described line overlap rate δ and residual altitude Δ x is
&delta; = ( d - &Delta;d ) d &times; 100 % = ( 1 - &xi; ) &times; 100 %
In formula: Δ d is ablation distance between centers of tracks, Δ d=ξ d; D is ablation line width, and ξ is relative residual altitude, d=D;
E, paired pulses frequency carry out assignment, and are 4.0J/cm in energy density 2~ 8.0J/cm 2, sweep speed is calculate residual altitude under 0 ~ 3mm/s condition; If Δ x > Δ x max, do not meet the demands, re-enter variable and calculate; If Δ x≤Δ x max, meet machining accuracy, export guide parameters, complete analog computation.
CN201310086318.1A 2013-03-18 2013-03-18 Analog calculation method of ablating silicon nitride by ultrashort pulse laser Active CN103268064B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201310086318.1A CN103268064B (en) 2013-03-18 2013-03-18 Analog calculation method of ablating silicon nitride by ultrashort pulse laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201310086318.1A CN103268064B (en) 2013-03-18 2013-03-18 Analog calculation method of ablating silicon nitride by ultrashort pulse laser

Publications (2)

Publication Number Publication Date
CN103268064A CN103268064A (en) 2013-08-28
CN103268064B true CN103268064B (en) 2015-04-29

Family

ID=49011700

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201310086318.1A Active CN103268064B (en) 2013-03-18 2013-03-18 Analog calculation method of ablating silicon nitride by ultrashort pulse laser

Country Status (1)

Country Link
CN (1) CN103268064B (en)

Families Citing this family (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104308368B (en) * 2014-09-03 2015-12-30 大连理工大学 The quantitative minimizing technology of multi-shot laser ablation metal coating
CN104764747B (en) * 2015-03-05 2017-06-27 江苏大学 Judge the method whether matrix damages online
CN108994453B (en) * 2018-10-11 2019-08-23 燕山大学 Ultra-short pulse laser working process parameter self-adaptation control method in numerical control processing
CN109948288B (en) * 2019-04-01 2020-08-25 大连理工大学 Nanosecond laser ablation micro-groove section profile prediction method
CN110125553B (en) * 2019-05-28 2020-10-30 中国人民解放军国防科技大学 Transient laser ablation simulation method for metal material
CN115620847B (en) * 2022-12-06 2023-03-28 中国空气动力研究与发展中心计算空气动力研究所 Method for determining ablation morphology of silicon-based composite material and related device

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1448755A (en) * 2003-05-09 2003-10-15 中国科学院上海光学精密机械研究所 Method for preparing periodic microstructure on metal film by femtosecond laser
CN1845812A (en) * 2003-07-31 2006-10-11 康宁股份有限公司 A method of making at least one hole in a transparent body and devices made by this method
JP2008114250A (en) * 2006-11-02 2008-05-22 Semiconductor Energy Lab Co Ltd Laser beam machining method and laser beam machining apparatus
CN101311358A (en) * 2008-03-28 2008-11-26 西安交通大学 Process for preparing zinc oxide nanometer wire array by femtosecond laser and device thereof
EP2075082A1 (en) * 2006-09-22 2009-07-01 Osaka University Substance joining method, substance joining device, joined body, and its manufacturing method

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7919764B2 (en) * 2008-05-06 2011-04-05 The United States Of America As Represented By The Secretary Of The Army Method and apparatus for enhanced terahertz radiation from high stacking fault density

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1448755A (en) * 2003-05-09 2003-10-15 中国科学院上海光学精密机械研究所 Method for preparing periodic microstructure on metal film by femtosecond laser
CN1845812A (en) * 2003-07-31 2006-10-11 康宁股份有限公司 A method of making at least one hole in a transparent body and devices made by this method
EP2075082A1 (en) * 2006-09-22 2009-07-01 Osaka University Substance joining method, substance joining device, joined body, and its manufacturing method
JP2008114250A (en) * 2006-11-02 2008-05-22 Semiconductor Energy Lab Co Ltd Laser beam machining method and laser beam machining apparatus
CN101311358A (en) * 2008-03-28 2008-11-26 西安交通大学 Process for preparing zinc oxide nanometer wire array by femtosecond laser and device thereof

Also Published As

Publication number Publication date
CN103268064A (en) 2013-08-28

Similar Documents

Publication Publication Date Title
CN103268064B (en) Analog calculation method of ablating silicon nitride by ultrashort pulse laser
Sun et al. Numerical analysis of laser ablation and damage in glass with multiple picosecond laser pulses
Zhai et al. Influence of surface morphology on processing of C/SiC composites via femtosecond laser
Malhotra et al. Laser-induced plasma micro-machining (LIPMM) for enhanced productivity and flexibility in laser-based micro-machining processes
Tangwarodomnukun et al. An investigation of hybrid laser–waterjet ablation of silicon substrates
Li et al. Modeling of waterjet guided laser grooving of silicon
CN104308368B (en) The quantitative minimizing technology of multi-shot laser ablation metal coating
CN104297925B (en) A kind of folding realizing femtosecond laser Diode laser spreads out the method for designing of hybrid element
CN105081564A (en) Processing method and device for inner hole of tempered glass
CN103394807A (en) Method and device for improving metal cladding deposition additive manufacturing accuracy by means of laser edge cutting
Wang et al. Simulation of femtosecond laser ablation sapphire based on free electron density
CN105468873A (en) Silicon substrate optical waveguide laser surface smoothing simulation method
Eppelt et al. Diagnostic and simulation of ps-laser glass cutting
CN105522281B (en) A kind of laser ablation processing method of quartz crystal
Yang et al. Numerical simulation and experimental research on reduction of taper and HAZ during laser drilling using moving focal point
Bao et al. Experiment and simulation study of laser dicing silicon with water-jet
Vaghasiya et al. Thermal and non-thermal ablation mechanisms in crystalline silicon by femtosecond laser pulses: Classical approach of the carrier density two temperature model
Liao et al. An analytical model to predict the sizes of modified layer in glass with femtosecond Bessel beam
Liao et al. Shape regulation of tapered microchannels in silica glass ablated by femtosecond laser with theoretical modeling and machine learning
Sun et al. Laser ablation mechanism of transparent dielectrics with picosecond laser pulses
Saetang et al. Laser scribing of fluorine-doped tin oxide coated on glass substrate in air and water
Yang et al. Model development for nanosecond laser-induced damage caused by manufacturing-induced defects on potassium dihydrogen phosphate crystals
Wang et al. A prediction model for ablation fluence threshold in femtosecond laser processing of fused silica
Heltzel et al. Nanostructuring borosilicate glass with near-field enhanced energy using a femtosecond laser pulse
Motomura Micro drilling simulation of ultra-short pulsed laser ablation of glass

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant