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The physical mechanisms of The physical mechanisms of short-pulse laser ablationshort-pulse laser ablation
D. Von der Linde, K. Sokolowski-D. Von der Linde, K. Sokolowski-TintenTinten
A summary report by Ryan A summary report by Ryan NewsonNewson
June 25, 2004June 25, 2004
Laser AblationLaser Ablation
Important for materials processingImportant for materials processing Many permutations of beam parameters; Many permutations of beam parameters;
many materialsmany materials Ultrashort pulses (fs-ps) interact Ultrashort pulses (fs-ps) interact
fundamentally different than longer pulsesfundamentally different than longer pulses
Importance in Our Machining Importance in Our Machining ExperimentExperiment
This discussion This discussion about one about one ultrashort pulseultrashort pulse
Our experiment Our experiment deals with a train of deals with a train of ultrashort pulsesultrashort pulses
Important to extend Important to extend this knowledge to this knowledge to our regimeour regime
Experiment SetupExperiment Setup
Pump pulse Pump pulse angled so that angled so that “sweeping” action “sweeping” action can be recordedcan be recorded
Probe pulse (weak Probe pulse (weak w/ orthogonal w/ orthogonal polarization) polarization) provides time-provides time-resolved resolved measurementsmeasurements
Breakdown Threshold & PlasmaBreakdown Threshold & Plasma
Previous experiments Previous experiments noticed there existed a noticed there existed a threshold “breakdown” threshold “breakdown” intensity of each materialintensity of each material
Measured with similar Measured with similar setup, looking at setup, looking at reflectivity change of reflectivity change of plasmaplasma
Ablation experiment Ablation experiment made sure breakdown made sure breakdown not not reached (no plasma)reached (no plasma)
[6] D. von der Linde, H. Schuler, J. Opt. Soc. Am. B 13 (1996) 216
Physical ProcessesPhysical Processes
1.1. Laser hits atoms – deposits energy to Laser hits atoms – deposits energy to electronic states of valence & conduction electronic states of valence & conduction bandsbands
2.2. Energy state distribution – relaxation time tEnergy state distribution – relaxation time tRR
3.3. Energy transported macroscopicallyEnergy transported macroscopically4.4. Displacement of atoms – ablation time tDisplacement of atoms – ablation time tAA
Thermal processes dominant when tThermal processes dominant when tAA >> t >> tRR
MaterialsMaterials
Shown in detail is silicon, but many metals Shown in detail is silicon, but many metals and semiconductors usedand semiconductors used
All show same results (to follow)All show same results (to follow) Hence results apply to our experiment, Hence results apply to our experiment,
where aluminum is primarily usedwhere aluminum is primarily used
Time-Resolved ResultsTime-Resolved Results
liquid metallic Siliquid metallic Si
start of ring start of ring structurestructure
surfacesurface
resolidificationresolidification
boundary of boundary of ablated areaablated area
amorphous Siamorphous Si
Ring PatternRing Pattern
Where does it Where does it occur?occur? Used Used
interference interference microscopy microscopy (bottom)(bottom)
Occurs only on Occurs only on ablation areaablation area
Ring Pattern cont.Ring Pattern cont.
Physical structure Physical structure or optical or optical interference?interference? Varied probe pulse Varied probe pulse
wavelengthswavelengths Ring spacing Ring spacing
wavelengthwavelength Must be Must be
interference – interference – Newton ringsNewton rings
HypothesisHypothesis
Gas-filled bubble Gas-filled bubble forming in molten forming in molten materialmaterial
Some problems… Some problems… (not supposed to (not supposed to be possible)be possible)
Unsteady Isentropic ExpansionUnsteady Isentropic Expansion
laser excitation &laser excitation &
thermalizationthermalization
isentropic isentropic expansionsexpansions
hybrid gas-liquid hybrid gas-liquid statestate
Ablation LayerAblation Layer
Speed of sound Speed of sound drastically lower in drastically lower in hybrid phasehybrid phase
Two steep density Two steep density boundaries developboundaries develop
Forms a kind of Forms a kind of “gas bubble” “gas bubble” hypothesizedhypothesized
Optical PropertiesOptical Properties
Inhomogeneous phase Inhomogeneous phase in ablation layer in ablation layer difficult to modeldifficult to model
Can approximate with Can approximate with Maxwell-Garnett Maxwell-Garnett modelmodel(right)(right)
Calculate n=2 for Si… Calculate n=2 for Si… high enough to explain high enough to explain ringsrings
Summary & Application to UsSummary & Application to Us
Ultrafast pulses ablate material in the Ultrafast pulses ablate material in the fashion outlined in this paperfashion outlined in this paper
Ultrafast pulses eject surface material in Ultrafast pulses eject surface material in volatile and sometimes unpredictable volatile and sometimes unpredictable statesstates
If the incident intensity is high enough, If the incident intensity is high enough, a plasma can forma plasma can form
If another pulse hit the material If another pulse hit the material immediately after the first, it would immediately after the first, it would interact with the ejected materialinteract with the ejected material