This book describes the ultra-short laser–matter interactions from the subtle atomic motion to the generation of extreme pressures inside the bulk of a transparent crystal. It is the successor to Femtosecond Laser–Matter Interactions: Theory, Experiment and Applications (2011). Explanation and experimental verification of the exceptional technique for the phase transformations under high pressure are in the core of the book. The novel phase formation occurs along the unique solid-plasmasolid transformation path: the memory of the initial state is lost after conversion to plasma. New phase forms from chaos during the cooling to the ambient. The pressure-affected material remains detained inside a pristine crystal at the laboratory tabletop. Unique super-dense aluminium and new phases of silicon were created by the confined micro-explosions. The text also describes the recent studies that used the quasi-non-diffracting Bessel beams. The applications comprise the new high-pressure material formation and micromachining. The book is an appealing source for readers interested in the cutting-edge research exploring extreme conditions and creating nanostructures at the laboratory tabletop.
Author(s): Eugene G. Gamaly
Edition: 2
Publisher: Jenny Stanford Publishing
Year: 2022
Language: English
Pages: 292
City: Singapore
Cover
Half Title
Title Page
Copyright Page
Dedication
Table of Contents
Preface
List of frequently used symbols
Chapter 1: Basics of Laser–Matter Interactions: Light and Matter
1.1: Laser Beam
1.1.1: Macroscopic Electrodynamics
1.1.2: Polarization States
1.1.3: Spectral Structure
1.1.4: Temporal/Spatial Shape of the Incident Laser Pulse Intensity
1.1.5: Focussing Positions of the Laser Beam on/in a Target
1.1.6: Focussing to Diffraction Limit with the High NA Lens
1.1.7: Diffraction-Free Beams
1.2: The Matter
1.2.1: Electrons’ Oscillations and Scattering in the High-Frequency Electromagnetic Field
1.2.2: The Drude Model for the Permittivity of Simple Plasma in the High-Frequency Electric Field
1.2.2.1: Electrons’ plasma frequency
1.2.2.2: Critical density of electrons
1.2.3: Absorbed Energy Density
1.2.4: Hierarchy of the Laser-Affected Material Transformations as a Function of Laser Intensity/Fluence
1.2.4.1: Melting
1.2.4.2: Ablation
1.2.4.3: Atomic field intensity
1.2.4.4: The relativistic intensity
1.3: Summary
Chapter 2: Interaction with Metals
2.1: Interaction of the Plane Wave with a Metal Layer
2.2: Electron and Lattice Temperature, Energy Balance, Two-Temperature Approximation
2.3: Temperature Dependence of the Electronic and Lattice Heat Capacity
2.4: Electrons Relaxation Processes in the Laser-Affected Metal
2.4.1: Electron–Electron Collisions
2.4.2: Electron–Phonon Momentum Transfer
2.4.3: Electron–Phonon Energy Transfer
2.4.4: Electron-to-Ion Momentum and Energy Transfer
2.4.5: Electron-to-Ion Energy Exchange Time
2.4.5.1: Non-ideality effects
2.4.5.1: Effects of the oscillations in high-frequency electromagnetic field on the electrons’ collision rate
2.5: Modification of the Electron Distribution Function: From the Fermi–Dirac to the Maxwell–Boltzmann
2.6: Electronic Heat Conduction
2.7: Summary
Chapter 3: Interaction with Dielectrics
3.1: Ionization in the Strong High-Frequency Electric Field: Electrons Transfer from the Valence to Conduction Band and to Continuum
3.1.1: Tunnelling Ionization Rate in the Limit y << 1
3.1.1.1: Linear polarization
3.1.1.2: Tunnel ionization in the elliptically polarized electric field
3.1.2: Multi-Photon Ionization Rate
3.1.2.1: Linear polarization
3.1.2.2: Time dependence of the ionization degree produced by the Gaussian laser pulse with the MPI domination
3.1.2.3: Circular polarization
3.1.3: Ionization by the Electron Impact
3.1.3.1: Transition to the avalanche regime
3.1.4: Distribution Function of Electrons Transferred to the Conduction Band in Dielectrics
3.2: Electrons’ Collision Rates: Momentum and Energy Transfer
3.2.1: Electron–Phonon Collisions
3.2.2: Momentum and Energy Transfer Collisions in a Dielectric Converted to Plasma
3.2.3: Effects of the Electrons’ Oscillations in the HF Field on the Collision Rates
3.3: Transient Permittivity in the Laser-Affected Dielectric
3.3.1: Non-Linear Contributions to the Permittivity at the Low Intensity (I << Iat)
3.3.2: Kerr-Nonlinearity in Silica: Temperature Dependence
3.3.3: Permittivity in the Intense-Laser-Excited Dielectric
3.3.3.1: Reaching the state Ɛre = 0
3.4: Laser Interaction with the Electrically Inhomogeneous Dielectric
3.4.1: Normal Incidence
3.4.2: Oblique Incidence
3.4.2.1: s-Polarization
3.4.2.2: p-Polarization
3.4.2.3: Band gap modification and collapse
3.5: Energy Density Thresholds for Achieving the Major Steps in Dielectric-Plasma Transformation
3.5.1: Threshold to Achieve the State Where Ɛre = 0
3.5.2: Threshold Fluence for Transferring All Valence Electrons to the Conduction Band
3.5.3: Ionization Threshold: Transfer Electrons to the Solid Plasma State
3.6: Energy Equations: Two-Temperature Approximation
3.7: Linear and Non-Linear Heat Conduction: Transition from Heat Transfer in Solid to That in Plasma
3.7.1: Heat Diffusion in the Isotropic Medium
3.7.2: Thermal Conduction in Dielectrics: Energy Carriers are Phonons
3.7.3: Electronic Heat Conduction in Plasma
3.7.4: Applicability of Diffusion Approximation for Description the Heat Conduction in the Laser-Created Plasma
3.7.5: Linear and Non-Linear Heat Propagation from the Focal Region
3.7.5.1: Linear heat conduction
3.7.5.2: Non-linear heat propagation
3.8: Summary
Chapter 4: Non-Destructive Transformations: Formation, Lifetime and Decay of Unconventional States of Matter
4.1: Generation and Decay of the Coherent Phonons
4.1.1: Melting in Equilibrium: Atomic Vibrations Become Anharmonic
4.1.2: Swift Deposition of the Energy Density Comparable to the Enthalpy of Fusion by the Ultra-Short Laser Pulse
4.1.2.1: Processes during the pulse: building the electronic pressure force
4.1.2.2: After the end of the pulse: electronic heat transfer, electron–lattice temperature equilibration, and phonon’s decay rate
4.1.2.3: Phonon’s excitation imprinted into the transient optical properties
4.1.2.4: Experiments
4.2: Fast Transformations in Non-Equilibrium: Transient Phase States—Neither Solid Nor Melt
4.2.1: Road to Melting in Equilibrium: Sequence of the Catastrophes
4.2.1.1: Main features of the melting in equilibrium
4.2.1.2: Critical entropy and critical temperature
4.2.2: Ultra-Fast Material Transformations
4.2.2.1: The legitimacy of the entropy concept for the description of rapidly excited metal
4.2.2.2: Entropy changes during the quick heating
4.2.3: Novel Transient Phase States—Neither Solids Nor Melts
4.2.3.1: Excitation of metals/semi-metals—Ga, Bi, Al
4.3: Mixed Dielectric/Metal Properties in Swiftly Excited Transparent Dielectric
4.4: Inverse Population in Laser-Excited Sapphire and Silica
4.5: Summary
Chapter 5: Ablation of Metals and Dielectrics
5.1: Evaporation in Equilibrium
5.2: Major Relaxation Processes under Swift Short Pulse Excitation
5.3: Short Pulse Ablation Thresholds
5.3.1: Ablation of Metals
5.3.1.1: Extremely short pulses of duration shorter tc,i
5.3.1.2: Comparison to the Coulomb explosions of clusters
5.3.1.3: Ultra-short pulses ω-1pi < tp < theat
5.3.1.4: Ablation threshold fluence for metals
5.3.2: Ablation of Dielectrics
5.4: Dependence of the Ablation Thresholds on the Laser Wavelength for Metals and Dielectrics
5.5: Long Pulse Ablation Thresholds
5.6: Ablation Thresholds in the Ambient Gas
5.7: Ablation Rate, Depth and Mass Per Single Pulse
5.8: Control over the Phase State of the Ablated Plume
5.8.1: Criterion for Complete Atomization of Ablated Plume
5.8.2: Experimental Verification of the Plume’s Atomization
5.9: Multiple Pulse Action: Accumulation Effects
5.9.1: Dwell Time: Control over the Number of Pulses Hitting the Spot
5.9.2: Multiple-Pulse Action on Dielectrics: Energy Accumulation
5.9.3: Achieving Thermal Ablation Threshold with the Low-Energy Multiple Pulses
5.9.4: Smoothing of the Intensity Distribution across the Focal Spot
5.9.5: Change of the Interaction Mode: Density Build-Up near the Target Surface
5.10: Summary
Chapter 6: Extreme Energy Density Confined inside a Transparent Crystal—Novel Path for New Materials Creation: Solid-Plasma-Solid Transformations
6.1: Introduction
6.2: Interaction of the Gauss Beam Tightly Focused inside a Transparent Crystal
6.2.1: Beam Propagation
6.2.2: Focusing of the Gauss Beam with the High-NA Optics
6.2.2.1: Conventional approach to the high-NA focusing
6.2.2.2: Experimental evidence: high-NA focus produces nano-sharp intensity distribution
6.2.3: Laser Modification of the Dielectric Permittivity: Conversion to Solid Density Plasma
6.2.3.1: Threshold for Conversion of Dielectric into Absorbing Medium (εre = 0)
6.2.3.2: Conversion a dielectric to the solid density plasma
6.2.3.3: Ionization after the end of the pulse
6.2.4: Relaxation Processes
6.2.4.1: Range for the maximum temperature/pressure value in the absorption volume
6.2.4.2: Ion’s acceleration by the gradient of the electronic pressure
6.2.4.3: Electrons-to-ions energy transfer by the Coulomb collisions: Spatial separation of the light and heavy ions
6.2.4.4: Diffusion of ions with the different masses: The experimental evidence of the spatial separation
6.2.5: Micro-Explosion in Sapphire Considered as a Strong Point-Like Explosion
6.2.5.1: Interpretation of the micro-explosion experiments using the strong point-like explosion solution
6.2.6: Summary of the Conditions after the Electron–Ion Energy Equilibration Shock Wave Generation, Propagation and Stopping
6.2.6.1: Analysis of the experimentally observed structure on the basis of the energy and mass conservation laws
6.2.6.2: Evolution of the conditions and the structure of the laser affectedzone during expansion
6.2.7: Modelling the Hydrodynamics of the Confined Explosion
6.2.8: Relaxation of the Laser-Affected Material to the Ambient Conditions
6.3: Interaction of the Gauss Beam Tightly Focused on the Surface of an Opaque Solid Buried under the Transparent Cover
6.3.1: Upper Limit for the Energy Density Directly Delivered to the Opaque Medium through the Transparent Layer
6.3.2: High-Energy-Density Interaction at the Silicon/Silica Interface
6.3.3: Shock Wave Generation in Silica Layer
6.4: Summary of the Gauss Beam–Generated Confined Micro-Explosions
6.5: Interaction of the Bessel Beam Focused inside a Bulk of the Transparent Crystal
6.5.1: Status of the BB–Transparent Crystal Interactions
6.5.2: Non-Diffractive Bessel Beam
6.5.3: Creation of the BB by the Circular Slit
6.5.4: Formation the BB by Transmitting the GB through the Axicon
6.5.5: BB Interaction with the Transparent Medium at Low Intensity
6.5.6: Intense BB Interaction: Conversion a Dielectric into Plasma Near the Axis
6.5.7: BB Interaction with Plasma
6.5.8: Energy Deposition in Plasma to the End of the Pulse
6.5.9: Strong Cylindrical Explosion
6.5.10: Experimental Evidence of the High Energy Density Achieved by the BB Induced Cylindrical Explosion
6.6: Solid-Plasma-Solid Transformation in Confined Micro-Explosion: New Path for High-Pressure Material Phase Formations
6.6.1: Discovery of Superdense bcc-Al in Sapphire Irradiated by the Tightly Focused Gauss Beam
6.6.2: Discovery of New Tetragonal Polymorphs of Silicon
6.7: Summary: Confined Micro-Explosion by the Gauss and Bessel Beams
Conclusions and Future Directions
Appendices
Bibliography
Index