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			<titleStmt><title level='a'>Atomistic Modeling of Ultrashort Pulse Laser-Induced Generation of Crystal Defects</title></titleStmt>
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				<publisher></publisher>
				<date>08/01/2022</date>
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				<bibl> 
					<idno type="par_id">10344075</idno>
					<idno type="doi">10.1017/S1431927622003816</idno>
					<title level='j'>Microscopy and Microanalysis</title>
<idno>1431-9276</idno>
<biblScope unit="volume">28</biblScope>
<biblScope unit="issue">S1</biblScope>					

					<author>Miao He</author><author>Eaman T. Karim</author><author>Maxim V. Shugaev</author><author>Cheng-Yu Shih</author><author>Leonid V. Zhigilei</author>
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<div xmlns="http://www.tei-c.org/ns/1.0"><p>Rapid advancements in the development of accessible sources of ultrashort (pico-and femtosecond) laser pulses open up new possibilities for surface modification with high accuracy and spatial resolution. The shallow depths of the laser energy deposition and steep temperature gradients, produced by the ultrashort pulse laser irradiation, can lead to the cooling rates of more than 10 12 K/s. Resolidification of a transiently melted surface region, occurring under conditions of rapid quenching and dynamic relaxation of laser-induced stresses, creates the conditions for generation of highly nonequilibrium densities and configurations of crystal defects, which can drastically alter the physical, chemical, and mechanical properties of surface layers processed by ultrashort laser pulses <ref type="bibr">[1,</ref><ref type="bibr">2]</ref>.</p><p>Detailed characterization of microstructural changes produced by ultrashort pulse laser irradiation has revealed the presence of high densities of dislocations <ref type="bibr">[3,</ref><ref type="bibr">4]</ref>, nanoscale twinned domains <ref type="bibr">[5,</ref><ref type="bibr">6]</ref>, and nanograins <ref type="bibr">[6]</ref> in the surface regions of the irradiated targets. The small size of the laser-modified zone, however, makes the characterization of laser-induced nanostructure challenging and, at the same time, increases the importance of understanding of the nucleation, mobility, interactions and stability of individual crystal defects. Large-scale atomistic modeling of laser-materials interactions <ref type="bibr">[2,</ref><ref type="bibr">5,</ref><ref type="bibr">[7]</ref><ref type="bibr">[8]</ref><ref type="bibr">[9]</ref><ref type="bibr">[10]</ref><ref type="bibr">[11]</ref> can help in the physical interpretation of experimental data and, eventually, in the development of new reliable methodology for experimental probing of laser-modified zone with nanometer structural and compositional resolutions. Several examples of the application of atomistic modeling to investigation of the generation of crystal defects in ultrashort pulse laser interactions are provided below.</p><p>The mechanisms of the generation of vacancies, dislocations, stacking faults, and twin boundaries in Nibased single-phase solid-solution alloys (Ni 50 Fe 50 , Ni 80 Fe 20 , and Ni 80 Cr 20 ) are investigated in the irradiation regime of melting and resolidification <ref type="bibr">[8]</ref>. The decrease in the thermal conductivity and strengthening of the electron-phonon coupling due to the intrinsic chemical disorder in the solid-solution alloys are found to have important implications on localization of the energy deposition and generation of thermoelastic stresses. The interaction of the laser-induced stress waves with the melting front is found to play a key role in roughening of the crystal-liquid interface and generation of dislocations upon the solidification, e.g., Figure <ref type="figure">1a</ref>. A common feature revealed in the structural analysis of all irradiated targets is the presence of high vacancy concentrations exceeding the equilibrium values at the melting temperature by about an order of magnitude, e.g., Figure <ref type="figure">1b</ref>. The analysis of the first atomic shell surrounding the vacancy sites in Ni-Fe alloys uncovers the preference for the vacancy sites to be surrounded by Fe atoms, Figure <ref type="figure">1c</ref>, and suggests that atomic-scale chemical heterogeneities may play an important role in defining the properties of the single-phase concentrated solid-solution alloys. The simulations of laser-material interactions are complemented by systematic analysis of the generation of crystal defects at a rapidly advancing solidification front in molecular dynamics simulations of solidification occurring at fixed levels of undercooling. The generation of defects is correlated with the velocity of the solidification front, and the processes responsible for creating the strong vacancy supersaturation <ref type="bibr">[11]</ref> and nanoscale twinned domains <ref type="bibr">[5]</ref> are revealed. At higher laser fluences, above the ablation threshold, the generation of crystal defects is intertwined with processes responsible for the material ejection (phase explosion, spallation), which affect the cooling rates and solidification kinetics. In particular, the generation of high densities of dislocations and vacancies in frozen surface features produced by spatially-modulated laser ablation of Cr targets is predicted in atomistic simulations illustrated by Figure 2 <ref type="bibr">[9,</ref><ref type="bibr">10]</ref>. The mechanical and chemical properties of the frozen protrusions generated by the ablation in vacuum (Figure <ref type="figure">2a</ref>) and in water environment (Figure <ref type="figure">2b</ref>) can be expected to be strongly affected by the very high vacancy concentrations exceeding 10 -3 and dislocation densities on the order of 10 15 m -2 . <ref type="bibr">[12]</ref> Figure <ref type="figure">2</ref>. Dislocations and vacancy clusters present in and below the frozen protrusions generated in simulations of spatially-modulated laser ablation of Cr targets in vacuum <ref type="bibr">[9]</ref> and in water environment <ref type="bibr">[10]</ref>. The defects are exposed by blanking the atoms with local bcc coordination.</p></div><note xmlns="http://www.tei-c.org/ns/1.0" place="foot" xml:id="foot_0"><p>Microsc. Microanal. 28 (Suppl 1), 2022</p></note>
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