2018
DOI: 10.1007/978-3-319-96845-2_5
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Insights into Laser-Materials Interaction Through Modeling on Atomic and Macroscopic Scales

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Cited by 15 publications
(9 citation statements)
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“…Excited electronic ensemble equilibrates at an electronic temperature high above the atomic one. It induces a variety of effects, including electronic energy exchange with atoms/ions, modification of the interatomic potential, possible charge nonequilbirium and Coulombic response of the ions, evolution of the material properties and phase transitions [9][10][11]. Within this work, we will only focus on the first one, the electron-ion coupling.…”
Section: Introductionmentioning
confidence: 99%
“…Excited electronic ensemble equilibrates at an electronic temperature high above the atomic one. It induces a variety of effects, including electronic energy exchange with atoms/ions, modification of the interatomic potential, possible charge nonequilbirium and Coulombic response of the ions, evolution of the material properties and phase transitions [9][10][11]. Within this work, we will only focus on the first one, the electron-ion coupling.…”
Section: Introductionmentioning
confidence: 99%
“…For ultrashort pulses, the dynamic reflectivity depends on the electron temperature. The dynamic reflectivity of Zn was measured for 150 fs, 800 nm laser pulse at different fluence values by Shugaev et al [40]. They demonstrated that the dynamic and static reflectivity of Zn stays the same up to 1 J∕cm 2 .…”
Section: Discussionmentioning
confidence: 99%
“…To account for the changing dielectric permittivity with increasing electron temperature, Kirkwood et al divided the dielectric function into three domains based on the Fermi temperature ( T F ), namely metallic (Drude-Lorentz) dielectric function m for T e ≤ (1∕3) * T F , plasma dielectric function plasma for T e > 3 * T F and a combination of m and plasma for (1∕3) * T F < T e ≥ 3 * T F [41]. For femtosecond pulses, the plasma contribution is small on the dynamic reflectivity for Au and Zn, and primarily contributes to the leveling-off of reflectance value [40]. For picosecond laser pulses, the pulse duration is long enough to increase electron temperature above the Fermi temperature, to affect the electron-phonon coupling and subsequent early plasma formation during the pulse.…”
Section: Discussionmentioning
confidence: 99%
“…The interaction of ultrashort laser pulses with metals is typically described by the twotemperature model (TTM) [4,[7][8][9]. This consists of two heat flow equations; one for the conduction electrons, that absorb the laser radiation, and one for the lattice.…”
Section: Introductionmentioning
confidence: 99%
“…A deep insight into fundamental aspects of the electron gas behavior under non-equilibrium laser heating conditions can be obtained based on the Boltzmann equation [11,12], which however is difficult to use for practical application in view of the large computer resources required. There are many attempts to improve the TTM description using more sophisticated dependences of the free electron gas properties [8,9,[13][14][15][16], in particular, utilizing parameters calculated based on the density of states theory developed in [17] under the assumption of equilibrium conditions. However, the actual parameters of the free electron gas in metals are expected to lie in between the two extremes, resulting in a more complicated behavior under the highly non-equilibrium conditions obtained under ultrafast laser action [18].…”
Section: Introductionmentioning
confidence: 99%