2014
DOI: 10.1364/josab.31.0000c8
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Pulsed laser modification of transparent dielectrics: what can be foreseen and predicted by numerical simulations?

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Cited by 42 publications
(40 citation statements)
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“…where E is the electric field, H is the magnetic field, J D is current derived from the Drude model for the dispersive media, J Kerr is Kerr polarization current, and J pi is the multiphoton ionization term by using the finite-difference time-domain (FDTD) method for nonlinear and disperse media [34,35,[48][49][50][51]. At the edges of the grid, absorbing boundary conditions related to convolutional perfect matched layers (CPML) are set to avoid nonphysical reflections [65].…”
Section: Numerical Modelmentioning
confidence: 99%
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“…where E is the electric field, H is the magnetic field, J D is current derived from the Drude model for the dispersive media, J Kerr is Kerr polarization current, and J pi is the multiphoton ionization term by using the finite-difference time-domain (FDTD) method for nonlinear and disperse media [34,35,[48][49][50][51]. At the edges of the grid, absorbing boundary conditions related to convolutional perfect matched layers (CPML) are set to avoid nonphysical reflections [65].…”
Section: Numerical Modelmentioning
confidence: 99%
“…The electromagnetic field in these regions is modeled by resolving the same system of Eqs. (1)- (5) with a narrower electron band gap E g = 5.2 eV [49,71,79,88]. As long as the size of the inhomogeneity is considerably smaller than the irradiation wavelength, the initial plasma generation follows the Rayleigh scattering distribution [62].…”
Section: Numerical Modelmentioning
confidence: 99%
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