“…The beam radius R(z), the maximum intensity (solid curve, left axis), the density of free electrons on-axis (dashed curve, right axis) and the fluence distribution are plotted as a function of the propagation distance. According to Couairon and Mysyrowicz (2006).…”
Section: Main Results Obtained By the Analytical Approaches (Beam-parmentioning
confidence: 98%
“…Moloney and Kolesik, 2007;Couairon and Mysyrowicz, 2006;Chin et al, 2005, for a review). The first numerical simulations in this field started with a minimal model in the form of a nonlinear Schrödinger equation describing the pulse propagation and catching the essential of the physics without developing heavy numerical tools.…”
Section: Model Equations Governing the Nonlinear Propagation Of Lasermentioning
confidence: 98%
“…The initial pulse (a) undergoes contraction in the transverse diffraction plane (b) plasma defocusing of its trailing part (c) which is subsequently refocused by the optical Kerr effect (apparent splitting beyond the nonlinear focus) (d,e,f) During the propagation in the form of a filament, successive focusing-defocusing cycles reinforce and accentuate the shortening and the stiffening of the pulse beyond the nonlinear focus. From Couairon and Mysyrowicz (2006). trail of the pulse and its subsequent refocusing by the optical Kerr effect.…”
Section: Numerical Simulations Of Filamentation In Airmentioning
confidence: 98%
“…22. From Couairon and Mysyrowicz (2006). (c) The power spectra of a filamented pulse at 1.1 Rayleigh lengths are compared in the absence (continuous curve) and in the presence (dashed curve) of self-steepening.…”
Section: Simulations Of Supercontinuum Generationmentioning
“…The beam radius R(z), the maximum intensity (solid curve, left axis), the density of free electrons on-axis (dashed curve, right axis) and the fluence distribution are plotted as a function of the propagation distance. According to Couairon and Mysyrowicz (2006).…”
Section: Main Results Obtained By the Analytical Approaches (Beam-parmentioning
confidence: 98%
“…Moloney and Kolesik, 2007;Couairon and Mysyrowicz, 2006;Chin et al, 2005, for a review). The first numerical simulations in this field started with a minimal model in the form of a nonlinear Schrödinger equation describing the pulse propagation and catching the essential of the physics without developing heavy numerical tools.…”
Section: Model Equations Governing the Nonlinear Propagation Of Lasermentioning
confidence: 98%
“…The initial pulse (a) undergoes contraction in the transverse diffraction plane (b) plasma defocusing of its trailing part (c) which is subsequently refocused by the optical Kerr effect (apparent splitting beyond the nonlinear focus) (d,e,f) During the propagation in the form of a filament, successive focusing-defocusing cycles reinforce and accentuate the shortening and the stiffening of the pulse beyond the nonlinear focus. From Couairon and Mysyrowicz (2006). trail of the pulse and its subsequent refocusing by the optical Kerr effect.…”
Section: Numerical Simulations Of Filamentation In Airmentioning
confidence: 98%
“…22. From Couairon and Mysyrowicz (2006). (c) The power spectra of a filamented pulse at 1.1 Rayleigh lengths are compared in the absence (continuous curve) and in the presence (dashed curve) of self-steepening.…”
Section: Simulations Of Supercontinuum Generationmentioning
“…Recently, as a way to improve the interaction time and reduce the repetition frequency, it has been suggested to use elongated and linear energy deposition [15]- [18]. This idea is guided by the recent progress of femtosecond lasers, which are known to create thin ionized channels [12] [13] [19]. These channels can be used to guide an electric discharge and there is currently an ongoing research effort to couple more energy to this ionized channel using various mechanisms (more powerful nanosecond lasers [21], pulsed discharges or microwave excitation [22]).…”
The goal of this study is to demonstrate experimentally the "Laser Spike" concept in a supersonic flow. The "Laser Spike" uses a thin filament of plasma created by a femtosecond laser. This plasma filament formed by the TeraWatt laser pulse acts as a linear energy deposition upstream of the shock wave created by a blunt body. It has been found that the laser energy deposition induces a significant transient reduction of the drag. This reduction has been quantified using a drag balance. These experiments have been simulated numerically by modeling the plasma filament as a source term in the energy equation. It is shown that the plasma filament created by the ultra-short laser pulse forms a low-density heated core that interacts with the detached bow shock. This interaction produces an inflating recirculating bubble and leads to a transient reduction of the drag. These findings demonstrate the interest of ultrashort laser for flow control. Drag reduction, flow control and trajectory control are among the possible applications of the "laser spike" concept. Sonic boom alleviation could also be improved with this device.
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