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  1. info.fusion.ciemat.es

    Pulse propagation in non-linear media is an important topic in many areas of science, plasma physics and non-linear optics being obvious examples. Such pulse propagation is subject to scaling laws that go beyond the non-linear extension of the linear dispersion of the carrier wave. These laws govern the relationships between pulse amplitude ...
  2. ui.adsabs.harvard.edu

    Pulse propagation in non-linear media is an important topic plasma physics and non-linear optics. Such pulse propagation is subject to scaling laws that go beyond the non-linear extension of the linear dispersion of the carrier wave. These laws govern the relationships (''ideal lines'') between pulse amplitude, spatial width, temporal duration and propagation speed, and the evolution of all ...
    Author:Raoul M. G. M. Trines, Schmitz H, Jorge Vieira, Luís Miguel Oliveira e Silva, Ricardo Fonseca, Richa...Published:2018
  3. academia.edu

    media R. Trines1, H. Schmitz1, E.P. Alves2, F. Fiúza2, J. Vieira3, L.O. Silva3, R. Bingham1,4 1 Central Laser Facility, STFC Rutherford Appleton Laboratory, Didcot, OX11 0QX, United Kingdom 2 SLAC National Accelerator Laboratory, Menlo Park, CA ... Universal scaling laws for pulse propagation in plasma and non-linear media. Universal scaling ...
  4. the pulse during propagation due to self-phase modulation, see Fig. 3.2 (a), we find, that the pulse redistributes its energy, such that the low frequency contributions are in the front of the pulse and the high frequencies in the back of the pulse, similar to the case of positive dispersion.
  5. meetings.aps.org

    Pulse propagation in non-linear media is an important topic plasma physics and non-linear optics. Such pulse propagation is subject to scaling laws that go beyond the non-linear extension of the linear dispersion of the carrier wave. These laws govern the relationships ("ideal lines") between pulse amplitude, spatial width, temporal duration ...
  6. 5.1 General Treatment of Linear Waves in Anisotropic Medium Start with general approach to waves in a linear Medium: Maxwell: 1 ∂E ∂B ∧B = µ oj + ; (5.1) c2 ∂t ∧E = − ∂t we keep all the medium's response explicit in j. Plasma is (infinite and) uniform so we Fourier analyze in space and time.
  7. labsites.rochester.edu

    the pulse, which is proportional to the scaling factor s. For n2 > 0, temporal stretching occurs in the front part of the pulse, leading to a corresponding decrease in s,as depicted by the solid line in Fig. 1(b), which is the famil-iar frequency red-shift. In contrast, temporal compres-sion occurs in the back portion of the pulse, resulting
  8. lations of pulse propagation in a commonly-used nonlin-ear material, β-barium borate (BBO). We find general dimensionless scaling laws quite similar to the ones from the NLSE, except that one must express them through Neff. The simulations span a very wide input-pulse pa-rameter space and the scaling laws therefore provide an important tool ...
  9. link.springer.com

    6.1 Pulse Propagation in Nonlinear Semiconductor Media 97 Fig. 6.1. Pulse propagation in the linear gain regime: snapshots of the intensity (left) and carrier density (right) in the active area of a broad-area laser amplifier 4ps(a, d), 8 ps (b, e) and 12 ps (c, f) after optical injection of a light pulse with

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