Abstract
This thesis is dedicated to the generation and amplification of intense, ultrashort light pulses. For a thorough understanding of the physical effects encountered when working with such pulses, the following chapter provides a mathematical description of the propagation and interaction of light.
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Notes
- 1.
More precisely: there is only a small change of \(\varvec{\tilde{U}}\) within a distance of one wavelength \(\lambda = 2\pi /k\).
- 2.
The mathematical requirement is that the difference between phase velocity \(v_\mathrm {p}=\frac{\omega }{k}\) and group velocity \(v_\mathrm {g}=\frac{\partial \omega }{\partial k}\) is small compared to the latter.
- 3.
Not to be confused with the dispersion coefficient for the group delay \(D_1\) = GD\((\omega _0)\) which is the temporal delay of the carrier frequency \(\omega _0\) and hence a single value.
- 4.
This substitution adds a factor of two due to the historical definition of \(d_\mathrm {eff}\) and another factor of two due to the permutation symmetry of \(\chi _{ijk}^{(2)}\). The relation between \(d_\mathrm {eff}\) and \(\chi _{ijk}^{(2)}\) will be further explained in Sect. 2.3.4.
- 5.
For orthorhombic crystals the principle axes correspond to the crystallographic axes. For non-orthogonal crystal structures such as hexagonal or triclinic crystals, however, principle and crystallographic axes do not coincide.
- 6.
For simplicity we consider in the following only linearly polarized beams.
- 7.
For a derivation of Eq. (2.84) see Sect. A.2.2 in the appendix.
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Kessel, A. (2018). Fundamentals. In: Generation and Parametric Amplification of Few‐Cycle Light Pulses at Relativistic Intensities. Springer Theses. Springer, Cham. https://doi.org/10.1007/978-3-319-92843-2_2
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