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Notes
- 1.
The time dependent modulation is usually achieved with an acousto-optic or electro-optic modulator. If the modulation is synchronized with the resonator round trips, ultra-short pulses can be generated: a pulse with the “correct” timing can pass the modulator at times where the losses are at a minimum and the wings of the pulse are attenuated, which leads to (slight) pulse shortening in each round trip [7]. The pulse duration is typically in the picosecond range.
- 2.
The light transmissivity through a fast saturable absorber is an increasing function of the instantaneous input intensity. In this way the saturable absorber destabilizes the laser operation into configurations where most of the power is concentrated in short pulses.
- 3.
In a finite system this picture is only precise when the spectral correlation length is shorter than the finite bandwidth, so that the number of modes involved in the laser dynamic is large enough.
- 4.
- 5.
We refer, in particular, to the so-called Frequency Matching Condition, mentioned in Eq. (1.1).
- 6.
The quality factor (or Q factor) of a resonator is the ratio between the resonance frequency and the full width at half-maximum bandwidth of the resonance.
- 7.
The Ioffe-Regel criterion [36] for light localization states that, if the ratio of photon wave-vector k to mean free-path length l (of a photon not colliding with anything) is such that \(kl < 1\), then there is a finite probability that photons will become trapped, similarly to electrons under Anderson localization.
- 8.
Levy distributions are characterized by a slowly decaying (power-law) tail, so they have infinite variance and describe the occurrence of rare but very large values.
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Antenucci, F. (2016). Introduction. In: Statistical Physics of Wave Interactions. Springer Theses. Springer, Cham. https://doi.org/10.1007/978-3-319-41225-2_1
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