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Abstract

In the last decades, the subject of laser-induced damage (LID) moved from a topic of scientific interest toward laser material processing for technical applications. When using pulsed lasers, the cumulative effect known as incubation is one of the most fundamental features of the processing event. Incubation manifests by the fact that the critical fluence for LID (known as laser-induced damage threshold, LIDT) depends on the number of pulses N exciting one spot on the sample. In most cases, the threshold fluence decreases with N starting from the single-shot ablation threshold and remains constant for large N. No ablation or damage occurs for any N, if the fluence is kept below the multiple-pulse threshold. In contrast, examples where the LIDT increases with N have been reported. The latter effect is known as laser conditioning and is advantageously used when ramping up the power of high-power laser systems. Incubation has been described for many types of solids; the motivation for these comprehensive efforts is twofold. Firstly, one tries to prevent the damage of optical materials in the beam path of high-energy or high-peak-power lasers. Secondly, one deliberately uses this damage for the sculpting of components. In this chapter, we introduce the reader to the mechanisms of incubation. We are going to look at the parameters controlling LID and highlight the peculiarity of the parameter "number of pulses". We will give an overview of the experimental work done in a variety of materials. There are several physical and chemical mechanisms proposed that govern incubation, and there are several mathematical models to describe the behavior of threshold fluence and ablation rate in dependence on the number of pulses. In a few cases, the two classes of mechanisms are even related to each other. Eventually, we will show the implications that incubation has on real-world laser machining.