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Lecture Notes in Physics

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8 H. Schwoerer<br />

Fig. 2.1. If the focal spot size of the sunlight lens is 0.1 mm 2 , the <strong>in</strong>tensity there<br />

would be 10 20 W/cm 2 . This value can be reached with state-of-the-art high-<strong>in</strong>tensity<br />

laser systems, admittedly, only for 10 −12 s<br />

In the laboratory however, they can be produced only <strong>in</strong> a controlled way <strong>in</strong><br />

high-<strong>in</strong>tensity laser plasmas.<br />

Before we describe the fundamental <strong>in</strong>teraction between such <strong>in</strong>tense light<br />

fields with matter, we quickly have to characterize the light fields themselves<br />

<strong>in</strong> the follow<strong>in</strong>g Sect. 2.2. In Sect. 2.3, we will <strong>in</strong>troduce the basic mechanisms<br />

of laser–matter <strong>in</strong>teraction at relativistic <strong>in</strong>tensities, start<strong>in</strong>g from the free<br />

electron <strong>in</strong> a strong electromagnetic wave all the way to the forced wakefield<br />

or bubble acceleration. Section 2.4 covers the generation of Bremsstrahlung<br />

<strong>in</strong> the multi-MeV range, and the f<strong>in</strong>al Sect. 2.5 describes the fundamentals of<br />

proton and ion acceleration with <strong>in</strong>tense laser pulses.<br />

2.2 The Most Intense Light Fields<br />

The <strong>in</strong>tensity of a laser pulse is given by the pulse energy E divided by the<br />

pulse duration τ and the size of the focal area A. In order to reach relativistic<br />

<strong>in</strong>tensities, E has to be large whereas τ and A must be as small as possible.<br />

For technical and f<strong>in</strong>ancial reasons basically two comb<strong>in</strong>ations of these parameters<br />

exist <strong>in</strong> real lasers: a high-energy version and an ultrashort version.<br />

The high-energy laser systems typically deliver pulse energies of hundreds to<br />

thousand Joules with<strong>in</strong> pretty short pulses below 1 ps. The ultrashort laser<br />

systems concentrate their pulse energy <strong>in</strong> the range of 1 J with<strong>in</strong> much less<br />

than 100 fs. Because of better focusability <strong>in</strong> the latter case, both types are<br />

able to generate the same maximum <strong>in</strong>tensity. Another difference between the<br />

two types of lasers is the rate of shots. Thermal effects with<strong>in</strong> the laser typically<br />

limit the high-energy systems to one shot with<strong>in</strong> half an hour whereas<br />

the ultrashort systems can operate around 10 Hz. Because of the high <strong>in</strong>vestments<br />

and operational costs of a high-energy laser system, these are run by<br />

national laboratories like the Rutherford Appleton Laboratory <strong>in</strong> the United

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