Hauptseite > Publikationsdatenbank > Spatial characteristics of K alpha X-ray emission from relativistic femtosecond laser plasmas > print

001     31495
005     20230217124338.0
024 7 _ |2 DOI
|a 10.1103/PhysRevE.68.056408
024 7 _ |2 WOS
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024 7 _ |2 Handle
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041 _ _ |a eng
082 _ _ |a 530
084 _ _ |2 WoS
|a Physics, Fluids & Plasmas
084 _ _ |2 WoS
|a Physics, Mathematical
100 1 _ |a Reich, Ch.
|b 0
|0 P:(DE-HGF)0
245 _ _ |a Spatial characteristics of K alpha X-ray emission from relativistic femtosecond laser plasmas
260 _ _ |a College Park, Md.
|b APS
|c 2003
264 _ 1 |3 online
|2 Crossref
|b American Physical Society (APS)
|c 2003-11-21
264 _ 1 |3 print
|2 Crossref
|b American Physical Society (APS)
|c 2003-11-01
300 _ _ |a 056408
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440 _ 0 |a Physical Review E
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520 _ _ |a The spatial structure of the Kalpha emission from Ti targets irradiated with a high intensity femtosecond laser has been studied using a two-dimensional monochromatic imaging technique. For laser intensities I<5x10(17) W/cm(2), the observed spatial structure of the Kalpha emission can be explained by the scattering of the hot electrons inside the solid with the help of a hybrid particle-in-cell/Monte Carlo model. By contrast, at the maximum laser intensity I=7x10(18) W/cm(2) the half-width of the Kalpha emission was 70 mum compared to a laser-focus half-width of 3 mum. Moreover, the main Kalpha peak was surrounded by a halo of weak Kalpha emission with a diameter of 400 mum and the Kalpha intensity at the source center did not increase with increasing laser intensity. These three features point to the existence of strong self-induced fields, which redirect the hot electrons over the target surface.
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700 1 _ |a Uschmann, I.
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700 1 _ |a Ewald, F.
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700 1 _ |a Düsterer, S.
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700 1 _ |a Lübcke, A.
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700 1 _ |a Schwoerer, H.
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700 1 _ |a Sauerbrey, R.
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700 1 _ |a Förster, E.
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700 1 _ |a Gibbon, P.
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773 1 8 |a 10.1103/physreve.68.056408
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