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X-ray emission by the rear side of laser-irradiated gold targets

Published online by Cambridge University Press:  09 March 2009

D. Babonneau
Affiliation:
Commissariat à l'Energie Atomique, Centre d'Etudes de Limeil-Valenton, 94195 Villeneuve Saint-Georges Cedex, France
J. L. Bocher
Affiliation:
Commissariat à l'Energie Atomique, Centre d'Etudes de Limeil-Valenton, 94195 Villeneuve Saint-Georges Cedex, France
C. Bayer
Affiliation:
Commissariat à l'Energie Atomique, Centre d'Etudes de Limeil-Valenton, 94195 Villeneuve Saint-Georges Cedex, France
A. Decoster
Affiliation:
Commissariat à l'Energie Atomique, Centre d'Etudes de Limeil-Valenton, 94195 Villeneuve Saint-Georges Cedex, France
D. Juraszek
Affiliation:
Commissariat à l'Energie Atomique, Centre d'Etudes de Limeil-Valenton, 94195 Villeneuve Saint-Georges Cedex, France
J. P. Perrine
Affiliation:
Commissariat à l'Energie Atomique, Centre d'Etudes de Limeil-Valenton, 94195 Villeneuve Saint-Georges Cedex, France
G. Thiell
Affiliation:
Commissariat à l'Energie Atomique, Centre d'Etudes de Limeil-Valenton, 94195 Villeneuve Saint-Georges Cedex, France

Abstract

We present results of X-ray emission by the rear side of gold thin targets irradiated by the Phebus laser at λ = 0.35 μm, τ = 0.7 and 1.3 ns, and EL = 1.5 kJ. A streak camera coupled with a transmission grating gave the time-resolved X-ray emission of the rear side. Also, a streak camera coupled with a slit allowed us to obtain information about the space and time evolution of the plasma. Some other diagnostics gave information about the energy balance and the X-ray conversion efficiency. The results are in good agreement with previous ones obtained with the Octal laser, particularly on optimum thicknesses for X-ray conversion efficiencies. Values of the thermal flux limiter are deduced. Simulations with FCI 1 code with multigroup radiative transfer and non-LTE ionization reproduce the experimental results only about some points. A number of reasons, such as 2-D effects and problems of opacity, are invoked.

Type
Research Article
Copyright
Copyright © Cambridge University Press 1991

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References

REFERENCES

Babonneau, D. et al. 1987 Bull. Am. Phys. Soc. 32, 1770.Google Scholar
Babonneau, D. et al. 1989 In Laser Interaction with Matter (World Scientific, Singapore), p. 281.Google Scholar
Busquet, M. 1982 Phys. Rev. A 25, 2302.CrossRefGoogle Scholar
Decoster, A. 1991 In preparation.Google Scholar
Duston, D. 1986 Can. J. Phys. 64, 998.CrossRefGoogle Scholar
Max, C. 1981 Physics of Laser Fusion, Vol. 1, Technical Report UCRL 53107, Lawrence Livermore National Laboratory.Google Scholar