Bremsstrahlung and K alpha fluorescence measurements for inferring conversion efficiencies into fast ignition relevant hot electrons
The Bremsstrahlung and K-shell emission from 1×1×1 mm[superscript 3] planar targets irradiated by a short-pulse 3×10[superscript 18]–8×10[superscript 19] W/cm[superscript 2] laser were measured. The Bremsstrahlung was measured using a filter stack spectrometer with spectral discrimination up to 50...
| Main Authors: | , , , , , , , , , , , , , , , , , , |
|---|---|
| מחברים אחרים: | |
| פורמט: | Article |
| שפה: | en_US |
| יצא לאור: |
American Institute of Physics
2010
|
| גישה מקוונת: | http://hdl.handle.net/1721.1/52297 https://orcid.org/0000-0002-9518-4097 |
| סיכום: | The Bremsstrahlung and K-shell emission from 1×1×1 mm[superscript 3] planar targets irradiated by a short-pulse 3×10[superscript 18]–8×10[superscript 19] W/cm[superscript 2] laser were measured. The Bremsstrahlung was measured using a filter stack spectrometer with spectral discrimination up to 500 keV. K-shell emission was measured using a single photon counting charge coupled device. From Monte Carlo modeling of the target emission, conversion efficiencies into 1–3 MeV electrons of 3%–12%, representing 20%–40% total conversion efficiencies, were inferred for intensities up to 8×10[superscript 19] W/cm[superscript 2]. Comparisons to scaling laws using synthetic energy spectra generated from the intensity distribution of the focal spot imply slope temperatures less than the ponderomotive potential of the laser. Resistive transport effects may result in potentials of a few hundred kV in the first few tens of microns in the target. This would lead to higher total conversion efficiencies than inferred from Monte Carlo modeling but lower conversion efficiencies into 1–3 MeV electrons. |
|---|