2010
DOI: 10.1007/s11182-010-9430-1
|View full text |Cite
|
Sign up to set email alerts
|

Spectrum reconstruction of a nanosecond electron beam from the data on its extinction in thin foils

Abstract: A possibility of reconstructing the electron beam spectrum from the dependence of beam extinction on foil thickness is demonstrated. The electron energy distributions are calculated using Tikhonov's regularization of the Fredholm integral equation with the least number of a priori assumptions on the beam spectrum shape. The spectra experimentally obtained in a vacuum diode loaded by nanosecond voltage pulses are reconstructed and analyzed.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...

Citation Types

0
1
0

Year Published

2012
2012
2022
2022

Publication Types

Select...
3
1

Relationship

0
4

Authors

Journals

citations
Cited by 4 publications
(1 citation statement)
references
References 3 publications
(7 reference statements)
0
1
0
Order By: Relevance
“…[1][2][3][4][5][6] Foil spectroscopy methods employing either photomultiplier tubes (PMT) or Faraday cups were used to study the dependence of parameters of the x-ray generation accompanying the discharge on pressure and voltage values 4,7 and RAE energy. 8,9 Two possible origins of RAE were proposed: field or explosive emission, from the cathode 2,3 or from the boundary of the propagating streamer. In the latter case, the streamer boundary serves as a source of RAE either continuously during streamer's propagation toward the anode 10 or only when the streamer approaches the vicinity of the anode, where the electric field becomes sufficient for RAE generation.…”
mentioning
confidence: 99%
“…[1][2][3][4][5][6] Foil spectroscopy methods employing either photomultiplier tubes (PMT) or Faraday cups were used to study the dependence of parameters of the x-ray generation accompanying the discharge on pressure and voltage values 4,7 and RAE energy. 8,9 Two possible origins of RAE were proposed: field or explosive emission, from the cathode 2,3 or from the boundary of the propagating streamer. In the latter case, the streamer boundary serves as a source of RAE either continuously during streamer's propagation toward the anode 10 or only when the streamer approaches the vicinity of the anode, where the electric field becomes sufficient for RAE generation.…”
mentioning
confidence: 99%