Loading…

Electron density measurement via dual-angle Thomson scattering diagnosis

In this article, we present experiments measuring the electron density of a blown-off aluminum plasma created by a 2 ω (532 nm) laser using dual-angle Thomson scattering diagnosis. By fitting two ion-acoustic-wave feature spectra collected from two angles simultaneously, in a typical shot, the elect...

Full description

Saved in:
Bibliographic Details
Published in:Journal of applied physics 2021-01, Vol.129 (4)
Main Authors: Tan, Wei-qiang, Liu, Yao-yuan, Li, Xin-yan, Yuan, Peng, Zhao, Hang, Li, Zhi-chao, Zheng, Jian
Format: Article
Language:English
Subjects:
Citations: Items that this one cites
Items that cite this one
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
Description
Summary:In this article, we present experiments measuring the electron density of a blown-off aluminum plasma created by a 2 ω (532 nm) laser using dual-angle Thomson scattering diagnosis. By fitting two ion-acoustic-wave feature spectra collected from two angles simultaneously, in a typical shot, the electron density obtained 400  μm in front of the target as given by Thomson scattering diagnosis was ( 5.9 ± 0.6 ) × 10 18 cm − 3, which is 35% higher than the average result of ( 4.4 ± 0.7 ) × 10 18 cm − 3 as measured by digital holography diagnosis. The distribution of the electron density along the laser axis from 400  μm to 700  μm as given by dual-angle Thomson scattering was broadly consistent with that obtained from digital holography diagnosis. At a location of 250  μm in front of the target, a unique set of plasma parameters cannot be obtained by dual-angle Thomson scattering diagnosis. This may be a result of the steep density gradient visible in the hologram in this region. Dual-angle Thomson scattering diagnosis can provide a good estimation of the electron density in plasma parameter regimes similar to those in these experiments, in which the scattering parameter α < 2. This technique may be useful for small laser facilities that cannot afford a second probe laser with a different wavelength and for measuring electron density with 4 ω Thomson scattering on large laser facilities. This article presents several factors that need to be considered when employing this method.
ISSN:0021-8979
1089-7550
DOI:10.1063/5.0032388