Enhancement of laser-driven electron acceleration in an ion channel
Abstract
A laser beam with duration longer than the period of plasma oscillations propagating through an underdense plasma produces a steady-state positively charged channel in the electron density. We consider a test electron in the two-dimensional plane channel under the combined action of the laser field and the transverse static electric field of the channel. At ultrarelativistic laser wave amplitude (a≫1), the electron is pushed primarily forward. As the electron gradually dephases from the wave, the field it samples and its relativistic γ-factor strongly oscillate. The natural frequency of electron oscillations across the channel (betatron frequency) depends on γ, which couples the betatron oscillations to the longitudinal motion induced by the wave. We show that the modulation of the natural frequency makes the oscillations unstable. The resulting amplification of the oscillations across the channel reduces the axial dephasing between the electron and the wave, leading to a considerable electron energy enhancement well above the ponderomotive energy. We find that there is a well-pronounced laser amplitude threshold a{sub *}, above which the enhancement takes place, that scales as a{sub *}∝1/√(n{sub 0}), where n{sub 0} is the ion density. The presented mechanism of energy enhancement is robust with respect to a longitudinal variationmore »
- Authors:
-
- Institute for Fusion Studies, The University of Texas, Austin, Texas 78712 (United States)
- Sandia National Laboratories, Albuquerque, New Mexico 87185 (United States)
- Publication Date:
- OSTI Identifier:
- 22251958
- Resource Type:
- Journal Article
- Journal Name:
- Physics of Plasmas
- Additional Journal Information:
- Journal Volume: 21; Journal Issue: 3; Other Information: (c) 2014 AIP Publishing LLC; Country of input: International Atomic Energy Agency (IAEA); Journal ID: ISSN 1070-664X
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 70 PLASMA PHYSICS AND FUSION TECHNOLOGY; BETATRON OSCILLATIONS; BETATRONS; ELECTRIC FIELDS; ELECTRON DENSITY; ELECTRONS; LASER RADIATION; LASERS; PLASMA WAVES; PONDEROMOTIVE FORCE; RELATIVISTIC RANGE; STEADY-STATE CONDITIONS
Citation Formats
Arefiev, Alexey V., Khudik, Vladimir N., and Schollmeier, Marius. Enhancement of laser-driven electron acceleration in an ion channel. United States: N. p., 2014.
Web. doi:10.1063/1.4867491.
Arefiev, Alexey V., Khudik, Vladimir N., & Schollmeier, Marius. Enhancement of laser-driven electron acceleration in an ion channel. United States. https://doi.org/10.1063/1.4867491
Arefiev, Alexey V., Khudik, Vladimir N., and Schollmeier, Marius. 2014.
"Enhancement of laser-driven electron acceleration in an ion channel". United States. https://doi.org/10.1063/1.4867491.
@article{osti_22251958,
title = {Enhancement of laser-driven electron acceleration in an ion channel},
author = {Arefiev, Alexey V. and Khudik, Vladimir N. and Schollmeier, Marius},
abstractNote = {A laser beam with duration longer than the period of plasma oscillations propagating through an underdense plasma produces a steady-state positively charged channel in the electron density. We consider a test electron in the two-dimensional plane channel under the combined action of the laser field and the transverse static electric field of the channel. At ultrarelativistic laser wave amplitude (a≫1), the electron is pushed primarily forward. As the electron gradually dephases from the wave, the field it samples and its relativistic γ-factor strongly oscillate. The natural frequency of electron oscillations across the channel (betatron frequency) depends on γ, which couples the betatron oscillations to the longitudinal motion induced by the wave. We show that the modulation of the natural frequency makes the oscillations unstable. The resulting amplification of the oscillations across the channel reduces the axial dephasing between the electron and the wave, leading to a considerable electron energy enhancement well above the ponderomotive energy. We find that there is a well-pronounced laser amplitude threshold a{sub *}, above which the enhancement takes place, that scales as a{sub *}∝1/√(n{sub 0}), where n{sub 0} is the ion density. The presented mechanism of energy enhancement is robust with respect to a longitudinal variation of the density, because it relies on a threshold phenomenon rather than on a narrow linear resonance.},
doi = {10.1063/1.4867491},
url = {https://www.osti.gov/biblio/22251958},
journal = {Physics of Plasmas},
issn = {1070-664X},
number = 3,
volume = 21,
place = {United States},
year = {Sat Mar 15 00:00:00 EDT 2014},
month = {Sat Mar 15 00:00:00 EDT 2014}
}