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Chin. Phys. B, 2013, Vol. 22(2): 025203    DOI: 10.1088/1674-1056/22/2/025203
PHYSICS OF GASES, PLASMAS, AND ELECTRIC DISCHARGES Prev   Next  

Monoenergetic electron parameters in a spheroid bubble model

H. Sattariana, Sh. Rahmatallahpurb, T. Tohidic
a Maraghe Branch, Physics Department, Islamic Azad University, Maragheh, Iran;
b Bonab Branch, Physics Department, Islamic Azad University, Bonab, Iran;
c Department of Physics, Azarbaijan University of Tarbiat Moallem, Tabriz, Iran
Abstract  A reliable analytical expression for the potential of plasma waves with phase velocities near the speed of light is derived. The presented spheroid cavity model is more consistent than the previous spherical and ellipsoidal models and it explains the mono-energetic electron trajectory more accurately, especially at the relativistic region. The maximum energy of electrons is calculated and it is shown that the maximum energy of the spheroid model is less than that of the spherical model. The electron energy spectrum is also calculated and it is found that the energy distribution ratio of electrons ΔE/E for the spheroid model under the conditions reported here is half that of the spherical model and it is in good agreement with the experimental value in the same conditions. As a result, the quasi-mono-energetic electron output beam interacting with the laser plasma can be more appropriately described with this model.
Keywords:  quasi-mono-energetic electron bunches      intense laser      plasma accelerator      laser wake field      bubble regime  
Received:  11 May 2011      Revised:  15 August 2012      Accepted manuscript online: 
PACS:  52.38.-r (Laser-plasma interactions)  
  41.75.Jv (Laser-driven acceleration?)  
  42.62.-b (Laser applications)  
  41.75.Lx (Other advanced accelerator concepts)  
Corresponding Authors:  H. Sattarian     E-mail:  hsattarian@yahoo.com; rahmatsh@yahoo.com

Cite this article: 

H. Sattarian, Sh. Rahmatallahpur, T. Tohidi Monoenergetic electron parameters in a spheroid bubble model 2013 Chin. Phys. B 22 025203

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