Abstract

The dispersion relation of the FEL Amplifiers is sensitive to the linear tapered strong axial magnetic fields, electron cyclotron frequency and plasma frequency of electrons. For the synchronism of the pumped frequency, it should be closed to electron cyclotron frequency which is resonantly enhanced the wiggler wave number that produces the amplifier radiation for higher frequency from sub millimeter wave to optical ranges. The guiding of radiation signal into the waveguide and charge neutralization phenomenon, the beam density should be greater than the background plasma density with tapered strong axial magnetic field. It is quite considerable that radiation signal slowed down at much higher background plasma density comparable to the density of beams and enhanced the instability growth rate also. In Raman Regime operation, the growth rate decreases as increases with operation frequency of the amplifier, however, the growth rate is larger in this regime. It is noted that as increases with background plasma density, the beat wave frequency of the Ponderomotive waves is increases thus the mechanism of background plasma density can serve for tenability of the higher frequencies. The tapering of the strong guided magnetic field is a crucial role for enhancing the efficiency of the net transfer energy as well as reduction of interaction region along the axis. It is observed that, an efficiency of the transfer energy enhanced by while the reduction along the interaction region of about with the variation of tapering in a strong axial guided magnetic fields.

Highlights

  • The free electron laser amplifier (FELA) is an attractive device to employment of an electrostatic and electromagnetic wiggler for the production of tunable and coherent high power radiated signal using with mildly relativistic electron beams (REBs) to the higher frequencies from sub millimetre wave to optical ranges

  • For the synchronism of the pumped frequency, it should be closed to electron cyclotron frequency which is resonantly enhanced the wiggler wave number that produces the amplifier radiation for higher frequency from sub millimeter wave to optical ranges

  • The dispersion relation of the FEL Amplifier is sensitive to the tapered strong axial magnetic fields, electron cyclotron frequency and plasma frequency of electrons, which plays an important role in this configuration

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Summary

Introduction

The free electron laser amplifier (FELA) is an attractive device to employment of an electrostatic and electromagnetic wiggler for the production of tunable and coherent high power radiated signal using with mildly relativistic electron beams (REBs) to the higher frequencies from sub millimetre wave to optical ranges. Gardelle et al [23] explored the effects of space charge and quality of electron beams to improve the efficiency of FEL Amplifiers They have examined the collective effect on super radiant free electron laser amplifiers for a given interaction region and 2.5% efficiency is estimated to 35MW at 4mm lengths [24] [25]. A relativistic beam density of electron no and beam velocity v o zob ob that propagates through back ground plasma with interaction region It acquires an oscillatory velocity in transverse mode due to the whistler pumped with frequency o k v o and the axial magnetic ob o ob field gives to the cyclotron motion of electrons at a frequency . If radiated electrons move with a whistler wave, the phase matching condition to be satisfied

Raman regime operation
FEL amplifier gain
Results and discussion
Conclusion
Full Text
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