THEORY OF CIRCULAR FREE ELECTRON LASER WITH AN INTENSE RELATIVISTIC NONNEUTRAL ELECTRON RING

Yin Yuanzhao

Volume 14 Issue 4

Jul. 1992

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Yin Yuanzhao. THEORY OF CIRCULAR FREE ELECTRON LASER WITH AN INTENSE RELATIVISTIC NONNEUTRAL ELECTRON RING[J]. Journal of Electronics & Information Technology, 1992, 14(4): 385-389.

Citation:

Yin Yuanzhao. THEORY OF CIRCULAR FREE ELECTRON LASER WITH AN INTENSE RELATIVISTIC NONNEUTRAL ELECTRON RING[J]. Journal of Electronics & Information Technology, 1992, 14(4): 385-389.

Yin Yuanzhao. THEORY OF CIRCULAR FREE ELECTRON LASER WITH AN INTENSE RELATIVISTIC NONNEUTRAL ELECTRON RING[J]. Journal of Electronics & Information Technology, 1992, 14(4): 385-389.

Citation:

Yin Yuanzhao. THEORY OF CIRCULAR FREE ELECTRON LASER WITH AN INTENSE RELATIVISTIC NONNEUTRAL ELECTRON RING[J]. Journal of Electronics & Information Technology, 1992, 14(4): 385-389.

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THEORY OF CIRCULAR FREE ELECTRON LASER WITH AN INTENSE RELATIVISTIC NONNEUTRAL ELECTRON RING

Yin Yuanzhao

Received Date: 1991-04-04
Rev Recd Date: 1991-07-25
Publish Date: 1992-07-19

Abstract

Abstract

The working properties of a circular free electron laser with an intenserelarivistic nonneutral electron ring have been investigated with in the framework of the Vla-sov-Maxwell equations. The results show that the space charge of intense electron beam can enhance the radiation growth rate and frequency

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References(1)

References

Y.Z.Yin, G. Bekefi, Phys. Fluids, 28(1985)4, 1186-1192.[2]Y. Z.Yin et al., IEEE J. of QE, QE-23(1987)9, 1610-1616.[3]H. Saito, J.S. Wurtele, Phys. Fluids, 30(1987)7, 2209-2220.[4]H. Saito, Y.Z. Yin. Nucl. Instrum. Methods Phys. Res. A272(1988)1/2, 319-322.[5]L. S. Schuetz et al., Phys. Fluids, 31(1988)6, 1720-1726.[6]W. Destler et al., Phys. Fluids, 28(1985)6, 1962-1967.[7]Chojnacki, W. W. Destler, IEEE J. of QE, QE-23(1987)9, 1605-1726.

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